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Ch. 35 - Diffraction
Giancoli Douglas - Physics for Scientists and Engineers 5th edition
Giancoli Douglas5th editionPhysics for Scientists and EngineersISBN: 9780137488179Non è quello che usi tu?Cambia libro di testo
Capitolo 34, Problema 22

(a) Derive an expression for the intensity in the interference pattern for three equally spaced slits. Express in terms of δ = 2πd sin θ / λ where d is the distance between adjacent slits and assume the slit width D ≈ λ.
(b) Show that there is only one secondary maximum between principal peaks.

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Start by recalling the general expression for the intensity in an interference pattern for multiple slits. The intensity is proportional to the square of the amplitude of the resultant wave. For three equally spaced slits, the resultant amplitude is the sum of the contributions from each slit, taking into account the phase difference δ between adjacent slits.
Write the expression for the resultant amplitude: \( A_{total} = A_1 + A_2 e^{i\delta} + A_3 e^{i2\delta} \), where \( A_1, A_2, A_3 \) are the amplitudes of the waves from the three slits, and \( \delta = \frac{2\pi d \sin \theta}{\lambda} \) is the phase difference between adjacent slits.
Simplify the expression for the resultant amplitude using the geometric series formula. Since the amplitudes are equal (\( A_1 = A_2 = A_3 = A \)), the resultant amplitude becomes \( A_{total} = A (1 + e^{i\delta} + e^{i2\delta}) \). Use the formula for the sum of a finite geometric series to simplify this further.
The intensity is proportional to the square of the magnitude of the resultant amplitude. Compute \( |A_{total}|^2 \) by taking the magnitude squared of the simplified amplitude expression. This will give the intensity as a function of \( \delta \): \( I(\delta) \propto |1 + e^{i\delta} + e^{i2\delta}|^2 \). Expand and simplify this expression to derive the final formula for intensity.
To show that there is only one secondary maximum between principal peaks, analyze the conditions for maxima. Principal maxima occur when \( \delta = 2n\pi \) (where \( n \) is an integer). For secondary maxima, find the values of \( \delta \) that satisfy the derivative of the intensity function \( I(\delta) \) being zero, excluding the principal maxima. Solve this condition and verify that there is only one secondary maximum between two consecutive principal maxima.

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Interference Pattern

An interference pattern is created when waves from multiple sources overlap, leading to regions of constructive and destructive interference. In the case of slits, the path difference between waves emanating from different slits determines whether they reinforce or cancel each other. The resulting pattern consists of bright and dark fringes, which can be mathematically described using the phase difference between the waves.
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Path Difference and Phase Difference

The path difference is the difference in distance traveled by waves from different slits to a point on the screen. It is related to the phase difference, which is the fraction of a wavelength by which one wave lags behind another. The expression δ = 2πd sin θ / λ quantifies this relationship, where d is the distance between slits, θ is the angle of observation, and λ is the wavelength of the light used.
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Secondary Maxima

Secondary maxima are the smaller peaks in an interference pattern that occur between the principal maxima. For three equally spaced slits, the conditions for these secondary maxima can be derived from the interference equations. The analysis shows that there is only one secondary maximum between each pair of principal peaks, which is a result of the specific phase relationships established by the three slits.
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