How Do You Calculate the Thickness of a Soap Film for Constructive Interference?

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Homework Help Overview

The problem involves calculating the thickness of a soap film with a refractive index of 1.333, illuminated by white light at an angle of 45 degrees. The light produces two bright bands corresponding to specific wavelengths, leading to questions about the conditions for constructive and destructive interference.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the interpretation of bright bands and whether they indicate constructive or destructive interference. There is confusion regarding which wavelength to use and how to apply the interference equations correctly. Some participants question the definitions of variables and the implications of the angle of incidence versus the angle of refraction.

Discussion Status

The discussion is ongoing, with participants offering various interpretations of the interference conditions and the equations involved. Some guidance has been provided regarding the use of different wavelengths and the order of interference, but no consensus has been reached on the correct approach or assumptions.

Contextual Notes

Participants note potential confusion regarding the angles involved and the path differences in the film, as well as the implications of the refractive index on the calculations. The original poster expresses uncertainty about which wavelength to consider, highlighting the complexity of the problem.

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Homework Statement


a soap film of refractive index 1.333 is illuminated with white light at an angle of 45.the light refracted by it is examined and two bright bands are focussed corresponding to wavelengths 6.1 X 10 to the power -5 and 6.0 X 10 to the power -5.find thickness "t" of the film


Homework Equations



since it is given as destructive interference,formula will be

2 Xrefractive index(myu) X t Xcosr=n Xlamda

The Attempt at a Solution



2 X 1.333 X t X cos45=?

what is the wavelength i should take.there are two.its bit confusing for me...please help me...
 
Last edited:
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Why do bright bands lead you to think in terms of destructive interference? If two different wavelengths are bright under the same geometric conditions, then the thickness must be creating the same interference condition for both wavelengths.
 
so should i take lamda1 and lamda2,then is this is the formula
2 X mu X t Xcosr=n X lamda
or
2 X mu X t X cosr=(2n-1) X lamda/2
 
yamini said:
so should i take lamda1 and lamda2,then is this is the formula
2 X mu X t Xcosr=n X lamda
or
2 X mu X t X cosr=(2n-1) X lamda/2

I'm not sure what you mean by r, and I have never seen μ used for index of refraction, but if that is what you mean by mu, then it does come into play.

The optical path difference (number of wavelengths) between two rays incident at 45º needs to be determined. The rays change direction when entering the liquid, and there is a phase revesal at one surface (which one?) assuming air is on both sides of the film. It is not clear to me that you have the path difference correct in either equation. It appears you have not accounted for the extra path length in air while the one ray is in the liquid. I could be wrong and will look at it moe carefully if you tell me you think you have.
 
Last edited:
actually "r" here means the angle and "mu" is the refractive index as i attempted in the solution.as per given question refractive index is 1.333 and r=45.
 
yamini said:
actually "r" here means the angle and "mu" is the refractive index as i attempted in the solution.as per given question refractive index is 1.333 and r=45.

I don't think r is 45º. If the light is incident on the first surface at 45º then it is refracted to a new angle within the higher inex film. The light reflected at the first surface has a longer path length in air than the light that is reflected at the second surface. It is not apparent to me that you have accounted for that extra path length in air.

Draw your two parallel incident rays with a line perpendicular to these rays (which represents a wave front) that intersects the first point of contact with film and do the same at the exit point of the penetrating ray. The optical path difference from the entry front to the exit front is what determines the final phase difference between the rays.
 
You are considering the transmitted system (and not the reflected system), I presume. The condition for brightness in the transmitted system is the one you have written. You will get two values for ‘n’ on substituting the two given values of the wave length. What are you going to calculate?
If you are given that the angle of refraction is 45 degrees you can substitute it in the equation. If the given angle (45 degrees) is the angle of incidence, you will have to find cos r using the equation, refractive index = sini/sinr.
 
yamini said:

Homework Statement


a soap film of refractive index 1.333 is illuminated with white light at an angle of 45.the light refracted by it is examined and two bright bands are focussed corresponding to wavelengths 6.1 X 10 to the power -5 and 6.0 X 10 to the power -5.find thickness "t" of the film


Homework Equations



since it is given as destructive interference,formula will be

2 Xrefractive index(myu) X t Xcosr=n Xlamda

The Attempt at a Solution



2 X 1.333 X t X cos45=?

what is the wavelength i should take.there are two.its bit confusing for me...please help me...

Since you want to calculate the thickness ‘t’ of the film using the transmitted system, use the equation, 2 n t cosr = mλ where ‘n’ is the refractive index ‘m’ is the order of the interference band and ‘λ’ is the wave length.
The lower order (m) will be for the longer wave length (λ1 = 6.1×10^ –5 cm). Understand that the order ‘m’ for the longer wave length implies that the thickness of the film is such that there has to be a path difference of ‘m’ wave lengths of this light. The condition for constructive interference for the light of shorter wave length (λ2 = 6.0×10^ –5 cm) is established when the order increases by 1. Therefore, the order of the band produced by the shorter wave length light is (m+1).
So, you have, mλ1 = (m+1)λ2 from which m = λ2/( λ1– λ2) .
Now you have, 2 n t cosr = m λ1 and 2 n t cosr = (m+1)λ2. Use one of these equations to calculate the thickness ‘t’, substituting for n (= 1.333) and cos r.
Since the angle of incidence i = 45 degrees, the value of ‘r’ will wok out to very nearly 32 degrees using n = sini/sinr. Now, calculate 't'.
 

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