GREPhysics.NET
GR | # Login | Register
   
  GR9277 #96
Problem
GREPhysics.NET Official Solution    Alternate Solutions
\prob{96}
9277_96

A gas-filled cell of length 5 cm is inserted in one arm of a Michelson interferometer, as shown in the figure above. The interferometer is illuminated by light of wavelength 500 nm. As the gas is evacuated from the cell, 40 fringes cross a point in the field of view. The refractive index of this gas is most nearly


  1. 1.02
  2. 1.002
  3. 1.0002
  4. 1.00002
  5. 0.98

Optics}Interferometer

An (effective) path change of produces a fringe shift. Thus, the interferometer formula is similar to the interference formula at normal incident, .

Thus, . Thus, , as in choice (C).

See GR0177.100 on the same site for more info.

See below for user comments and alternate solutions! See below for user comments and alternate solutions!
Alternate Solutions
faham
2006-10-26 22:33:35
Let:

* N be the number of full wavelengths across the gas-filled cell

* N' be the number of full wavelengths across the cell when it's empty

* lambda_0 is the wavelength of light in vaccuum

* lambda is the wavelength of light in a material of index of refraction n

* d is the length of the cell (5 cm)

* M is the number of fringes seen on the screen

N = d/lambda_0

N' = d/lambda

Now, we know that lambda = lambda_0/n, so

N' = d*n/lambda_0

Be aware that the light goes IN and back OUT of the cell (it's an interferometer!), so

N' - N = M/2

Again, even though you see 40 fringes, it's 20 wavelengths that N gets shifted by.

N' - N = M/2 = d*n/lambda_0 - d/lambda_0

M/2 = d/lambda_0*(n-1)

Solving for n:

n = M*lambda_0/(2*d) + 1

n = (40)*(500nm)/(2*5cm) + 1

n = 1.0002

So the answer is C
Alternate Solution - Unverified
Comments
Imperate
2008-10-17 07:03:31
The key here is the optical path difference, given that the mirrors dont move etc everything else is constant except the bit of path going through the gas chamber. The optical path length of this section is 0.1n [metres]. For a maxima the total path difference of the total rays must be a integer multiple of the wavelength m \lambda .Therefore one obtains the expression  \Delta D= constant-0.1n=m \lambda . Multiply both sides by 10, and one can see that if the optical n changes by 10 \lambda a new fringe will appear. Given that 40 fringes went past this implies  \Delta n=500E-9*10*40=0.0002 .
The refractive index of air is 1 therefore n=1+0.0002=1.00002 . Choice C
neon37
2008-10-29 14:26:51
refractive index of air is not 1, its 1.0002926 (http://en.wikipedia.org/wiki/List_of_indices_of_refraction) refractive index of vacuum is 1. The whole setup has to in vacuum. Btw, you have an extra 0 in your answer.
NEC
dumbguy
2007-10-10 18:01:07
What happened to the nanometers? Why did we choose to just leave them out?NEC
faham
2006-10-26 22:33:35
Let:

* N be the number of full wavelengths across the gas-filled cell

* N' be the number of full wavelengths across the cell when it's empty

* lambda_0 is the wavelength of light in vaccuum

* lambda is the wavelength of light in a material of index of refraction n

* d is the length of the cell (5 cm)

* M is the number of fringes seen on the screen

N = d/lambda_0

N' = d/lambda

Now, we know that lambda = lambda_0/n, so

N' = d*n/lambda_0

Be aware that the light goes IN and back OUT of the cell (it's an interferometer!), so

N' - N = M/2

Again, even though you see 40 fringes, it's 20 wavelengths that N gets shifted by.

N' - N = M/2 = d*n/lambda_0 - d/lambda_0

M/2 = d/lambda_0*(n-1)

Solving for n:

n = M*lambda_0/(2*d) + 1

n = (40)*(500nm)/(2*5cm) + 1

n = 1.0002

So the answer is C
caffeinated
2008-04-08 12:56:36
Why do you use lambda for N' when N' is the empty cell and lambda is lambda in the gas? I don't understand. Why wouldn't you use lambda-0 for N'?
Alternate Solution - Unverified
astro_allison
2005-11-26 22:02:48
\lambda?
astro_allison
2005-11-26 22:17:25
wouldn't n = \frac{m \lambda}{2d} + 1 ?
yosun
2005-11-26 23:06:44
astro_allison: thanks for the typo-alerts; both typos have been corrected.
Fixed Typos!

Post A Comment!
Username:
Password:
Click here to register.
This comment is best classified as a: (mouseover)
 
Mouseover the respective type above for an explanation of each type.

Bare Basic LaTeX Rosetta Stone

LaTeX syntax supported through dollar sign wrappers $, ex., $\alpha^2_0$ produces .
type this... to get...
$\int_0^\infty$
$\partial$
$\Rightarrow$
$\ddot{x},\dot{x}$
$\sqrt{z}$
$\langle my \rangle$
$\left( abacadabra \right)_{me}$
$\vec{E}$
$\frac{a}{b}$
 
The Sidebar Chatbox...
Scroll to see it, or resize your browser to ignore it...


ShoutMix chat widget

Millions of Books, Journals and Articles

Find Scholarships Today!

Search FastWeb see Green!

SL Button 125

Free 3D Virtual World. Largest User-Created Fantasy World. Don't Play, Experience. Join Now!

Bored, got time to kill, and want to earn micro-cash by mindlessly clicking on links? Join CrownGPT. Click Offers. Click the Paid to Click button... then click to your heart's delight.

90% Off + FREE SHIPPING!

FREE 3D Virtual World Chat - Join Second Life Today!