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Experiment 2: the index of refraction of air, Introduction, Procedure 1 – PASCO OS-9257A PRECISION INTERFEROMETER User Manual

Page 17: Where l

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012-07137A

Precision Interferometer

Experiment 2: The Index of Refraction of Air

EQUIPMENT NEEDED:

– Basic Interferometer (OS-9255A)
– Laser (OS-9171)
– Laser Alignment Bench (OS-9172)
– Interferometer Accessories (OS-9256A)

Rotational pointer, Vacuum cell, Vacuum pump

Introduction

In the Michelson interferometer, the characteristics of the

fringe pattern depend on the phase relationships between

the two interfering beams. There are two ways to change

the phase relationships. One way is to change the distance

traveled by one or both beams (by moving the movable

mirror, for example). Another way is to change the

medium through which one or both of the beams pass.

Either method will influence the interference pattern. In

this experiment you will use the second method to

measure the index of refraction for air.
For light of a specific frequency, the wavelength l varies

according to the formula:

l = l

o

/n;

where l

o

is the wavelength of the light in a vacuum, and

n is the index of refraction for the material in which the

light is propagating. For reasonably low pressures, the

index of refraction for a gas varies linearly with the gas

pressure. Of course for a vacuum, where the pressure is

zero, the index of refraction is exactly 1. A graph of

index of refraction versus pressure for a gas is shown in

Figure 2.1. By experimentally determining the slope, the

index of refraction of air can be determined at various

pressures.

Procedure

1.

Align the laser and interferometer in the Michelson mode. See Setup and Operation.

2.

Place the rotational pointer between the movable mirror and the beam-splitter (see Figure 2.2).

Attach the vacuum cell to its magnetic backing and push the air hose of the vacuum pump over the

air outlet hole of the cell. Adjust the alignment of the fixed mirror as needed so the center of the

interference pattern is clearly visible on the viewing screen. (The fringe pattern will be somewhat

distorted by irregularities in the glass end-plates of the vacuum cell. This is not a problem.)

3.

For accurate measurements, the end-plates of the vacuum cell must be perpendicular to the laser

beam. Rotate the cell and observe the fringes. Based on your observations, how can you be sure

that the vacuum cell is properly aligned?

2

1

0

0

Index of Refraction (n)

Ž

Gas Pressure (cm Hg)

Ž

Figure 2.1. Index of Refraction versus Gas

Pressure

OS-9255A

PRECISION

INTERFEROMETER

-5

0

5

10

15

25

30

ADJUSTABLE MIRROR

MICHELSON, TWYMAN-GREEN

BEAM SPLITTER

MICHELSON

COMPENSA

TO

R

MICHELSON

18 mm FL

LENS

VIEWING SCREEN

MICHELSON, TWYMAN-GREEN

1 div = 1 MICRON

Vacuum Cell

Air Outlet

Figure 2.2. Equipment Setup

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