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In Fig. 35-45, a broad beam of light of wavelength 620 nm is sent directly downward through the top plate of a pair of glass plates touching at the left end. The air between the plates acts as a thin film, and an interference pattern can be seen from above the plates. Initially, a dark fringe lies at the left end, a bright fringe lies at the right end, and nine dark fringes lie between those two end fringes. The plates are then very gradually squeezed together at a constant rate to decrease the angle between them. As a result, the fringe at the right side changes between being bright to being dark every 15.0 s.

(a) At what rate is the spacing between the plates at the right end being changed?

(b) By how much has the spacing there changed when both left and right ends have a dark fringe and there are five dark fringes between them?

Short Answer

Expert verified

(a) The rate of change of this spacing is 10.33nm/s.

(b) The change in the spacing is 1085nm.

Step by step solution

01

Introduction

Wavelength is defined as the distance between successive crests of a wave, especially points in a sound wave or electromagnetic wave.

02

The rate at which the spacing between the plates at the right end being changed

(a)

Here initially there are 9 dark fringes between two ends.

Therefore we should have LR=m+12λ2n

Here n=1,m=9 (since 9th dark fringe)

Wave length λ=620nm

LR=9+12620nm21=2945

But in 15 s every bright fringe is changing to dark fringe.

So after 15 s the 9th dark fringe is changing to 9th bright fringe.

Therefore for bright fringe,

LR'=mλ2n=9620nm21=2790

Therefore changing in the width of the left edge is ΔLR=LR-LR'

=2745nm - 2790nm= 155nm

This change takes place in Δt=15s

The rate of change of this spacing is

ΔLτΔt155nm15s=10.33nm/s

Hence, the rate of change of this spacing is 10.33nm/s.

03

Step 3: The change in spacing when both left and right ends have a dark fringe

(b)

Here there are 5 dark fringes between left and right ends and each end have dark fringes. Therefore there are 7 dark fringes.

Therefore m=6

role="math" localid="1663148654843" LR'=6λ2n=620nm21=1860nm

Change in the spacing is

LR-LR'=2945nm - 1860nm= 1085nm

Hence, the change in the spacing is 1085nm.

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Most popular questions from this chapter

Transmission through thin layers. In Fig. 35-43, light is incident perpendicularly on a thin layer of material 2 that lies between (thicker) materials 1 and 3. (The rays are tilted only for clarity.) Part of the light ends up in material 3 as rayr3(the light does not reflect inside material 2) andr4(the light reflects twice inside material 2). The waves ofr3and r4interfere, and here we consider the type of interference to be either maximum (max) or minimum (min). For this situation, each problem in Table 35-3 refers to the indexes of refraction n1,n2and n3the type of interference, the thin-layer thickness Lin nanometers, and the wavelength λin nanometers of the light as measured in air. Whereλis missing, give the wavelength that is in the visible range. Where Lis missing, give the second least thickness or the third least thickness as indicated.

In Fig. 35-37, two isotropic point sources S1 and S2 emit identical light waves in phase at wavelengthλ. The sources lie at separation on an x axis, and a light detector is moved in a circle of large radius around the midpoint between them. It detects 30points of zero intensity, including two on the xaxis, one of them to the left of the sources and the other to the right of the sources. What is the value of dλ?

Transmission through thin layers. In Fig. 35-43, light is incident perpendicularly on a thin layer of material 2 that lies between (thicker) materials 1 and 3. (The rays are tilted only for clarity.) Part of the light ends up in material 3 as ray r3(the light does not reflect inside material 2) and r4(the light reflects twice inside material 2). The waves of r3andr4interfere, and here we consider the type of interference to be either maximum (max) or minimum (min). For this situation, each problem in Table 35-3 refers to the indexes of refraction n1,n2and n3the type of interference, the thin-layer thickness Lin nanometers, and the wavelength λin nanometers of the light as measured in air. Where λis missing, give the wavelength that is in the visible range. Where Lis missing, give the second least thickness or the third least thickness as indicated.

In Fig. 35-23, three pulses of light— a, b, and c—of the same wavelength are sent through layers of plastic having the given indexes of refraction and along the paths indicated. Rank the pulses according to their travel time through the plastic layers, greatest first.

A thin flake of mica (n = 1.58) is used to cover one slit of a double-slit interference arrangement. The central point on the viewing screen is now occupied by what had been the seventh bright side fringe (m = 7). If λ=550nm , what is the thickness of the mica?

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