比特派app官方下载网站安卓|interference
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Interference | Definition, Examples, & Facts | Britannica
Interference | Definition, Examples, & Facts | Britannica
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Last Updated:
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Table of Contents
interference
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Category:
Science & Tech
Key People:
Augustin-Jean Fresnel
Thomas Young
(Show more)
Related Topics:
beat
interference fringe
Young’s experiment
modulation of waves
wave train
(Show more)
See all related content →
Understanding wave interference through sound experimentsOverview of interference using the example of sound waves.(more)See all videos for this articleinterference, in physics, the net effect of the combination of two or more wave trains moving on intersecting or coincident paths. The effect is that of the addition of the amplitudes of the individual waves at each point affected by more than one wave.If two of the components are of the same frequency and phase (i.e., they vibrate at the same rate and are maximum at the same time), the wave amplitudes are reinforced, producing constructive interference. But if the two waves are out of phase by 1/2 period (i.e., one is minimum when the other is maximum), the result is destructive interference, producing complete annulment if they are of equal amplitude. The solid line in Figures A, B, and C represents the resultant of two waves (dotted lines) of slightly different amplitude but of the same wavelength. The two component waves are in phase in Figure A but out of phase by 1/4 period and 1/2 period in B and C.
Britannica Quiz
Physics and Natural Law
When two stones are dropped into a pool of water, waves spread out from each source, and interference occurs where they overlap. Constructive interference results where the crest of one coincides with the crest of the other. Two wave trains of light from a double slit produce interference, an effect that is visible on a screen as a pattern of alternating dark and light bands caused by intensification and extinction at points at which the waves are in phase and out of phase, respectively.Interference also occurs between two wave trains moving in the same direction but having different wavelengths or frequencies. The resultant effect is a complex wave. A pulsating frequency, called a beat, results when the wavelengths are slightly different. Figures D, E, and F show complex waves (solid lines) composed of two component interfering waves (dotted lines), the ratio of their wavelengths being 1:2 and of their amplitudes 1:3.
Interference between waves traveling in opposite directions produces standing waves. The Editors of Encyclopaedia BritannicaThis article was most recently revised and updated by Erik Gregersen.
Interference Definition & Meaning - Merriam-Webster
Interference Definition & Meaning - Merriam-Webster
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interference
noun
in·ter·fer·ence
ˌin-tər-ˈfir-ən(t)s
ˌin-tə-
Synonyms of interference
1
a
: the act or process of interfering
b
: something that interferes : obstruction
2
a
: the illegal hindering of an opponent in sports
b
: the legal blocking of an opponent in football to make way for the ballcarrier
3
a
: confusion of a received radio signal due to the presence of noise (such as atmospherics) or signals from two or more transmitters on a single frequency
b
: something that produces such confusion
4
: the mutual effect on meeting of two wave trains (as of light or sound) that constitutes alternating areas of increased and decreased amplitude (such as light and dark lines or louder and softer sound)
5
: partial or complete inhibition or sometimes facilitation of other genetic crossovers in the vicinity of a chromosomal locus where a preceding crossover has occurred
6
: the disturbing effect of new learning on the performance of previously learned behavior with which it is inconsistent
interferential
ˌin-tər-fə-ˈren(t)-shəl
ˌin-tə-
-ˌfir-ˈen(t)-
adjective
Synonyms
balk
bar
block
chain
clog
cramp
crimp
deterrent
drag
embarrassment
encumbrance
fetter
handicap
hindrance
holdback
hurdle
impediment
inhibition
let
manacle
obstacle
obstruction
shackles
stop
stumbling block
trammel
See all Synonyms & Antonyms in Thesaurus
Examples of interference in a Sentence
We had to put up with loud noise and constant interference from the neighbors.
interference in the affairs of another nation
trying to avoid governmental interference
It was hard to hear the radio program because of all the interference.
The TV picture had a lot of interference.
a hockey player receiving a penalty for interference
See More
Recent Examples on the Web
Noteworthy features include multi-link operation (MLO) for simultaneous connections, stream classification service (SCS) for latency-sensitive applications and spectrum efficiency and interference mitigation measures.
—Cristian Randieri, Forbes, 29 Feb. 2024
The case involved a custody dispute over frozen embryos and the court found that applying the law to the embryos would violate the sperm donor’s fundamental rights to privacy, freedom from government interference and right to not procreate.
—Jonathan Shorman, Kansas City Star, 28 Feb. 2024
In the Texas case, the company accused Media Matters of disparagement and interference with X’s contracts with advertisers.
—Joseph Menn, Washington Post, 28 Feb. 2024
Shell and other oil companies often blame third-party interference, namely militant attacks and vandalism by oil thieves, for spills.
—Taiwo Adebayo, Quartz, 28 Feb. 2024
Protect against interference or taking a risk that can affect your health or financial well-being.
—Eugenia Last, The Mercury News, 28 Feb. 2024
The under-prescription wasn't due to the interference of parents.
—Kamala Thiagarajan, NPR, 27 Feb. 2024
Fulton County District Attorney Fani Willis gestures while testifying as Fulton County Superior Judge Scott McAfee presides during a hearing on the Georgia election interference case, Thursday, Feb. 15, 2024, in Atlanta.
—Democrat-Gazette Staff From Wire Reports, arkansasonline.com, 16 Feb. 2024
However, the ability for consumers to choose which apps to install on their phone without interference is not the only feature that will improve the iPhone.
—Ewan Spence, Forbes, 16 Feb. 2024
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These examples are programmatically compiled from various online sources to illustrate current usage of the word 'interference.' Any opinions expressed in the examples do not represent those of Merriam-Webster or its editors. Send us feedback about these examples.
Word History
First Known Use
1783, in the meaning defined at sense 1a
Time Traveler
The first known use of interference was
in 1783
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Phrases Containing interference
RNA interference
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Merriam-Webster
“Interference.” Merriam-Webster.com Dictionary, Merriam-Webster, https://www.merriam-webster.com/dictionary/interference. Accessed 12 Mar. 2024.
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Kids Definition
interference
noun
in·ter·fer·ence
ˌint-ə(r)-ˈfir-ən(t)s
1
a
: the act or process of interfering
b
: something that interferes
2
: the shared effect on meeting of two waves (as of light or sound) whereby the waves cancel each other at some points and strengthen each other at other points
3
a
: the act of legally blocking an opponent in football
b
: the act of illegally getting in the way of an opponent in sports
4
a
: confusion of received radio signals due to undesired signals
b
: something that produces such confusion
Medical Definition
interference
noun
in·ter·fer·ence
-ˈfir-ən(t)s
1
: the act or process of interfering
2
: the mutual effect on meeting of two wave trains (as of light or sound) that constitutes alternating areas of increased and decreased amplitude (as light and dark lines or louder and softer sound)
3
: partial or complete inhibition or sometimes facilitation of other genetic crossovers in the vicinity of a chromosomal locus where a preceding crossover has occurred
4
: the disturbing effect of new learning on the performance of previously learned behavior with which it is inconsistent compare negative transfer
5
: prevention of typical growth and development of a virus in a suitable host by the presence of another virus in the same host individual see interference phenomenon
Legal Definition
interference
noun
in·ter·fer·ence
1
a
: the act or an instance of interfering
interference with contract
b
: something that interferes
2
: a hearing to determine the priority of invention at issue in a patent dispute
More from Merriam-Webster on interference
Nglish: Translation of interference for Spanish Speakers
Britannica English: Translation of interference for Arabic Speakers
Britannica.com: Encyclopedia article about interference
Last Updated:
4 Mar 2024
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Interference of Waves - Interference Definition, Derivation, Review Question, Video and FAQs
Interference of Waves - Interference Definition, Derivation, Review Question, Video and FAQs
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PhysicsWavesInterference Of Waves
Interference of Waves
Have you ever wondered what happens when two waves travelling in the same medium meet? Will the two waves bounce off each other, or do they pass through each other? Or, will the meeting of two waves affect the appearance of the medium? These questions about the meeting of waves pertain to the topic of wave interference. In this article, we will discuss wave interference definition and its types in detail.
Table of Contents:
What is Interference
Derivation
Check Your Understanding
Frequently Asked Questions – FAQs
What is Interference?
Interference is what happens when two or more waves meet each other. Depending on the overlapping waves’ alignment of peaks and troughs, they might add up, or they can partially or entirely cancel each other. As per the interference definition, it is defined as
, The phenomenon in which two or more waves superpose to form a resultant wave of greater, lower or the same amplitude.
The interference of waves results in the medium taking on a shape resulting from the net effect of the two individual waves. To better understand, let us consider the example of two pulses of the same amplitude travelling in different directions in the same medium. Let us consider each displaced upward by 1 unit at its crest and has the shape of a sine wave. As these sine pulses move towards each other, there will be a moment in time when they are completely overlapped. At this point, the shape of the medium would be an upward displaced sine wave with an amplitude of 2 units. After understanding the interference definition, let us learn the derivation of wave interference.
Derivation
The figure illustrates the before and during interference snapshots of the medium of two pulses. The individual sine pulses are drawn in pink and blue, and the resulting wave is green in colour.The principle of superposition of waves states that when two or more waves of the same type are incident on the same point, the resultant amplitude at that point is equal to the vector sum of the amplitudes of the individual waves. If the crest of a wave meets the crest of another wave of the same frequency at the same point, then the resultant amplitude is the sum of individual amplitudes – this is known as constructive interference. Similarly, suppose a wave’s crest meets another wave’s trough. In that case, the resultant amplitude is equal to the difference in the individual amplitudes – this is known as destructive interference. The formula for the sum of two waves can be derived as follows:
The amplitude of a sinusoidal wave travelling to the right along the x-axis is given by,
\(\begin{array}{l}W_1(x,t)=A\cos (kx-\omega t)\end{array} \)
Where A is the peak amplitude, k = 2π/λ is the wavenumber and ω = 2πf is the angular frequency of the wave.
Consider another wave of the same frequency and amplitude but with a different phase travelling to the right.
\(\begin{array}{l}W_2(x,t)=A\cos (kx-\omega t+\phi )\end{array} \)
where φ is the phase difference between the waves in radians
The two waves superimpose and add; the equation gives the resultant wave,
\(\begin{array}{l}W_1+W_2=A[\cos (kx-\omega t)+\cos (kx-\omega t+\phi)]\end{array} \) (1)
The equation gives the sum of two cosines,
\(\begin{array}{l}\cos a+\cos b=2\cos (\frac{a-b}{2})\cos (\frac{a+b}{2})\end{array} \)
Solving equation (1) using the formula, we get
\(\begin{array}{l}W_1+W_2=2A\cos \frac{\phi }{2}\cos (kx-\omega t+\frac{\phi }{2})\end{array} \)
Constructive Interference: When the phase difference is an even multiple of π (φ = ….., –4π, –2π, 0, 2π, 4π,……), then cos φ/2 =1, so the sum of the two waves is a wave with twice the amplitude.
\(\begin{array}{l}W_1+W_2=2A\cos (kx-\omega t)\end{array} \)
Destructive Interference: When the phase difference is an odd multiple of π (φ =….., –3π, –π, 0, π, 3π, 5π,……), then cos φ/2 = 0, so the sum of the two waves will be zero.
\(\begin{array}{l}W_1+W_2= 0\end{array} \)
Check Your Understanding
Two fishes create a series of circular waves by swimming in the water. The waves undergo interference and create the pattern as represented in the diagram. The thick lines represent crests, and the thin lines represent troughs. Several positions in the diagram are labelled with a letter. Categorize the labelled position as being either constructive or destructive interference.
Answer:
Constructive Interference: A and B
Destructive Interference: C
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Frequently Asked Questions-FAQsQ1 State the interference definition.
As per the interference definition, it is defined as the phenomenon in which two waves superpose to form the resultant wave of the lower, higher or same amplitude.
Q2 What are the types of light interference?
The following are the types of light interference:
Constructive interference
Destructive interference
Q3 State true or false: The interference of waves results in the medium taking shape resulting from the net effect of the two individual waves.
TRUE.
Q4 Do sound waves undergo interference?
Yes, sound waves can undergo interference.
Q5 State the principle of superposition of waves?
The principle of superposition of waves states that when two or more waves of the same type are incident on the same point, the resultant amplitude at that point is equal to the vector sum of the amplitudes of the individual waves.
Test your knowledge on Interference Of Waves
Q5
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INTERFERENCE | English meaning - Cambridge Dictionary
INTERFERENCE | English meaning - Cambridge Dictionary
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English (UK)
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English
Meaning of interference in English
interferencenoun [ U ] uk
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/ˌɪn.təˈfɪə.rəns/ us
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/ˌɪn.t̬ɚˈfɪr.əns/
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C1 an occasion when someone tries to interfere in a situation: She seems to regard any advice or help from me as interference. The government's interference in the strike has been widely criticized.
C2 noise or other electronic signals that stop you from getting good pictures or sound on a television or radio
More examplesFewer examplesThe political subtext of her novel is a criticism of government interference in individual lives.In the end he moved to another part of the country to escape his mother's continual interference in his private life.They dreamed of a new world order, composed of co-operating independent nation states, free from outside interference.Now can I please get on with the job, without any more interference from you?I'm sorry if he sees it as interference - we were only trying to be helpful.
SMART Vocabulary: related words and phrases
Getting involved for one's own benefit or against others' will
a piece/slice of the action idiom
act
action
bandwagon
be in bed with idiom
bed
get
get in on something
get/muscle in on the act idiom
have a finger in the pie idiom
horn
horn in
interfere
intrude
intrusion
jump/climb/get on the bandwagon idiom
non-interference
snoot
stick your snoot in/into (something) idiom
See more results »
You can also find related words, phrases, and synonyms in the topics:
Communications - general words
Idiom
run interference
(Definition of interference from the Cambridge Advanced Learner's Dictionary & Thesaurus © Cambridge University Press)
interference | American Dictionary
interferencenoun [ U ] us
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/ˌɪn·tərˈfɪər·əns/
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On the radio, television, or telephone, interference is noise, lines, etc., that prevent a clear sound or picture from being received.
physics Interference between two waves happens when they have the same frequency and produce a force that is either stronger or weaker than one wave alone.
In sports, interference is an action that is against the rules which prevents an opposing player from completing a play.
(Definition of interference from the Cambridge Academic Content Dictionary © Cambridge University Press)
Examples of interference
interference
Instead, paternalism views the interferences as justified in themselves, not merely as permissible, all things considered.
From the Cambridge English Corpus
Finally, quantum computing uses interferences between different registers as a resource.
From the Cambridge English Corpus
In sum, to have any chance of identifying interferences correctly one needs to be sure that the data collected come from a truly monolingual mode.
From the Cambridge English Corpus
We emphasise the role of computing interferences, that is, the necessity of avoiding them in order to give a causal implementation to logical operations.
From the Cambridge English Corpus
However, in real life, interferences are not always that bad.
From the Cambridge English Corpus
In the same way, spiritualism avoids logical interferences, but this does not mean that they do not make sense.
From the Cambridge English Corpus
The approaches followed in circuit design to deal with computing interferences fall into two main classes.
From the Cambridge English Corpus
Moreover, our encoding was also designed to avoid all interferences with other processes (if we restrict internal names for the request/server mechanism).
From the Cambridge English Corpus
Interlanguage errors, also called interferences, are due to the first language influencing the second language.
From the Cambridge English Corpus
Obviously, with proper design, the problem of interferences can be avoided yielding above emphasized necessary conditions of the integrated robotic system design.
From the Cambridge English Corpus
At the lowest level, the correct functioning of a single component may be endangered by computing interferences within the component itself, due to internal loops and instabilities of internal variables.
From the Cambridge English Corpus
There is a physical analogy: when you enter a plane, you are supposed to turn off your cellular phone, because of interferences: that is a smart spiritual move.
From the Cambridge English Corpus
The interferences and resonances between these influences pose aesthetic questions that are explored within the piece and its performance, while remaining open for the analyst and audience.
From the Cambridge English Corpus
To avoid unwanted interferences that might be caused by using the same sentence twice, different names were used in each of the two experimental sentences made from one stimulus sentence.
From the Cambridge English Corpus
We want to use natural causes as much as possible, because artificial interferences are often fraught with great danger.
From the Hansard archive
Example from the Hansard archive. Contains Parliamentary information licensed under the Open Parliament Licence v3.0
See all examples of interference
These examples are from corpora and from sources on the web. Any opinions in the examples do not represent the opinion of the Cambridge Dictionary editors or of Cambridge University Press or its licensors.
Collocations with interference
interference
These are words often used in combination with interference.Click on a collocation to see more examples of it.
arbitrary interferenceIn these treaties, privacy is recognized as a form of autonomy-a way to ensure protection from ' 'arbitrary interference' '1 by the state or other entities.
From the Cambridge English Corpus
bureaucratic interferenceThis is a quite monstrous case of bureaucratic interference.
From the Hansard archive
Example from the Hansard archive. Contains Parliamentary information licensed under the Open Parliament Licence v3.0
constant interferenceBut this coming and going, this constant pinpricking, this constant interference without any consecutive thought and philosophy behind it, is not something to take lightly.
From the Hansard archive
Example from the Hansard archive. Contains Parliamentary information licensed under the Open Parliament Licence v3.0
These examples are from corpora and from sources on the web. Any opinions in the examples do not represent the opinion of the Cambridge Dictionary editors or of Cambridge University Press or its licensors.
See all collocations with interference
What is the pronunciation of interference?
C1,C2
Translations of interference
in Chinese (Traditional)
干涉,干預, (雜訊或其他電子訊號對電視或收音機的)干擾…
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in Chinese (Simplified)
干涉,干预, (噪声或其他电子信号对电视或收音机的)干扰…
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in Spanish
intromisión, injerencia, interferencias…
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in Portuguese
intromissão, interferência, intrometimento [masculine]…
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in Marathi
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in Catalan
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हस्तक्षेप, ढवळाढवळ, गोंगाट…
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干渉, 混信, 干渉(かんしょう)…
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müdahale, burnunu sokma, karışma…
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intrusion [feminine], ingérence [feminine], interférence [feminine]…
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ingerència, intromissió, interferència…
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inmenging, storing…
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யாராவது ஒரு சூழ்நிலையில் தலையிட முயற்சிக்கும் ஒரு சந்தர்ப்பம், தொலைக்காட்சி அல்லது வானொலியில் நல்ல படங்கள் அல்லது ஒலியைப் பெறுவதைத் தடுக்கும் சத்தம் அல்லது பிற மின்னணு சமிக்ஞைகள்…
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(एक व्यक्ति के द्वारा किसी परिस्थिति में) हस्तक्षेप, टेलीविज़न या रेडियो पर अच्छी तस्वीरें या आवाज़ को बाधित करने वाले शोर या इलेक्ट्रॉनिक संकेत…
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હસ્તક્ષેપ, રુકાવટ, અવરોધ…
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indblanding, forstyrrelse…
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inblandning, störningar…
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masuk campur, gangguan…
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die Einmischung, die Störung…
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innblanding [masculine], forstyrrelse [masculine], interferens [masculine]…
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مداخلت, رکاوٹ, ٹیلی ویژن کے پردہ پر پیدا ہونے والی مداخلت…
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втручання, перешкоди…
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вмешательство, помехи…
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జోక్యం/ ఎవరైనా ఒక పరిస్థితిలో జోక్యం చేసుకోవడానికి ప్రయత్నించిన ఒక సందర్భం, టెలివిజన్ లేదా రేడియోలో నుంచి మంచి చిత్రాలు లేదా ధ్వని పొందకుండా మిమ్మల్ని ఆపే శబ్దం లేదా ఇతర ఎలక్ట్రానిక్ సిగ్నల్స్…
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تَدخّل, تَشويش…
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হস্তক্ষেপ করা, আওয়াজ বা অন্যান্য ইলেকট্রনিক সংকেত যা আপনাকে টেলিভিশন বা রেডিওতে ভাল ছবি বা শব্দ পেতে বাধা দেয়…
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zasahování, rušení, interference…
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turut campur, gangguan…
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สิ่งรบกวน, เสียงรบกวน…
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sự can thiệp, sự nhiễu…
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ingerencja, zakłócenia, mieszanie się…
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간섭, 방해…
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interferenza, ingerenza, intromissione…
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17.1 Understanding Diffraction and Interference - Physics | OpenStax
Understanding Diffraction and Interference - Physics | OpenStaxSkip to ContentGo to accessibility pageKeyboard shortcuts menuPhysics17.1 Understanding Diffraction and InterferencePhysics17.1 Understanding Diffraction and InterferenceSearchSearchCloseSearchContentsContentsHighlightsPrintTable of contentsPreface1
What is Physics?Introduction1.1 Physics: Definitions and Applications1.2 The Scientific Methods1.3 The Language of Physics: Physical Quantities and UnitsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response2
Motion in One DimensionIntroduction2.1 Relative Motion, Distance, and Displacement2.2 Speed and Velocity2.3 Position vs. Time Graphs2.4 Velocity vs. Time GraphsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response3
AccelerationIntroduction3.1 Acceleration3.2 Representing Acceleration with Equations and GraphsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response4
Forces and Newton’s Laws of MotionIntroduction4.1 Force4.2 Newton's First Law of Motion: Inertia4.3 Newton's Second Law of Motion4.4 Newton's Third Law of MotionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response5
Motion in Two DimensionsIntroduction5.1 Vector Addition and Subtraction: Graphical Methods5.2 Vector Addition and Subtraction: Analytical Methods5.3 Projectile Motion5.4 Inclined Planes5.5 Simple Harmonic MotionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response6
Circular and Rotational MotionIntroduction6.1 Angle of Rotation and Angular Velocity6.2 Uniform Circular Motion6.3 Rotational MotionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response7
Newton's Law of GravitationIntroduction7.1 Kepler's Laws of Planetary Motion7.2 Newton's Law of Universal Gravitation and Einstein's Theory of General RelativityKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response8
MomentumIntroduction8.1 Linear Momentum, Force, and Impulse8.2 Conservation of Momentum8.3 Elastic and Inelastic CollisionsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response9
Work, Energy, and Simple MachinesIntroduction9.1 Work, Power, and the Work–Energy Theorem9.2 Mechanical Energy and Conservation of Energy9.3 Simple MachinesKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response10
Special RelativityIntroduction10.1 Postulates of Special Relativity10.2 Consequences of Special RelativityKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response11
Thermal Energy, Heat, and WorkIntroduction11.1 Temperature and Thermal Energy11.2 Heat, Specific Heat, and Heat Transfer11.3 Phase Change and Latent HeatKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response12
ThermodynamicsIntroduction12.1 Zeroth Law of Thermodynamics: Thermal Equilibrium12.2 First law of Thermodynamics: Thermal Energy and Work12.3 Second Law of Thermodynamics: Entropy12.4 Applications of Thermodynamics: Heat Engines, Heat Pumps, and RefrigeratorsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response13
Waves and Their PropertiesIntroduction13.1 Types of Waves13.2 Wave Properties: Speed, Amplitude, Frequency, and Period13.3 Wave Interaction: Superposition and InterferenceKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response14
SoundIntroduction14.1 Speed of Sound, Frequency, and Wavelength14.2 Sound Intensity and Sound Level14.3 Doppler Effect and Sonic Booms14.4 Sound Interference and ResonanceKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response15
LightIntroduction15.1 The Electromagnetic Spectrum15.2 The Behavior of Electromagnetic RadiationKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response16
Mirrors and LensesIntroduction16.1 Reflection16.2 Refraction16.3 LensesKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response17
Diffraction and InterferenceIntroduction17.1 Understanding Diffraction and Interference17.2 Applications of Diffraction, Interference, and CoherenceKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response18
Static ElectricityIntroduction18.1 Electrical Charges, Conservation of Charge, and Transfer of Charge18.2 Coulomb's law18.3 Electric Field18.4 Electric Potential18.5 Capacitors and DielectricsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response19
Electrical CircuitsIntroduction19.1 Ohm's law19.2 Series Circuits19.3 Parallel Circuits19.4 Electric PowerKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response20
MagnetismIntroduction20.1 Magnetic Fields, Field Lines, and Force20.2 Motors, Generators, and Transformers20.3 Electromagnetic InductionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response21
The Quantum Nature of LightIntroduction21.1 Planck and Quantum Nature of Light21.2 Einstein and the Photoelectric Effect21.3 The Dual Nature of LightKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response22
The AtomIntroduction22.1 The Structure of the Atom22.2 Nuclear Forces and Radioactivity22.3 Half Life and Radiometric Dating22.4 Nuclear Fission and Fusion22.5 Medical Applications of Radioactivity: Diagnostic Imaging and RadiationKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response23
Particle PhysicsIntroduction23.1 The Four Fundamental Forces23.2 Quarks23.3 The Unification of ForcesKey TermsSection SummaryChapter ReviewConcept ItemsCritical Thinking ItemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended ResponseA | Reference TablesIndex
Section Learning Objectives
By the end of this section, you will be able to do the following:
Explain wave behavior of light, including diffraction and interference, including the role of constructive and destructive interference in Young’s single-slit and double-slit experiments
Perform calculations involving diffraction and interference, in particular the wavelength of light using data from a two-slit interference pattern
Teacher Support
Teacher Support
The learning objectives in this section will help your students master the following standards:
(7) Science concepts. The student knows the characteristics and behavior of waves. The student is expected to:
(D)
investigate behaviors of waves, including reflection, refraction, diffraction, interference, resonance, and the Doppler effect
Section Key Terms
diffraction
Huygens’s principle
monochromatic
wavefront
Diffraction and Interference
Teacher Support
Teacher Support
[BL]Explain constructive and destructive interference graphically on the board.
[OL]Ask students to look closely at a shadow. Ask why the edges are not sharp lines. Explain that this is caused by diffraction, one of the wave properties of electromagnetic radiation. Define the nanometer in relation to other metric length measurements.
[AL]Ask students which, among speed, frequency, and wavelength, stay the same, and which change, when a ray of light travels from one medium to another. Discuss those quantities in terms of colors (wavelengths) of visible light.
We know that visible light is the type of electromagnetic wave to which our eyes responds. As we have seen previously, light obeys the equation
c=fλ,
c=fλ,
where
c=3.00×
10
8
c=3.00×
10
8
m/s is the speed of light in vacuum, f is the frequency of the electromagnetic wave in Hz (or s–1), and
λ
λ is its wavelength in m. The range of visible wavelengths is approximately 380 to 750 nm. As is true for all waves, light travels in straight lines and acts like a ray when it interacts with objects several times as large as its wavelength. However, when it interacts with smaller objects, it displays its wave characteristics prominently. Interference is the identifying behavior of a wave.
In Figure 17.2, both the ray and wave characteristics of light can be seen. The laser beam emitted by the observatory represents ray behavior, as it travels in a straight line. Passing a pure, one-wavelength beam through vertical slits with a width close to the wavelength of the beam reveals the wave character of light. Here we see the beam spreading out horizontally into a pattern of bright and dark regions that are caused by systematic constructive and destructive interference. As it is characteristic of wave behavior, interference is observed for water waves, sound waves, and light waves.
Figure
17.2
(a) The light beam emitted by a laser at the Paranal Observatory (part of the European Southern Observatory in Chile) acts like a ray, traveling in a straight line. (credit: Yuri Beletsky, European Southern Observatory) (b) A laser beam passing through a grid of vertical slits produces an interference pattern—characteristic of a wave. (credit: Shim’on and Slava Rybka, Wikimedia Commons)
That interference is a characteristic of energy propagation by waves is demonstrated more convincingly by water waves. Figure 17.3 shows water waves passing through gaps between some rocks. You can easily see that the gaps are similar in width to the wavelength of the waves and that this causes an interference pattern as the waves pass beyond the gaps. A cross-section across the waves in the foreground would show the crests and troughs characteristic of an interference pattern.
Figure
17.3
Incoming waves (at the top of the picture) pass through the gaps in the rocks and create an interference pattern (in the foreground).
Light has wave characteristics in various media as well as in a vacuum. When light goes from a vacuum to some medium, such as water, its speed and wavelength change, but its frequency, f, remains the same. The speed of light in a medium is
v=c/n
v=c/n
, where n is its index of refraction. If you divide both sides of the equation
c=fλ
c=fλ
by n, you get
c/n=v=fλ/n
c/n=v=fλ/n
. Therefore,
v=f
λ
n
v=f
λ
n
, where
λ
n
λ
n
is the wavelength in a medium, and
λ
n
=
λ
n
,
λ
n
=
λ
n
,
where
λ
λ is the wavelength in vacuum and n is the medium’s index of refraction. It follows that the wavelength of light is smaller in any medium than it is in vacuum. In water, for example, which has n = 1.333, the range of visible wavelengths is (380 nm)/1.333 to (760 nm)/1.333, or
λ
n
=
λ
n
=
285–570 nm. Although wavelengths change while traveling from one medium to another, colors do not, since colors are associated with frequency.
The Dutch scientist Christiaan Huygens (1629–1695) developed a useful technique for determining in detail how and where waves propagate. He used wavefronts, which are the points on a wave’s surface that share the same, constant phase (such as all the points that make up the crest of a water wave). Huygens’s principle states, “Every point on a wavefront is a source of wavelets that spread out in the forward direction at the same speed as the wave itself. The new wavefront is a line tangent to all of the wavelets.”
Figure 17.4 shows how Huygens’s principle is applied. A wavefront is the long edge that moves; for example, the crest or the trough. Each point on the wavefront emits a semicircular wave that moves at the propagation speed v. These are drawn later at a time, t, so that they have moved a distance
s=vt
s=vt
. The new wavefront is a line tangent to the wavelets and is where the wave is located at time t. Huygens’s principle works for all types of waves, including water waves, sound waves, and light waves. It will be useful not only in describing how light waves propagate, but also in how they interfere.
Figure
17.4
Huygens’s principle applied to a straight wavefront. Each point on the wavefront emits a semicircular wavelet that moves a distance
s=vt
s=vt . The new wavefront is a line tangent to the wavelets.
What happens when a wave passes through an opening, such as light shining through an open door into a dark room? For light, you expect to see a sharp shadow of the doorway on the floor of the room, and you expect no light to bend around corners into other parts of the room. When sound passes through a door, you hear it everywhere in the room and, thus, you understand that sound spreads out when passing through such an opening. What is the difference between the behavior of sound waves and light waves in this case? The answer is that the wavelengths that make up the light are very short, so that the light acts like a ray. Sound has wavelengths on the order of the size of the door, and so it bends around corners.
Teacher Support
Teacher Support
[OL]Discuss the fact that, for a diffraction pattern to be visible, the width of a slit must be roughly the wavelength of the light. Try to give students an idea of the size of visible light wavelengths by noting that a human hair is roughly 100 times wider.
If light passes through smaller openings, often called slits, you can use Huygens’s principle to show that light bends as sound does (see Figure 17.5). The bending of a wave around the edges of an opening or an obstacle is called diffraction. Diffraction is a wave characteristic that occurs for all types of waves. If diffraction is observed for a phenomenon, it is evidence that the phenomenon is produced by waves. Thus, the horizontal diffraction of the laser beam after it passes through slits in Figure 17.2 is evidence that light has the properties of a wave.
Figure
17.5
Huygens’s principle applied to a straight wavefront striking an opening. The edges of the wavefront bend after passing through the opening, a process called diffraction. The amount of bending is more extreme for a small opening, consistent with the fact that wave characteristics are most noticeable for interactions with objects about the same size as the wavelength.
Once again, water waves present a familiar example of a wave phenomenon that is easy to observe and understand, as shown in Figure 17.6.
Figure
17.6
Ocean waves pass through an opening in a reef, resulting in a diffraction pattern. Diffraction occurs because the opening is similar in width to the wavelength of the waves.
Watch Physics
Single-Slit Interference
This video works through the math needed to predict diffraction patterns that are caused by single-slit interference.
Access multimedia content
Which values of m denote the location of destructive interference in a single-slit diffraction pattern?
whole integers, excluding zero
whole integers
real numbers excluding zero
real numbers
The fact that Huygens’s principle worked was not considered enough evidence to prove that light is a wave. People were also reluctant to accept light’s wave nature because it contradicted the ideas of Isaac Newton, who was still held in high esteem. The acceptance of the wave character of light came after 1801, when the English physicist and physician Thomas Young (1773–1829) did his now-classic double-slit experiment (see Figure 17.7).
Figure
17.7
Young’s double-slit experiment. Here, light of a single wavelength passes through a pair of vertical slits and produces a diffraction pattern on the screen—numerous vertical light and dark lines that are spread out horizontally. Without diffraction and interference, the light would simply make two lines on the screen.
When light passes through narrow slits, it is diffracted into semicircular waves, as shown in Figure 17.8 (a). Pure constructive interference occurs where the waves line up crest to crest or trough to trough. Pure destructive interference occurs where they line up crest to trough. The light must fall on a screen and be scattered into our eyes for the pattern to be visible. An analogous pattern for water waves is shown in Figure 17.8 (b). Note that regions of constructive and destructive interference move out from the slits at well-defined angles to the original beam. Those angles depend on wavelength and the distance between the slits, as you will see below.
Figure
17.8
Double slits produce two sources of waves that interfere. (a) Light spreads out (diffracts) from each slit, because the slits are narrow. The waves overlap and interfere constructively (bright lines) and destructively (dark regions). You can only see the effect if the light falls onto a screen and is scattered into your eyes. (b) The double-slit interference pattern for water waves is nearly identical to that for light. Wave action is greatest in regions of constructive interference and least in regions of destructive interference. (c) When light that has passed through double slits falls on a screen, we see a pattern such as this.
Virtual Physics
Wave Interference
Access multimedia content
This simulation demonstrates most of the wave phenomena discussed in this section. First, observe interference between two sources of electromagnetic radiation without adding slits. See how water waves, sound, and light all show interference patterns. Stay with light waves and use only one source. Create diffraction patterns with one slit and then with two. You may have to adjust slit width to see the pattern.
Visually compare the slit width to the wavelength. When do you get the best-defined diffraction pattern?
when the slit width is larger than the wavelength
when the slit width is smaller than the wavelength
when the slit width is comparable to the wavelength
when the slit width is infinite
Calculations Involving Diffraction and Interference
Teacher Support
Teacher Support
[BL]The Greek letter
θ
θ is spelled theta. The Greek letter
λ
λ is spelled lamda. Both are pronounced the way you would expect from the spelling. The plurals of maximum and minimum are maxima and minima, respectively.
[OL]Explain that monochromatic means one color. Monochromatic also means one frequency. The sine of an angle is the opposite side of a right triangle divided by the hypotenuse. Opposite means opposite the given acute angle. Note that the sign of an angle is always ≥ 1.
The fact that the wavelength of light of one color, or monochromatic light, can be calculated from its two-slit diffraction pattern in Young’s experiments supports the conclusion that light has wave properties. To understand the basis of such calculations, consider how two waves travel from the slits to the screen. Each slit is a different distance from a given point on the screen. Thus different numbers of wavelengths fit into each path. Waves start out from the slits in phase (crest to crest), but they will end up out of phase (crest to trough) at the screen if the paths differ in length by half a wavelength, interfering destructively. If the paths differ by a whole wavelength, then the waves arrive in phase (crest to crest) at the screen, interfering constructively. More generally, if the paths taken by the two waves differ by any half-integral number of wavelengths
(
1
2
λ,
3
2
λ,
5
2
λ, etc.)
(
1
2
λ,
3
2
λ,
5
2
λ, etc.)
, then destructive interference occurs. Similarly, if the paths taken by the two waves differ by any integral number of wavelengths
(λ, 2λ, 3λ, etc.)
(λ, 2λ, 3λ, etc.)
, then constructive interference occurs.
Figure 17.9 shows how to determine the path-length difference for waves traveling from two slits to a common point on a screen. If the screen is a large distance away compared with the distance between the slits, then the angle
θ
θ between the path and a line from the slits perpendicular to the screen (see the figure) is nearly the same for each path. That approximation and simple trigonometry show the length difference,
ΔL
ΔL, to be
dsinθ
dsinθ, where d is the distance between the slits,
ΔL=dsinθ.
ΔL=dsinθ.
To obtain constructive interference for a double slit, the path-length difference must be an integral multiple of the wavelength, or
dsinθ=mλ, for m=0,1,−1,2,−2,…(constructive).
dsinθ=mλ, for m=0,1,−1,2,−2,…(constructive).
Similarly, to obtain destructive interference for a double slit, the path-length difference must be a half-integral multiple of the wavelength, or
dsinθ=(m+½)λ, for m=0,1,−1,2,−2,…(destructive).
dsinθ=(m+½)λ, for m=0,1,−1,2,−2,…(destructive).
The number m is the order of the interference. For example, m = 4 is fourth-order interference.
Figure
17.9
The paths from each slit to a common point on the screen differ by an amount
d sin θ
d sin θ, assuming the distance to the screen is much greater than the distance between the slits (not to scale here).
Figure 17.10 shows how the intensity of the bands of constructive interference decreases with increasing angle.
Figure
17.10
The interference pattern for a double slit has an intensity that falls off with angle. The photograph shows multiple bright and dark lines, or fringes, formed by light passing through a double slit.
Light passing through a single slit forms a diffraction pattern somewhat different from that formed by double slits. Figure 17.11 shows a single-slit diffraction pattern. Note that the central maximum is larger than those on either side, and that the intensity decreases rapidly on either side.
Figure
17.11
(a) Single-slit diffraction pattern. Monochromatic light passing through a single slit produces a central maximum and many smaller and dimmer maxima on either side. The central maximum is six times higher than shown. (b) The drawing shows the bright central maximum and dimmer and thinner maxima on either side. (c) The location of the minima are shown in terms of
λ
λ and D.
The analysis of single-slit diffraction is illustrated in Figure 17.12. Assuming the screen is very far away compared with the size of the slit, rays heading toward a common destination are nearly parallel. That approximation allows a series of trigonometric operations that result in the equations for the minima produced by destructive interference.
Dsinθ=mλ
Dsinθ=mλ
or
Dy
L
=mλ
Dy
L
=mλ
When rays travel straight ahead, they remain in phase and a central maximum is obtained. However, when rays travel at an angle
θ
θ relative to the original direction of the beam, each ray travels a different distance to the screen, and they can arrive in or out of phase. Thus, a ray from the center travels a distance
λ/2
λ/2
farther than the ray from the top edge of the slit, they arrive out of phase, and they interfere destructively. Similarly, for every ray between the top and the center of the slit, there is a ray between the center and the bottom of the slit that travels a distance
λ/2
λ/2
farther to the common point on the screen, and so interferes destructively. Symmetrically, there will be another minimum at the same angle below the direct ray.
Figure
17.12
Equations for a single-slit diffraction pattern, where λ is the wavelength of light, D is the slit width,
θ
θ is the angle between a line from the slit to a minimum and a line perpendicular to the screen, L is the distance from the slit to the screen, y is the distance from the center of the pattern to the minimum, and m is a nonzero integer indicating the order of the minimum.
Below we summarize the equations needed for the calculations to follow.
The speed of light in a vacuum, c, the wavelength of the light,
λ
λ, and its frequency, f, are related as follows.
c=fλ
c=fλ
The wavelength of light in a medium,
λ
n
λ
n
, compared to its wavelength in a vacuum,
λ
λ, is given by
λ
n
=
λ
n
.
λ
n
=
λ
n
.
17.1
To calculate the positions of constructive interference for a double slit, the path-length difference must be an integral multiple, m, of the wavelength.
λ
λ
dsinθ=mλ, for m=0,1,−1,2,−2,…(constructive),
dsinθ=mλ, for m=0,1,−1,2,−2,…(constructive),
where d is the distance between the slits and
θ
θ is the angle between a line from the slits to the maximum and a line perpendicular to the barrier in which the slits are located. To calculate the positions of destructive interference for a double slit, the path-length difference must be a half-integral multiple of the wavelength:
dsinθ=(m+½)λ, for m=0,1,−1,2,−2,…(destructive).
dsinθ=(m+½)λ, for m=0,1,−1,2,−2,…(destructive).
For a single-slit diffraction pattern, the width of the slit, D, the distance of the first (m = 1) destructive interference minimum, y, the distance from the slit to the screen, L, and the wavelength,
λ
λ, are given by
Dy
L
=λ.
Dy
L
=λ.
Also, for single-slit diffraction,
Dsinθ=mλ,
Dsinθ=mλ,
where
θ
θ is the angle between a line from the slit to the minimum and a line perpendicular to the screen, and m is the order of the minimum.
Worked Example
Two-Slit Interference
Suppose you pass light from a He-Ne laser through two slits separated by 0.0100 mm, and you find that the third bright line on a screen is formed at an angle of 10.95º relative to the incident beam. What is the wavelength of the light?
Strategy
The third bright line is due to third-order constructive interference, which means that m = 3. You are given d = 0.0100 mm and
θ
θ = 10.95º. The wavelength can thus be found using the equation
dsinθ=mλ
dsinθ=mλ
for constructive interference.
Solution
The equation is
dsinθ=mλ
dsinθ=mλ
. Solving for the wavelength,
λ
λ, gives
λ=
dsinθ
m
.
λ=
dsinθ
m
.
17.2
Substituting known values yields
λ=
(
0.0100 mm
)(
sin 10.95°
)
3
=6.33×
10
−4
mm=633 nm.
λ=
(
0.0100 mm
)(
sin 10.95°
)
3
=6.33×
10
−4
mm=633 nm.
17.3
Discussion
To three digits, 633 nm is the wavelength of light emitted by the common He-Ne laser. Not by coincidence, this red color is similar to that emitted by neon lights. More important, however, is the fact that interference patterns can be used to measure wavelength. Young did that for visible wavelengths. His analytical technique is still widely used to measure electromagnetic spectra. For a given order, the angle for constructive interference increases with
λ
λ, so spectra (measurements of intensity versus wavelength) can be obtained.
Worked Example
Single-Slit Diffraction
Visible light of wavelength 550 nm falls on a single slit and produces its second diffraction minimum at an angle of 45.0° relative to the incident direction of the light. What is the width of the slit?
Strategy
From the given information, and assuming the screen is far away from the slit, you can use the equation
Dsinθ=mλ
Dsinθ=mλ
to find D.
Solution
Quantities given are
λ
λ = 550 nm, m = 2, and
θ
2
θ
2
= 45.0°. Solving the equation
Dsinθ=mλ
Dsinθ=mλ
for D and substituting known values gives
D=
mλ
sinθ
=
2(550 nm)
sin45.0°
=1.56×
10
−6
m.
D=
mλ
sinθ
=
2(550 nm)
sin45.0°
=1.56×
10
−6
m.
17.4
Discussion
You see that the slit is narrow (it is only a few times greater than the wavelength of light). That is consistent with the fact that light must interact with an object comparable in size to its wavelength in order to exhibit significant wave effects, such as this single-slit diffraction pattern.
Practice Problems
1
.
Monochromatic light from a laser passes through two slits separated by
0.00500
mm
. The third bright line on a screen is formed at an angle of
18.0
∘
relative to the incident beam. What is the wavelength of the light?
51.5
nm
77.3
nm
515
nm
773
nm
2.
What is the width of a single slit through which 610-nm orange light passes to form a first diffraction minimum at an angle of 30.0°?
0.863 µm
0.704 µm
0.610 µm
1.22 µm
Check Your Understanding
Teacher Support
Teacher Support
Use these problems to assess student achievement of the section’s learning objectives. If students are struggling with a specific objective, these problems will help identify which and direct students to the relevant topics.
3
.
Which aspect of a beam of monochromatic light changes when it passes from a vacuum into water, and how does it change?
The wavelength first decreases and then increases.
The wavelength first increases and then decreases.
The wavelength increases.
The wavelength decreases.
4
.
Go outside in the sunlight and observe your shadow. It has fuzzy edges, even if you do not. Is this a diffraction effect? Explain.
This is a diffraction effect. Your whole body acts as the origin for a new wavefront.
This is a diffraction effect. Every point on the edge of your shadow acts as the origin for a new wavefront.
This is a refraction effect. Your whole body acts as the origin for a new wavefront.
This is a refraction effect. Every point on the edge of your shadow acts as the origin for a new wavefront.
5
.
Which aspect of monochromatic green light changes when it passes from a vacuum into diamond, and how does it change?
The wavelength first decreases and then increases.
The wavelength first increases and then decreases.
The wavelength increases.
The wavelength decreases.
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Authors: Paul Peter Urone, Roger Hinrichs
Publisher/website: OpenStax
Book title: Physics
Publication date: Mar 26, 2020
Location: Houston, Texas
Book URL: https://openstax.org/books/physics/pages/1-introduction
Section URL: https://openstax.org/books/physics/pages/17-1-understanding-diffraction-and-interference
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13.3 Wave Interaction: Superposition and Interference - Physics | OpenStax
Wave Interaction: Superposition and Interference - Physics | OpenStaxSkip to ContentGo to accessibility pageKeyboard shortcuts menuPhysics13.3 Wave Interaction: Superposition and InterferencePhysics13.3 Wave Interaction: Superposition and InterferenceSearchSearchCloseSearchContentsContentsHighlightsPrintTable of contentsPreface1
What is Physics?Introduction1.1 Physics: Definitions and Applications1.2 The Scientific Methods1.3 The Language of Physics: Physical Quantities and UnitsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response2
Motion in One DimensionIntroduction2.1 Relative Motion, Distance, and Displacement2.2 Speed and Velocity2.3 Position vs. Time Graphs2.4 Velocity vs. Time GraphsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response3
AccelerationIntroduction3.1 Acceleration3.2 Representing Acceleration with Equations and GraphsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response4
Forces and Newton’s Laws of MotionIntroduction4.1 Force4.2 Newton's First Law of Motion: Inertia4.3 Newton's Second Law of Motion4.4 Newton's Third Law of MotionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response5
Motion in Two DimensionsIntroduction5.1 Vector Addition and Subtraction: Graphical Methods5.2 Vector Addition and Subtraction: Analytical Methods5.3 Projectile Motion5.4 Inclined Planes5.5 Simple Harmonic MotionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response6
Circular and Rotational MotionIntroduction6.1 Angle of Rotation and Angular Velocity6.2 Uniform Circular Motion6.3 Rotational MotionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response7
Newton's Law of GravitationIntroduction7.1 Kepler's Laws of Planetary Motion7.2 Newton's Law of Universal Gravitation and Einstein's Theory of General RelativityKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response8
MomentumIntroduction8.1 Linear Momentum, Force, and Impulse8.2 Conservation of Momentum8.3 Elastic and Inelastic CollisionsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response9
Work, Energy, and Simple MachinesIntroduction9.1 Work, Power, and the Work–Energy Theorem9.2 Mechanical Energy and Conservation of Energy9.3 Simple MachinesKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response10
Special RelativityIntroduction10.1 Postulates of Special Relativity10.2 Consequences of Special RelativityKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response11
Thermal Energy, Heat, and WorkIntroduction11.1 Temperature and Thermal Energy11.2 Heat, Specific Heat, and Heat Transfer11.3 Phase Change and Latent HeatKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response12
ThermodynamicsIntroduction12.1 Zeroth Law of Thermodynamics: Thermal Equilibrium12.2 First law of Thermodynamics: Thermal Energy and Work12.3 Second Law of Thermodynamics: Entropy12.4 Applications of Thermodynamics: Heat Engines, Heat Pumps, and RefrigeratorsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response13
Waves and Their PropertiesIntroduction13.1 Types of Waves13.2 Wave Properties: Speed, Amplitude, Frequency, and Period13.3 Wave Interaction: Superposition and InterferenceKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response14
SoundIntroduction14.1 Speed of Sound, Frequency, and Wavelength14.2 Sound Intensity and Sound Level14.3 Doppler Effect and Sonic Booms14.4 Sound Interference and ResonanceKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response15
LightIntroduction15.1 The Electromagnetic Spectrum15.2 The Behavior of Electromagnetic RadiationKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response16
Mirrors and LensesIntroduction16.1 Reflection16.2 Refraction16.3 LensesKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response17
Diffraction and InterferenceIntroduction17.1 Understanding Diffraction and Interference17.2 Applications of Diffraction, Interference, and CoherenceKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response18
Static ElectricityIntroduction18.1 Electrical Charges, Conservation of Charge, and Transfer of Charge18.2 Coulomb's law18.3 Electric Field18.4 Electric Potential18.5 Capacitors and DielectricsKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response19
Electrical CircuitsIntroduction19.1 Ohm's law19.2 Series Circuits19.3 Parallel Circuits19.4 Electric PowerKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response20
MagnetismIntroduction20.1 Magnetic Fields, Field Lines, and Force20.2 Motors, Generators, and Transformers20.3 Electromagnetic InductionKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response21
The Quantum Nature of LightIntroduction21.1 Planck and Quantum Nature of Light21.2 Einstein and the Photoelectric Effect21.3 The Dual Nature of LightKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsProblemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response22
The AtomIntroduction22.1 The Structure of the Atom22.2 Nuclear Forces and Radioactivity22.3 Half Life and Radiometric Dating22.4 Nuclear Fission and Fusion22.5 Medical Applications of Radioactivity: Diagnostic Imaging and RadiationKey TermsSection SummaryKey EquationsChapter ReviewConcept ItemsCritical Thinking ItemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended Response23
Particle PhysicsIntroduction23.1 The Four Fundamental Forces23.2 Quarks23.3 The Unification of ForcesKey TermsSection SummaryChapter ReviewConcept ItemsCritical Thinking ItemsPerformance TaskTest PrepMultiple ChoiceShort AnswerExtended ResponseA | Reference TablesIndex
Section Learning Objectives
By the end of this section, you will be able to do the following:
Describe superposition of waves
Describe interference of waves and distinguish between constructive and destructive interference of waves
Describe the characteristics of standing waves
Distinguish reflection from refraction of waves
Teacher Support
Teacher Support
The learning objectives in this section will help your students master the following standards:
(7) Science concepts. The student knows the characteristics and behavior of waves. The student is expected to:
(D) investigate the behaviors of waves, including reflection, refraction, diffraction, interference, resonance, and the Doppler effect.
In addition, the High School Physics Laboratory Manual addresses content in this section in the lab titled: Waves, as well as the following standards:
(7) Science concepts. The student knows the characteristics and behavior of waves. The student is expected to:
(D) investigate behaviors of waves, including reflection, refraction, diffraction, interference, resonance, and the Doppler effect.
Section Key Terms
antinode
constructive interference
destructive interference
inversion
nodes
reflection
refraction
standing wave
superposition
Teacher Support
Teacher Support
[BL][OL] Review waves, their types, and their properties, as covered in the previous sections.
Superposition of Waves
Most waves do not look very simple. They look more like the waves in Figure 13.10, rather than the simple water wave considered in the previous sections, which has a perfect sinusoidal shape.
Figure
13.10
These waves result from the superposition of several waves from different sources, producing a complex pattern. (Waterborough, Wikimedia Commons)
Teacher Support
Teacher Support
The horizontal waves in the picture bounce off the wall of the lake seen in the front part of the picture. These superimpose or combine with waves moving in a different direction. When they combine, their energies get added, forming higher peaks and lower crests in specific places. This is why the water has a crisscross pattern.
Most waves appear complex because they result from two or more simple waves that combine as they come together at the same place at the same time—a phenomenon called superposition.
Waves superimpose by adding their disturbances; each disturbance corresponds to a force, and all the forces add. If the disturbances are along the same line, then the resulting wave is a simple addition of the disturbances of the individual waves, that is, their amplitudes add.
Wave InterferenceThe two special cases of superposition that produce the simplest results are pure constructive interference and pure destructive interference.
Pure constructive interference occurs when two identical waves arrive at the same point exactly in phase. When waves are exactly in phase, the crests of the two waves are precisely aligned, as are the troughs. Refer to Figure 13.11. Because the disturbances add, the pure constructive interference of two waves with the same amplitude produces a wave that has twice the amplitude of the two individual waves, but has the same wavelength.
Figure
13.11
The pure constructive interference of two identical waves produces a wave with twice the amplitude but the same wavelength.
Figure 13.12 shows two identical waves that arrive exactly out of phase—that is, precisely aligned crest to trough—producing pure destructive interference. Because the disturbances are in opposite directions for this superposition, the resulting amplitude is zero for pure destructive interference; that is, the waves completely cancel out each other.
Figure
13.12
The pure destructive interference of two identical waves produces zero amplitude, or complete cancellation.
While pure constructive interference and pure destructive interference can occur, they are not very common because they require precisely aligned identical waves. The superposition of most waves that we see in nature produces a combination of constructive and destructive interferences.
Waves that are not results of pure constructive or destructive interference can vary from place to place and time to time. The sound from a stereo, for example, can be loud in one spot and soft in another. The varying loudness means that the sound waves add partially constructively and partially destructively at different locations. A stereo has at least two speakers that create sound waves, and waves can reflect from walls. All these waves superimpose.
An example of sounds that vary over time from constructive to destructive is found in the combined whine of jet engines heard by a stationary passenger. The volume of the combined sound can fluctuate up and down as the sound from the two engines varies in time from constructive to destructive.
The two previous examples considered waves that are similar—both stereo speakers generate sound waves with the same amplitude and wavelength, as do the jet engines. But what happens when two waves that are not similar, that is, having different amplitudes and wavelengths, are superimposed? An example of the superposition of two dissimilar waves is shown in Figure 13.13. Here again, the disturbances add and subtract, but they produce an even more complicated-looking wave. The resultant wave from the combined disturbances of two dissimilar waves looks much different than the idealized sinusoidal shape of a periodic wave.
Figure
13.13
The superposition of nonidentical waves exhibits both constructive and destructive interferences.
Virtual Physics
Wave Interference
Access multimedia content
In this simulation, make waves with a dripping faucet, an audio speaker, or a laser by switching between the water, sound, and light tabs. Contrast and compare how the different types of waves behave. Try rotating the view from top to side to make observations. Then experiment with adding a second source or a pair of slits to create an interference pattern.
PhET Explorations: Wave Interference.
Make waves with a dripping faucet, audio speaker, or laser! Add a second source or a pair of slits to create an interference pattern.
Access multimedia content
In the water tab, compare the waves generated by one drip versus two drips. What happens to the amplitude of the waves when there are two drips? Is this constructive or destructive interference? Why would this be the case?
The amplitude of the water waves remains same because of the destructive interference as the drips of water hit the surface at the same time.
The amplitude of the water waves is canceled because of the destructive interference as the drips of water hit the surface at the same time.
The amplitude of water waves remains same because of the constructive interference as the drips of water hit the surface at the same time.
The amplitude of water waves doubles because of the constructive interference as the drips of water hit the surface at the same time.
Standing Waves
Sometimes waves do not seem to move and they appear to just stand in place, vibrating. Such waves are called standing waves and are formed by the superposition of two or more waves moving in opposite directions. The waves move through each other with their disturbances adding as they go by. If the two waves have the same amplitude and wavelength, then they alternate between constructive and destructive interference. Standing waves created by the superposition of two identical waves moving in opposite directions are illustrated in Figure 13.14.
Figure
13.14
A standing wave is created by the superposition of two identical waves moving in opposite directions. The oscillations are at fixed locations in space and result from alternating constructive and destructive interferences.
As an example, standing waves can be seen on the surface of a glass of milk in a refrigerator. The vibrations from the refrigerator motor create waves on the milk that oscillate up and down but do not seem to move across the surface. The two waves that produce standing waves may be due to the reflections from the side of the glass.
Earthquakes can create standing waves and cause constructive and destructive interferences. As the earthquake waves travel along the surface of Earth and reflect off denser rocks, constructive interference occurs at certain points. As a result, areas closer to the epicenter are not damaged while areas farther from the epicenter are damaged.
Standing waves are also found on the strings of musical instruments and are due to reflections of waves from the ends of the string. Figure 13.15 and Figure 13.16 show three standing waves that can be created on a string that is fixed at both ends. When the wave reaches the fixed end, it has nowhere else to go but back where it came from, causing the reflection. The nodes are the points where the string does not move; more generally, the nodes are the points where the wave disturbance is zero in a standing wave. The fixed ends of strings must be nodes, too, because the string cannot move there.
The antinode is the location of maximum amplitude in standing waves. The standing waves on a string have a frequency that is related to the propagation speed
v
w
v
w
of the disturbance on the string. The wavelength
λ
λ is determined by the distance between the points where the string is fixed in place.
Figure
13.15
The figure shows a string oscillating with its maximum disturbance as the antinode.
Figure
13.16
The figure shows a string oscillating with multiple nodes.
Reflection and Refraction of Waves
As we saw in the case of standing waves on the strings of a musical instrument, reflection is the change in direction of a wave when it bounces off a barrier, such as a fixed end. When the wave hits the fixed end, it changes direction, returning to its source. As it is reflected, the wave experiences an inversion, which means that it flips vertically. If a wave hits the fixed end with a crest, it will return as a trough, and vice versa (Henderson 2015). Refer to Figure 13.17.
Figure
13.17
A wave is inverted after reflection from a fixed end.
Tips For Success
If the end is not fixed, it is said to be a free end, and no inversion occurs. When the end is loosely attached, it reflects without inversion, and when the end is not attached to anything, it does not reflect at all. You may have noticed this while changing the settings from Fixed End to Loose End to No End in the Waves on a String PhET simulation.
Rather than encountering a fixed end or barrier, waves sometimes pass from one medium into another, for instance, from air into water. Different types of media have different properties, such as density or depth, that affect how a wave travels through them. At the boundary between media, waves experience refraction—they change their path of propagation. As the wave bends, it also changes its speed and wavelength upon entering the new medium. Refer to Figure 13.18.
Figure
13.18
A wave refracts as it enters a different medium.
For example, water waves traveling from the deep end to the shallow end of a swimming pool experience refraction. They bend in a path closer to perpendicular to the surface of the water, propagate slower, and decrease in wavelength as they enter shallower water.
Check Your Understanding
Teacher Support
Teacher Support
Use these questions to assess students’ achievement of the section’s learning objectives. If students are struggling with a specific objective, these questions will help identify such objective and direct them to the relevant content.
13.
What is the superposition of waves?
When a single wave splits into two different waves at a point
When two waves combine at the same place at the same time
14.
How do waves superimpose on one another?
By adding their frequencies
By adding their wavelengths
By adding their disturbances
By adding their speeds
15
.
What is interference of waves?
Interference is a superposition of two waves to form a resultant wave with higher or lower frequency.
Interference is a superposition of two waves to form a wave of larger or smaller amplitude.
Interference is a superposition of two waves to form a resultant wave with higher or lower velocity.
Interference is a superposition of two waves to form a resultant wave with longer or shorter wavelength.
16.
Is the following statement true or false? The two types of interference are constructive and destructive interferences.
True
False
17.
What are standing waves?
Waves that appear to remain in one place and do not seem to move
Waves that seem to move along a trajectory
18
.
How are standing waves formed?
Standing waves are formed by the superposition of two or more waves moving in opposite directions.
Standing waves are formed by the superposition of two or more waves moving in the same direction.
Standing waves are formed by the superposition of two or more waves moving in perpendicular directions.
Standing waves are formed by the superposition of two or more waves moving in arbitrary directions.
19
.
What is the reflection of a wave?
The reflection of a wave is the change in amplitude of a wave when it bounces off a barrier.
The reflection of a wave is the change in frequency of a wave when it bounces off a barrier.
The reflection of a wave is the change in velocity of a wave when it bounces off a barrier.
The reflection of a wave is the change in direction of a wave when it bounces off a barrier.
20
.
What is inversion of a wave?
Inversion occurs when a wave reflects off a fixed end and the wave amplitude changes sign.
Inversion occurs when a wave reflects off a loose end and the wave amplitude changes sign.
Inversion occurs when a wave reflects off a fixed end without the wave amplitude changing sign.
Inversion occurs when a wave reflects off a loose end without the wave amplitude changing sign.
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Location: Houston, Texas
Book URL: https://openstax.org/books/physics/pages/1-introduction
Section URL: https://openstax.org/books/physics/pages/13-3-wave-interaction-superposition-and-interference
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1Etymology
2Mechanisms
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2.1Real-valued wave functions
2.2Between two plane waves
2.3Between two spherical waves
2.4Multiple beams
3Complex valued wave functions
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3.1Optical wave interference
3.1.1Light source requirements
3.1.2Optical arrangements
3.2Quantum interference
4Applications
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4.1Beat
4.2Optical interferometry
4.3Radio interferometry
4.4Acoustic interferometry
5See also
6References
7External links
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Wave interference
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From Wikipedia, the free encyclopedia
Phenomenon resulting from the superposition of two waves
For interference in radio communications, see Interference (communication).
"Interference pattern" redirects here. For Moiré patterns, see Moiré pattern.
This article may be too technical for most readers to understand. Please help improve it to make it understandable to non-experts, without removing the technical details. (February 2022) (Learn how and when to remove this template message)
The interference of two waves. In phase: the two lower waves combine (left panel), resulting in a wave of added amplitude (constructive interference). Out of phase: (here by 180 degrees), the two lower waves combine (right panel), resulting in a wave of zero amplitude (destructive interference).
In physics, interference is a phenomenon in which two coherent waves are combined by adding their intensities or displacements with due consideration for their phase difference. The resultant wave may have greater intensity (constructive interference) or lower amplitude (destructive interference) if the two waves are in phase or out of phase, respectively.
Interference effects can be observed with all types of waves, for example, light, radio, acoustic, surface water waves, gravity waves, or matter waves as well as in loudspeakers as electrical waves.
Etymology[edit]
The word interference is derived from the Latin words inter which means "between" and fere which means "hit or strike", and was coined by Thomas Young in 1801.[1][2][3]
Mechanisms[edit]
Interference of right traveling (green) and left traveling (blue) waves in Two-dimensional space, resulting in final (red) wave
Interference of waves from two point sources.
Cropped tomography scan animation of laser light interference passing through two pinholes (side edges).
The principle of superposition of waves states that when two or more propagating waves of the same type are incident on the same point, the resultant amplitude at that point is equal to the vector sum of the amplitudes of the individual waves.[4] If a crest of a wave meets a crest of another wave of the same frequency at the same point, then the amplitude is the sum of the individual amplitudes—this is constructive interference. If a crest of one wave meets a trough of another wave, then the amplitude is equal to the difference in the individual amplitudes—this is known as destructive interference. In ideal mediums (water, air are almost ideal) energy is always conserved, at points of destructive interference energy is stored in the elasticity of the medium. For example when we drop 2 pebbles in a pond we see a pattern but eventually waves continue and only when they reach the shore is the energy absorbed away from the medium.
A magnified image of a coloured interference pattern in a soap film. The "black holes" are areas of almost total destructive interference (antiphase).
Constructive interference occurs when the phase difference between the waves is an even multiple of π (180°), whereas destructive interference occurs when the difference is an odd multiple of π. If the difference between the phases is intermediate between these two extremes, then the magnitude of the displacement of the summed waves lies between the minimum and maximum values.
Consider, for example, what happens when two identical stones are dropped into a still pool of water at different locations. Each stone generates a circular wave propagating outwards from the point where the stone was dropped. When the two waves overlap, the net displacement at a particular point is the sum of the displacements of the individual waves. At some points, these will be in phase, and will produce a maximum displacement. In other places, the waves will be in anti-phase, and there will be no net displacement at these points. Thus, parts of the surface will be stationary—these are seen in the figure above and to the right as stationary blue-green lines radiating from the centre.
Interference of light is a unique phenomenon in that we can never observe superposition of the EM field directly as we can, for example, in water. Superposition in the EM field is an assumed phenomenon and necessary to explain how two light beams pass through each other and continue on their respective paths. Prime examples of light interference are the famous double-slit experiment, laser speckle, anti-reflective coatings and interferometers.
In addition to classical wave model for understanding optical interference, quantum matter waves also demonstrate interference.
Real-valued wave functions[edit]
The above can be demonstrated in one dimension by deriving the formula for the sum of two waves. The equation for the amplitude of a sinusoidal wave traveling to the right along the x-axis is
W
1
(
x
,
t
)
=
A
cos
(
k
x
−
ω
t
)
{\displaystyle W_{1}(x,t)=A\cos(kx-\omega t)}
where
A
{\displaystyle A}
is the peak amplitude,
k
=
2
π
/
λ
{\displaystyle k=2\pi /\lambda }
is the wavenumber and
ω
=
2
π
f
{\displaystyle \omega =2\pi f}
is the angular frequency of the wave. Suppose a second wave of the same frequency and amplitude but with a different phase is also traveling to the right
W
2
(
x
,
t
)
=
A
cos
(
k
x
−
ω
t
+
φ
)
{\displaystyle W_{2}(x,t)=A\cos(kx-\omega t+\varphi )}
where
φ
{\displaystyle \varphi }
is the phase difference between the waves in radians. The two waves will superpose and add: the sum of the two waves is
W
1
+
W
2
=
A
[
cos
(
k
x
−
ω
t
)
+
cos
(
k
x
−
ω
t
+
φ
)
]
.
{\displaystyle W_{1}+W_{2}=A[\cos(kx-\omega t)+\cos(kx-\omega t+\varphi )].}
Using the trigonometric identity for the sum of two cosines:
cos
a
+
cos
b
=
2
cos
(
a
−
b
2
)
cos
(
a
+
b
2
)
,
{\textstyle \cos a+\cos b=2\cos \left({a-b \over 2}\right)\cos \left({a+b \over 2}\right),}
this can be written
W
1
+
W
2
=
2
A
cos
(
φ
2
)
cos
(
k
x
−
ω
t
+
φ
2
)
.
{\displaystyle W_{1}+W_{2}=2A\cos \left({\varphi \over 2}\right)\cos \left(kx-\omega t+{\varphi \over 2}\right).}
This represents a wave at the original frequency, traveling to the right like its components, whose amplitude is proportional to the cosine of
φ
/
2
{\displaystyle \varphi /2}
.
Constructive interference: If the phase difference is an even multiple of π:
φ
=
…
,
−
4
π
,
−
2
π
,
0
,
2
π
,
4
π
,
…
{\displaystyle \varphi =\ldots ,-4\pi ,-2\pi ,0,2\pi ,4\pi ,\ldots }
then
|
cos
(
φ
/
2
)
|
=
1
{\displaystyle \left|\cos(\varphi /2)\right|=1}
, so the sum of the two waves is a wave with twice the amplitude
W
1
+
W
2
=
2
A
cos
(
k
x
−
ω
t
)
{\displaystyle W_{1}+W_{2}=2A\cos(kx-\omega t)}
Destructive interference: If the phase difference is an odd multiple of π:
φ
=
…
,
−
3
π
,
−
π
,
π
,
3
π
,
5
π
,
…
{\displaystyle \varphi =\ldots ,-3\pi ,\,-\pi ,\,\pi ,\,3\pi ,\,5\pi ,\ldots }
then
cos
(
φ
/
2
)
=
0
{\displaystyle \cos(\varphi /2)=0\,}
, so the sum of the two waves is zero
W
1
+
W
2
=
0
{\displaystyle W_{1}+W_{2}=0}
Between two plane waves[edit]
Geometrical arrangement for two plane wave interference
Interference fringes in overlapping plane waves
A simple form of interference pattern is obtained if two plane waves of the same frequency intersect at an angle.
Interference is essentially an energy redistribution process. The energy which is lost at the destructive interference is regained at the constructive interference.
One wave is travelling horizontally, and the other is travelling downwards at an angle θ to the first wave. Assuming that the two waves are in phase at the point B, then the relative phase changes along the x-axis. The phase difference at the point A is given by
Δ
φ
=
2
π
d
λ
=
2
π
x
sin
θ
λ
.
{\displaystyle \Delta \varphi ={\frac {2\pi d}{\lambda }}={\frac {2\pi x\sin \theta }{\lambda }}.}
It can be seen that the two waves are in phase when
x
sin
θ
λ
=
0
,
±
1
,
±
2
,
…
,
{\displaystyle {\frac {x\sin \theta }{\lambda }}=0,\pm 1,\pm 2,\ldots ,}
and are half a cycle out of phase when
x
sin
θ
λ
=
±
1
2
,
±
3
2
,
…
{\displaystyle {\frac {x\sin \theta }{\lambda }}=\pm {\frac {1}{2}},\pm {\frac {3}{2}},\ldots }
Constructive interference occurs when the waves are in phase, and destructive interference when they are half a cycle out of phase. Thus, an interference fringe pattern is produced, where the separation of the maxima is
d
f
=
λ
sin
θ
{\displaystyle d_{f}={\frac {\lambda }{\sin \theta }}}
and df is known as the fringe spacing. The fringe spacing increases with increase in wavelength, and with decreasing angle θ.
The fringes are observed wherever the two waves overlap and the fringe spacing is uniform throughout.
Between two spherical waves[edit]
Optical interference between two point sources that have different wavelengths and separations of sources.
A point source produces a spherical wave. If the light from two point sources overlaps, the interference pattern maps out the way in which the phase difference between the two waves varies in space. This depends on the wavelength and on the separation of the point sources. The figure to the right shows interference between two spherical waves. The wavelength increases from top to bottom, and the distance between the sources increases from left to right.
When the plane of observation is far enough away, the fringe pattern will be a series of almost straight lines, since the waves will then be almost planar.
Multiple beams[edit]
Interference occurs when several waves are added together provided that the phase differences between them remain constant over the observation time.
It is sometimes desirable for several waves of the same frequency and amplitude to sum to zero (that is, interfere destructively, cancel). This is the principle behind, for example, 3-phase power and the diffraction grating. In both of these cases, the result is achieved by uniform spacing of the phases.
It is easy to see that a set of waves will cancel if they have the same amplitude and their phases are spaced equally in angle. Using phasors, each wave can be represented as
A
e
i
φ
n
{\displaystyle Ae^{i\varphi _{n}}}
for
N
{\displaystyle N}
waves from
n
=
0
{\displaystyle n=0}
to
n
=
N
−
1
{\displaystyle n=N-1}
, where
φ
n
−
φ
n
−
1
=
2
π
N
.
{\displaystyle \varphi _{n}-\varphi _{n-1}={\frac {2\pi }{N}}.}
To show that
∑
n
=
0
N
−
1
A
e
i
φ
n
=
0
{\displaystyle \sum _{n=0}^{N-1}Ae^{i\varphi _{n}}=0}
one merely assumes the converse, then multiplies both sides by
e
i
2
π
N
.
{\displaystyle e^{i{\frac {2\pi }{N}}}.}
The Fabry–Pérot interferometer uses interference between multiple reflections.
A diffraction grating can be considered to be a multiple-beam interferometer; since the peaks which it produces are generated by interference between the light transmitted by each of the elements in the grating; see interference vs. diffraction for further discussion.
Complex valued wave functions[edit]
Mechanical and gravity waves can be directly observed: they are real-valued wave functions; optical and matter waves cannot be directly observed: they are complex valued wave functions. Some of the differences between real valued and complex valued wave interference include:
The interference involves different types of mathematical functions: A classical wave is a real function representing the displacement from an equilibrium position; an optical or quantum wavefunction is a complex function. A classical wave at any point can be positive or negative; the quantum probability function is non-negative.
Any two different real waves in the same medium interfere; complex waves must be coherent to interfere. In practice this means the wave must come from the same source and have similar frequencies
Real wave interference is obtained simply by adding the displacements from equilibrium (or amplitudes) of the two waves; In complex wave interference, we measure the modulus of the wavefunction squared.
Optical wave interference[edit]
Creation of interference fringes by an optical flat on a reflective surface. Light rays from a monochromatic source pass through the glass and reflect off both the bottom surface of the flat and the supporting surface. The tiny gap between the surfaces means the two reflected rays have different path lengths. In addition the ray reflected from the bottom plate undergoes a 180° phase reversal. As a result, at locations (a) where the path difference is an odd multiple of λ/2, the waves reinforce. At locations (b) where the path difference is an even multiple of λ/2 the waves cancel. Since the gap between the surfaces varies slightly in width at different points, a series of alternating bright and dark bands, interference fringes, are seen.
Because the frequency of light waves (~1014 Hz) is too high for currently available detectors to detect the variation of the electric field of the light, it is possible to observe only the intensity of an optical interference pattern. The intensity of the light at a given point is proportional to the square of the average amplitude of the wave. This can be expressed mathematically as follows. The displacement of the two waves at a point r is:
U
1
(
r
,
t
)
=
A
1
(
r
)
e
i
[
φ
1
(
r
)
−
ω
t
]
{\displaystyle U_{1}(\mathbf {r} ,t)=A_{1}(\mathbf {r} )e^{i[\varphi _{1}(\mathbf {r} )-\omega t]}}
U
2
(
r
,
t
)
=
A
2
(
r
)
e
i
[
φ
2
(
r
)
−
ω
t
]
{\displaystyle U_{2}(\mathbf {r} ,t)=A_{2}(\mathbf {r} )e^{i[\varphi _{2}(\mathbf {r} )-\omega t]}}
where A represents the magnitude of the displacement, φ represents the phase and ω represents the angular frequency.
The displacement of the summed waves is
U
(
r
,
t
)
=
A
1
(
r
)
e
i
[
φ
1
(
r
)
−
ω
t
]
+
A
2
(
r
)
e
i
[
φ
2
(
r
)
−
ω
t
]
.
{\displaystyle U(\mathbf {r} ,t)=A_{1}(\mathbf {r} )e^{i[\varphi _{1}(\mathbf {r} )-\omega t]}+A_{2}(\mathbf {r} )e^{i[\varphi _{2}(\mathbf {r} )-\omega t]}.}
The intensity of the light at r is given by
I
(
r
)
=
∫
U
(
r
,
t
)
U
∗
(
r
,
t
)
d
t
∝
A
1
2
(
r
)
+
A
2
2
(
r
)
+
2
A
1
(
r
)
A
2
(
r
)
cos
[
φ
1
(
r
)
−
φ
2
(
r
)
]
.
{\displaystyle I(\mathbf {r} )=\int U(\mathbf {r} ,t)U^{*}(\mathbf {r} ,t)\,dt\propto A_{1}^{2}(\mathbf {r} )+A_{2}^{2}(\mathbf {r} )+2A_{1}(\mathbf {r} )A_{2}(\mathbf {r} )\cos[\varphi _{1}(\mathbf {r} )-\varphi _{2}(\mathbf {r} )].}
This can be expressed in terms of the intensities of the individual waves as
I
(
r
)
=
I
1
(
r
)
+
I
2
(
r
)
+
2
I
1
(
r
)
I
2
(
r
)
cos
[
φ
1
(
r
)
−
φ
2
(
r
)
]
.
{\displaystyle I(\mathbf {r} )=I_{1}(\mathbf {r} )+I_{2}(\mathbf {r} )+2{\sqrt {I_{1}(\mathbf {r} )I_{2}(\mathbf {r} )}}\cos[\varphi _{1}(\mathbf {r} )-\varphi _{2}(\mathbf {r} )].}
Thus, the interference pattern maps out the difference in phase between the two waves, with maxima occurring when the phase difference is a multiple of 2π. If the two beams are of equal intensity, the maxima are four times as bright as the individual beams, and the minima have zero intensity.
Classically the two waves must have the same polarization to give rise to interference fringes since it is not possible for waves of different polarizations to cancel one another out or add together. Instead, when waves of different polarization are added together, they give rise to a wave of a different polarization state.
Quantum mechanically the theories of Paul Dirac and Richard Feynman offer a more modern approach. Dirac showed that every quanta or photon of light acts on its own which he famously stated as "every photon interferes with itself". Richard Feynman showed that by evaluating a path integral where all possible paths are considered, that a number of higher probability paths will emerge. In thin films for example, film thickness which is not a multiple of light wavelength will not allow the quanta to traverse, only reflection is possible.
Light source requirements[edit]
The discussion above assumes that the waves which interfere with one another are monochromatic, i.e. have a single frequency—this requires that they are infinite in time. This is not, however, either practical or necessary. Two identical waves of finite duration whose frequency is fixed over that period will give rise to an interference pattern while they overlap. Two identical waves which consist of a narrow spectrum of frequency waves of finite duration (but shorter than their coherence time), will give a series of fringe patterns of slightly differing spacings, and provided the spread of spacings is significantly less than the average fringe spacing, a fringe pattern will again be observed during the time when the two waves overlap.
Conventional light sources emit waves of differing frequencies and at different times from different points in the source. If the light is split into two waves and then re-combined, each individual light wave may generate an interference pattern with its other half, but the individual fringe patterns generated will have different phases and spacings, and normally no overall fringe pattern will be observable. However, single-element light sources, such as sodium- or mercury-vapor lamps have emission lines with quite narrow frequency spectra. When these are spatially and colour filtered, and then split into two waves, they can be superimposed to generate interference fringes.[5] All interferometry prior to the invention of the laser was done using such sources and had a wide range of successful applications.
A laser beam generally approximates much more closely to a monochromatic source, and thus it is much more straightforward to generate interference fringes using a laser. The ease with which interference fringes can be observed with a laser beam can sometimes cause problems in that stray reflections may give spurious interference fringes which can result in errors.
Normally, a single laser beam is used in interferometry, though interference has been observed using two independent lasers whose frequencies were sufficiently matched to satisfy the phase requirements.[6]
This has also been observed for widefield interference between two incoherent laser sources.[7]
It is also possible to observe interference fringes using white light. A white light fringe pattern can be considered to be made up of a 'spectrum' of fringe patterns each of slightly different spacing. If all the fringe patterns are in phase in the centre, then the fringes will increase in size as the wavelength decreases and the summed intensity will show three to four fringes of varying colour. Young describes this very elegantly in his discussion of two slit interference. Since white light fringes are obtained only when the two waves have travelled equal distances from the light source, they can be very useful in interferometry, as they allow the zero path difference fringe to be identified.[8]
Optical arrangements[edit]
To generate interference fringes, light from the source has to be divided into two waves which then have to be re-combined. Traditionally, interferometers have been classified as either amplitude-division or wavefront-division systems.
In an amplitude-division system, a beam splitter is used to divide the light into two beams travelling in different directions, which are then superimposed to produce the interference pattern. The Michelson interferometer and the Mach–Zehnder interferometer are examples of amplitude-division systems.
In wavefront-division systems, the wave is divided in space—examples are Young's double slit interferometer and Lloyd's mirror.
Interference can also be seen in everyday phenomena such as iridescence and structural coloration. For example, the colours seen in a soap bubble arise from interference of light reflecting off the front and back surfaces of the thin soap film. Depending on the thickness of the film, different colours interfere constructively and destructively.
Iridiscence caused by thin-film interference
Smartphone with iridescent back panel
An oil spill
White light interference in a soap bubble.
Quantum interference[edit]
See also: Double-slit experiment and Matter wave
Part of a series of articles aboutQuantum mechanics
i
ℏ
∂
∂
t
|
ψ
(
t
)
⟩
=
H
^
|
ψ
(
t
)
⟩
{\displaystyle i\hbar {\frac {\partial }{\partial t}}|\psi (t)\rangle ={\hat {H}}|\psi (t)\rangle }
Schrödinger equation
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vte
Quantum interference – the observed wave-behavior of matter[9] – resembles optical interference. Let
Ψ
(
x
,
t
)
{\displaystyle \Psi (x,t)}
be a wavefunction solution of the Schrödinger equation for a quantum mechanical object. Then the probability
P
(
x
)
{\displaystyle P(x)}
of observing the object at position
x
{\displaystyle x}
is
P
(
x
)
=
|
Ψ
(
x
,
t
)
|
2
=
Ψ
∗
(
x
,
t
)
Ψ
(
x
,
t
)
{\displaystyle P(x)=|\Psi (x,t)|^{2}=\Psi ^{*}(x,t)\Psi (x,t)}
where * indicates complex conjugation. Quantum interference concerns the issue of this probability when the wavefunction is expressed as a sum or linear superposition of two terms
Ψ
(
x
,
t
)
=
Ψ
A
(
x
,
t
)
+
Ψ
B
(
x
,
t
)
{\displaystyle \Psi (x,t)=\Psi _{A}(x,t)+\Psi _{B}(x,t)}
:
P
(
x
)
=
|
Ψ
(
x
,
t
)
|
2
=
|
Ψ
A
(
x
,
t
)
|
2
+
|
Ψ
B
(
x
,
t
)
|
2
+
(
Ψ
A
∗
(
x
,
t
)
Ψ
B
(
x
,
t
)
+
Ψ
A
(
x
,
t
)
Ψ
B
∗
(
x
,
t
)
)
{\displaystyle P(x)=|\Psi (x,t)|^{2}=|\Psi _{A}(x,t)|^{2}+|\Psi _{B}(x,t)|^{2}+(\Psi _{A}^{*}(x,t)\Psi _{B}(x,t)+\Psi _{A}(x,t)\Psi _{B}^{*}(x,t))}
Usually,
Ψ
A
(
x
,
t
)
{\displaystyle \Psi _{A}(x,t)}
and
Ψ
B
(
x
,
t
)
{\displaystyle \Psi _{B}(x,t)}
correspond to distinct situations A and B. When this is the case, the equation
Ψ
(
x
,
t
)
=
Ψ
A
(
x
,
t
)
+
Ψ
B
(
x
,
t
)
{\displaystyle \Psi (x,t)=\Psi _{A}(x,t)+\Psi _{B}(x,t)}
indicates that the object can be in situation A or situation B. The above equation can then be interpreted as: The probability of finding the object at
x
{\displaystyle x}
is the probability of finding the object at
x
{\displaystyle x}
when it is in situation A plus the probability of finding the object at
x
{\displaystyle x}
when it is in situation B plus an extra term. This extra term, which is called the quantum interference term, is
Ψ
A
∗
(
x
,
t
)
Ψ
B
(
x
,
t
)
+
Ψ
A
(
x
,
t
)
Ψ
B
∗
(
x
,
t
)
{\displaystyle \Psi _{A}^{*}(x,t)\Psi _{B}(x,t)+\Psi _{A}(x,t)\Psi _{B}^{*}(x,t)}
in the above equation. As in the classical wave case above, the quantum interference term can add (constructive interference) or subtract (destructive interference) from
|
Ψ
A
(
x
,
t
)
|
2
+
|
Ψ
B
(
x
,
t
)
|
2
{\displaystyle |\Psi _{A}(x,t)|^{2}+|\Psi _{B}(x,t)|^{2}}
in the above equation depending on whether the quantum interference term is positive or negative. If this term is absent for all
x
{\displaystyle x}
, then there is no quantum mechanical interference associated with situations A and B.
The best known example of quantum interference is the double-slit experiment. In this experiment, matter waves from electrons, atoms or molecules approach a barrier with two slits in it. One slit becomes
Ψ
A
(
x
,
t
)
{\displaystyle \Psi _{A}(x,t)}
and the other becomes
Ψ
B
(
x
,
t
)
{\displaystyle \Psi _{B}(x,t)}
. The interference pattern occurs on the far side, observed by detectors suitable to the particles originating the matter wave.[10] The pattern matches the optical double slit pattern.
Applications[edit]
Beat[edit]
Main article: Beat (acoustics)
In acoustics, a beat is an interference pattern between two sounds of slightly different frequencies, perceived as a periodic variation in volume whose rate is the difference of the two frequencies.
With tuning instruments that can produce sustained tones, beats can be readily recognized. Tuning two tones to a unison will present a peculiar effect: when the two tones are close in pitch but not identical, the difference in frequency generates the beating. The volume varies like in a tremolo as the sounds alternately interfere constructively and destructively. As the two tones gradually approach unison, the beating slows down and may become so slow as to be imperceptible. As the two tones get further apart, their beat frequency starts to approach the range of human pitch perception,[11] the beating starts to sound like a note, and a combination tone is produced. This combination tone can also be referred to as a missing fundamental, as the beat frequency of any two tones is equivalent to the frequency of their implied fundamental frequency.
Main article: Interferometry
Optical interferometry[edit]
Main article: Optical interferometry
Interferometry has played an important role in the advancement of physics, and also has a wide range of applications in physical and engineering measurement.
Thomas Young's double slit interferometer in 1803 demonstrated interference fringes when two small holes were illuminated by light from another small hole which was illuminated by sunlight. Young was able to estimate the wavelength of different colours in the spectrum from the spacing of the fringes. The experiment played a major role in the general acceptance of the wave theory of light.[8]
In quantum mechanics, this experiment is considered to demonstrate the inseparability of the wave and particle natures of light and other quantum particles (wave–particle duality). Richard Feynman was fond of saying that all of quantum mechanics can be gleaned from carefully thinking through the implications of this single experiment.[12]
The results of the Michelson–Morley experiment are generally considered to be the first strong evidence against the theory of a luminiferous aether and in favor of special relativity.
Interferometry has been used in defining and calibrating length standards. When the metre was defined as the distance between two marks on a platinum-iridium bar, Michelson and Benoît used interferometry to measure the wavelength of the red cadmium line in the new standard, and also showed that it could be used as a length standard. Sixty years later, in 1960, the metre in the new SI system was defined to be equal to 1,650,763.73 wavelengths of the orange-red emission line in the electromagnetic spectrum of the krypton-86 atom in a vacuum. This definition was replaced in 1983 by defining the metre as the distance travelled by light in vacuum during a specific time interval. Interferometry is still fundamental in establishing the calibration chain in length measurement.
Interferometry is used in the calibration of slip gauges (called gauge blocks in the US) and in coordinate-measuring machines. It is also used in the testing of optical components.[13]
Radio interferometry[edit]
Main article: Astronomical interferometer
The Very Large Array, an interferometric array formed from many smaller telescopes, like many larger radio telescopes.
In 1946, a technique called astronomical interferometry was developed. Astronomical radio interferometers usually consist either of arrays of parabolic dishes or two-dimensional arrays of omni-directional antennas. All of the telescopes in the array are widely separated and are usually connected together using coaxial cable, waveguide, optical fiber, or other type of transmission line. Interferometry increases the total signal collected, but its primary purpose is to vastly increase the resolution through a process called Aperture synthesis. This technique works by superposing (interfering) the signal waves from the different telescopes on the principle that waves that coincide with the same phase will add to each other while two waves that have opposite phases will cancel each other out. This creates a combined telescope that is equivalent in resolution (though not in sensitivity) to a single antenna whose diameter is equal to the spacing of the antennas farthest apart in the array.
Acoustic interferometry[edit]
An acoustic interferometer is an instrument for measuring the physical characteristics of sound waves in a gas or liquid, such velocity, wavelength, absorption, or impedance. A vibrating crystal creates ultrasonic waves that are radiated into the medium. The waves strike a reflector placed parallel to the crystal, reflected back to the source and measured.
See also[edit]
Active noise control
Beat (acoustics)
Coherence (physics)
Diffraction
Haidinger fringes
Interference lithography
Interference visibility
Interferometer
Lloyd's Mirror
Moiré pattern
Multipath interference
Newton's rings
Optical path length
Thin-film interference
Rayleigh roughness criterion
Upfade
References[edit]
^ On the mechanism of the eye / by Thomas Young.; Young, Thomas; University College, London Library Services (1801). Young, Thomas, 1773-1829. University College London (UCL) UCL Library Services. London : printed by W. Bulmer and Co., Cleveland Row, St. James's.
^ Jones, Peter Ward (2001). Oxford University Press. Oxford Music Online. Oxford University Press. doi:10.1093/gmo/9781561592630.article.20622.
^ Kipnis, Nahum (1991). History of the Principle of Interference of Light. doi:10.1007/978-3-0348-8652-9. ISBN 978-3-0348-9717-4.
^ Ockenga, Wymke. Phase contrast. Leika Science Lab, 09 June 2011. "If two waves interfere, the amplitude of the resulting light wave will be equal to the vector sum of the amplitudes of the two interfering waves."
^ Steel, W. H. (1986). Interferometry. Cambridge: Cambridge University Press. ISBN 0-521-31162-4.
^ Pfleegor, R. L.; Mandel, L. (1967). "Interference of independent photon beams". Phys. Rev. 159 (5): 1084–1088. Bibcode:1967PhRv..159.1084P. doi:10.1103/physrev.159.1084.
^ Patel, R.; Achamfuo-Yeboah, S.; Light R.; Clark M. (2014). "Widefield two laser interferometry". Optics Express. 22 (22): 27094–27101. Bibcode:2014OExpr..2227094P. doi:10.1364/OE.22.027094. PMID 25401860.
^ a b Born, Max; Wolf, Emil (1999). Principles of Optics. Cambridge: Cambridge University Press. ISBN 0-521-64222-1.
^ Feynman R, Leighton R, and Sands M., The Feynman Lectures Website, September 2013."The Feynman Lectures on Physics, Volume III" (online edition)
^ Bach, Roger; Pope, Damian; Liou, Sy-Hwang; Batelaan, Herman (2013-03-13). "Controlled double-slit electron diffraction". New Journal of Physics. IOP Publishing. 15 (3): 033018. arXiv:1210.6243. doi:10.1088/1367-2630/15/3/033018. ISSN 1367-2630. S2CID 832961.
^ Levitin, Daniel J. (2006). This is Your Brain on Music: The Science of a Human Obsession. Dutton. p. 22. ISBN 978-0525949695.
^ Greene, Brian (1999). The Elegant Universe: Superstrings, Hidden Dimensions, and the Quest for the Ultimate Theory. New York: W.W. Norton. pp. 97–109. ISBN 978-0-393-04688-5.
^ RS Longhurst, Geometrical and Physical Optics, 1968, Longmans, London.
External links[edit]
Look up interference in Wiktionary, the free dictionary.
Wikimedia Commons has media related to Interference.
Easy JavaScript Simulation Model of One Dimensional Wave Interference
Expressions of position and fringe spacing
Java simulation of interference of water waves 1
Java simulation of interference of water waves 2
Flash animations demonstrating interference Archived 2009-06-24 at the Wayback Machine
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3: Interference - Physics LibreTexts
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The most certain indication of a wave is interference. This wave characteristic is most prominent when the wave interacts with an object that is not large compared with the wavelength. Interference is observed for water waves, sound waves, light waves, and, in fact, all types of waves.
3.1: Prelude to InterferenceIf you have ever looked at the reds, blues, and greens in a sunlit soap bubble and wondered how straw-colored soapy water could produce them, you have hit upon one of the many phenomena that can only be explained by the wave character of light. The same is true for the colors seen in an oil slick or in the light reflected from a DVD. These and other interesting phenomena cannot be explained fully by geometric optics. In these cases, light interacts with objects and exhibits wave characteristics.3.2: Young's Double-Slit InterferenceYoung’s double-slit experiment gave definitive proof of the wave character of light. An interference pattern is obtained by the superposition of light from two slits. When light passes through narrow slits, the slits act as sources of coherent waves and light spreads out as semicircular waves. Pure constructive interference occurs where the waves are crest to crest or trough to trough. Pure destructive interference occurs where they are crest to trough.3.3: Mathematics of InterferenceIn double-slit diffraction, constructive interference occurs when d sin θ = mλ (for m=0,±1,±2,±3…), where d is the distance between the slits, θ is the angle relative to the incident direction, and m is the order of the interference. Destructive interference occurs when \(d \space sin \space \theta = (m + \frac{1}{2}) \lambda\), for m = 0,±1,±2,±3,…3.4: Multiple-Slit InterferenceAnalyzing the interference of light passing through two slits lays out the theoretical framework of interference and gives us a historical insight into Thomas Young’s experiments. Much of the modern-day application of slit interference uses not just two slits but many, approaching infinity for practical purposes. We start the analysis of multiple-slit interference by taking the results from our analysis of the double slit (N = 2) and extending it to configurations with numbers of slits.3.5: Interference in Thin FilmsWhen light reflects from a medium having an index of refraction greater than that of the medium in which it is traveling, a 180° phase change (or a λ/2 shift) occurs. Thin-film interference occurs between the light reflected from the top and bottom surfaces of a film. In addition to the path length difference, there can be a phase change.3.6: The Michelson InterferometerThe Michelson interferometer (invented by the American physicist Albert A. Michelson, 1852–1931) is a precision instrument that produces interference fringes by splitting a light beam into two parts and then recombining them after they have traveled different optical paths.3.A: Interference (Answers)3.E: Interference (Exercises)3.S: Interference (Summary)
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2.S: Geometric Optics and Image Formation (Summary)
3.1: Prelude to Interference
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INTERFERENCE definition | Cambridge English Dictionary
INTERFERENCE definition | Cambridge English Dictionary
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Meaning of interference in English
interferencenoun [ U ] us
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/ˌɪn.t̬ɚˈfɪr.əns/ uk
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/ˌɪn.təˈfɪə.rəns/
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C1 an occasion when someone tries to interfere in a situation: She seems to regard any advice or help from me as interference. The government's interference in the strike has been widely criticized.
C2 noise or other electronic signals that stop you from getting good pictures or sound on a television or radio
More examplesFewer examplesThe political subtext of her novel is a criticism of government interference in individual lives.In the end he moved to another part of the country to escape his mother's continual interference in his private life.They dreamed of a new world order, composed of co-operating independent nation states, free from outside interference.Now can I please get on with the job, without any more interference from you?I'm sorry if he sees it as interference - we were only trying to be helpful.
SMART Vocabulary: related words and phrases
Getting involved for one's own benefit or against others' will
a piece/slice of the action idiom
act
action
bandwagon
be in bed with idiom
bed
get
get in on something
get/muscle in on the act idiom
have a finger in the pie idiom
horn
horn in
interfere
intrude
intrusion
jump/climb/get on the bandwagon idiom
non-interference
snoot
stick your snoot in/into (something) idiom
See more results »
You can also find related words, phrases, and synonyms in the topics:
Communications - general words
Idiom
run interference
(Definition of interference from the Cambridge Advanced Learner's Dictionary & Thesaurus © Cambridge University Press)
interference | Intermediate English
interferencenoun [ U ] us
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/ˌɪn·tərˈfɪər·əns/
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On the radio, television, or telephone, interference is noise, lines, etc., that prevent a clear sound or picture from being received.
physics Interference between two waves happens when they have the same frequency and produce a force that is either stronger or weaker than one wave alone.
In sports, interference is an action that is against the rules which prevents an opposing player from completing a play.
(Definition of interference from the Cambridge Academic Content Dictionary © Cambridge University Press)
Examples of interference
interference
They want to work together on those problems, without interference of outside militia.
From OregonLive.com
Word is out around the league about the interference in football operations.
From cleveland.com
It's pretty violent: there's no penalty for pass interference or late hits, and it's no fun unless you're hurting someone on every play.
From The Verge
Defensive pass interference is called approximately seven million times more than offensive pass interference (rough estimate).
From ESPN
It's been a ridiculous government interference on family issues.
From CNN
Their interference in the market prevents small companies from competing with large ones.
From CNN
We are not their family members and do not know what repercussions they could face by our individual interference.
From NPR
It does not seem to help answer why, when single photons pass through the grid, they still show interference.
From Phys.Org
I get to be a teacher without any interference.
From CNN
In licensed spectrum, interference disputes tend to get resolved without such loud, public fights.
From The Hill
Prosecutors are concentrating on proving that their case against him has been weakened by interference with witnesses.
From Reuters
We believe this is the first time such a quantum two-photon interference based on a parametric effect (an active process) has been demonstrated.
From Phys.Org
It just requires placing one fiber in the gas flow stream -- even in locations with strong magnetic interference.
From Phys.Org
These examples are from corpora and from sources on the web. Any opinions in the examples do not represent the opinion of the Cambridge Dictionary editors or of Cambridge University Press or its licensors.
Collocations with interference
interference
These are words often used in combination with interference. Click on a collocation to see more examples of it.
arbitrary interferenceIn these treaties, privacy is recognized as a form of autonomy-a way to ensure protection from ' 'arbitrary interference' '1 by the state or other entities.
From the Cambridge English Corpus
bureaucratic interferenceThis is a quite monstrous case of bureaucratic interference.
From the Hansard archive
Example from the Hansard archive. Contains Parliamentary information licensed under the Open Parliament Licence v3.0
constant interferenceBut this coming and going, this constant pinpricking, this constant interference without any consecutive thought and philosophy behind it, is not something to take lightly.
From the Hansard archive
Example from the Hansard archive. Contains Parliamentary information licensed under the Open Parliament Licence v3.0
These examples are from corpora and from sources on the web. Any opinions in the examples do not represent the opinion of the Cambridge Dictionary editors or of Cambridge University Press or its licensors.
See all collocations with interference
What is the pronunciation of interference?
C1,C2
Translations of interference
in Chinese (Traditional)
干涉,干預, (雜訊或其他電子訊號對電視或收音機的)干擾…
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in Chinese (Simplified)
干涉,干预, (噪声或其他电子信号对电视或收音机的)干扰…
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in Spanish
intromisión, injerencia, interferencias…
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in Portuguese
intromissão, interferência, intrometimento [masculine]…
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in more languages
in Marathi
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in Turkish
in French
in Catalan
in Dutch
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in Hindi
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in Danish
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in German
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हस्तक्षेप, ढवळाढवळ, गोंगाट…
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干渉, 混信, 干渉(かんしょう)…
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müdahale, burnunu sokma, karışma…
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intrusion [feminine], ingérence [feminine], interférence [feminine]…
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ingerència, intromissió, interferència…
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inmenging, storing…
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யாராவது ஒரு சூழ்நிலையில் தலையிட முயற்சிக்கும் ஒரு சந்தர்ப்பம், தொலைக்காட்சி அல்லது வானொலியில் நல்ல படங்கள் அல்லது ஒலியைப் பெறுவதைத் தடுக்கும் சத்தம் அல்லது பிற மின்னணு சமிக்ஞைகள்…
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(एक व्यक्ति के द्वारा किसी परिस्थिति में) हस्तक्षेप, टेलीविज़न या रेडियो पर अच्छी तस्वीरें या आवाज़ को बाधित करने वाले शोर या इलेक्ट्रॉनिक संकेत…
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હસ્તક્ષેપ, રુકાવટ, અવરોધ…
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indblanding, forstyrrelse…
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inblandning, störningar…
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masuk campur, gangguan…
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die Einmischung, die Störung…
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innblanding [masculine], forstyrrelse [masculine], interferens [masculine]…
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مداخلت, رکاوٹ, ٹیلی ویژن کے پردہ پر پیدا ہونے والی مداخلت…
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втручання, перешкоди…
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вмешательство, помехи…
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జోక్యం/ ఎవరైనా ఒక పరిస్థితిలో జోక్యం చేసుకోవడానికి ప్రయత్నించిన ఒక సందర్భం, టెలివిజన్ లేదా రేడియోలో నుంచి మంచి చిత్రాలు లేదా ధ్వని పొందకుండా మిమ్మల్ని ఆపే శబ్దం లేదా ఇతర ఎలక్ట్రానిక్ సిగ్నల్స్…
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تَدخّل, تَشويش…
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হস্তক্ষেপ করা, আওয়াজ বা অন্যান্য ইলেকট্রনিক সংকেত যা আপনাকে টেলিভিশন বা রেডিওতে ভাল ছবি বা শব্দ পেতে বাধা দেয়…
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zasahování, rušení, interference…
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turut campur, gangguan…
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สิ่งรบกวน, เสียงรบกวน…
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sự can thiệp, sự nhiễu…
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ingerencja, zakłócenia, mieszanie się…
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간섭, 방해…
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interferenza, ingerenza, intromissione…
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interfamily
interfere
interfere with something
interfered
interference
interfering
interferometer
BETA
interferometric
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interferometry
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destructive interference
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