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Interference is the addition (
Superposition principle) of two or more
waves that results in a new wave pattern.
As most commonly used, the term
interference usually refers to the interaction of waves which are correlated or Coherence (physics) with each other, either because they come from the same source or because they have the same or nearly the same
frequency.
Two non-monochromatic waves are only fully
coherent with each other if they both have exactly the same range of
wavelengths and the same
phase (waves) differences at each of the constituent wavelengths.
The total phase difference is derived from the sum of both the path difference and the initial phase difference (if the waves are generated from 2 or more different sources). It can then be concluded whether the waves reaching a point are
in phase(constructive interference) or
out of phase (destructive interference).
Theory
The principle of superposition of waves states that the resultant displacement at a point is equal to the sum of the displacements of different waves at that point. If a
Crest (physics) of a wave meets a crest of another wave at the same point then the crests interfere
constructively and the resultant wave
amplitude is greater. If a crest of a wave meets a trough of another wave then they interfere
destructively, and the overall amplitude is decreased.
This form of interference can occur whenever a wave can propagate from a source to a destination by two or more paths of different length. Two or more sources can only be used to produce interference when there is a fixed phase relation between them, but in this case the interference generated is the same as with a single source; see Huygens principle.
Experiments
Thomas Young (scientist)'s double-slit experiment showed interference phenomena where two beams of light which are coherent interfere to produce a pattern.
The beams of light both have the same wavelength range and at the center of the interference pattern. They have the same phase (waves)s at each wavelength, as they both come from the same source.
Interference patterns
For two coherent sources, the spacial separation between sources is half the wavelength times the number of nodal lines
Light from any source can be used to obtain interference patterns, for example, Newton's rings can be produced with
sunlight. However, in general
white light is less suited for producing clear interference patterns, as it is a mix of a full spectrum of colours, that each have different spacing of the interference fringes. Sodium light is close to monochromatic and is thus more suitable for producing interference patterns. The most suitable is laser light because it is almost perfectly monochromatic.
Constructive and destructive interference
. Bright bands are the result of
constructive interference while the dark bands are the result of
destructive interference.
Consider two waves that are in phase,with amplitudes A_1 and A_2. Their troughs and peaks line up and the resultant wave will have amplitude A = A_1 + A_2. This is known as
constructive interference.
If the two waves are
pi radians, or 180°, out of phase, then one wave's crests will coincide with another wave's troughs and so will tend to cancel out. The resultant amplitude is A = ].
{||-|
combined
waveform| colspan="2" rowspan="3" | |-|
wave 1|-|
wave 2|-|
|
Two waves in phase|
Two waves 180° out
of phase|}
General Quantum Interference
.
If a system is in state \psi its
wavefunction is described in Dirac or
bra-ket notation as:
] Basis (linear algebra)) and the \psi_i are the probability amplitude coefficients, which are complex numbers.
The probability of observing the system making a transition or quantum leap from state \psi to a new state \phi is the square of the modulus of the scalar product or
inner product of the two states:
prob(\psi \Rightarrow \phi) = ] so that \psi_i^* = \lang \psi|i \rang etc.
Now let's consider the situation classically and imagine that the system transited from |\psi \rang to |\phi \rang via an intermediate state |i\rang. Then we would
classically expect the probability of the two-step transition to be the sum of all the possible intermediate steps. So we would have
prob(\psi \Rightarrow \phi) = \sum_i prob(\psi \Rightarrow i \Rightarrow \phi) = \sum_i |\lang \psi |i \rang|^2|\lang i|\phi \rang|^2 = \sum_i|\psi_i|^2 |\phi_i|^2
The classical and quantum derivations for the transition probability differ by the presence, in the quantum case, of the extra terms \sum_{ij;i \ne j} \psi^*_i \psi_j \phi^*_j\phi_i; these extra quantum terms represent
interference between the different i \ne j intermediate "alternatives". These are consequently known as the quantum interference terms, or cross terms. This is a purely quantum effect and is a consequence of the non-additivity of the probabilities of quantum alternatives.
The interference terms vanish, via the mechanism of
quantum decoherence, if the intermediate state ], Decoherence and the transition from quantum to classical,
Physics Today, 44, pp 36-44 (1991)Wojciech H. Zurek, Decoherence, einselection, and the quantum origins of the classical,
Reviews of Modern Physics 2003, 75, 715 or .
Examples
A conceptually simple case of interference is a small (compared to wavelength) source - say, a small array of regularly spaced small sources (see diffraction grating).
Consider the case of a flat boundary (say, between two media with different or simply a flat mirror, onto which the plane wave is incident at some angle. In this case of continuous distribution of sources, constructive interference will only be in
specular direction - the direction at which angle with the normal is exactly the same as the angle of incidence. Thus, this results in the law of reflection which is simply the result of constructive interference of a plane wave on a plane surface.
See also
References
External links
- Expressions of position and fringe spacing
- Java demonstration of interference
- Java simulation of interference of water waves 1
- Java simulation of interference of water waves 2
- Flash animations demonstrating interference
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