Deriving Wien's Displacement Law from Planck's Law

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Homework Help Overview

The problem involves deriving Wien's displacement law from Planck's law, specifically establishing a relationship between temperature and the wavelength at which the spectral radiance is maximized, denoted as λmax. The original poster attempts to differentiate Planck's radiation law and analyze the resulting equation to demonstrate that Tλmax is a constant.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss differentiating Planck's law and setting the derivative to zero to find λmax. There are attempts to solve a transcendental equation numerically and questions about the implications of certain solutions, particularly regarding the physical meaning of the results.

Discussion Status

Some participants have offered numerical methods for solving the equation, including graphing and iterative techniques. There is recognition that the equation is transcendental and that multiple approaches may yield different insights. However, there is no explicit consensus on the best method or final outcome.

Contextual Notes

Participants note that certain constants in the equations are fixed, and there is discussion about the validity of solutions that yield zero, which raises questions about the physical interpretation of the results. The context of homework constraints is implied, as participants navigate through problem-solving strategies without providing direct solutions.

gnome
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Basically this problem is to derive Wien's displacement law from Planck's law.
Specifically:
a) Show that there is a general relationship between temperature and λmax stating that Tλmax = constant
and
b) Obtain a numerical value for this constant
[Hint: Start with Planck's radiation law and note that the slope of u(λ,T) is zero when λ = λmax ]

So I obediently try to differentiate u(λ, T) with respect to λ:

I'll let C1 = 8Πhc and C2 = hc/(kBT)

[tex]u(\lambda, T) = {C_1}\lambda^{-5} \left( e^\frac{C_2}{\lambda} - 1 \right)^{-1}[/tex]

[tex]\frac{\partial u}{\partial \lambda} = <br /> C_1 \left((\lambda^{-5})(-1)({e^{\frac{C_2}{\lambda}} - 1)^{-2}({e^\frac{C_2}{\lambda}})(-\frac{C_2}{\lambda^2}) + (e^{\frac{C_2}{\lambda}} - 1)^{-1}(-5)\lambda^{-6}\right) = 0[/tex]

I divide through by C1 & get

[tex]\frac{C_2e^\frac{C_2}{\lambda}}{\lambda^7({e^\frac{C_2}{\lambda}} -1)^2} - \frac{5}{\lambda^6({e^\frac{C_2}{\lambda}} -1)} = 0[/tex]

[tex]\frac{C_2{e^\frac{C_2}{\lambda}} - 5\lambda({e^\frac{C_2}{\lambda}} - 1)}{\lambda^7({e^\frac{C_2}{\lambda}} -1)^2} = 0[/tex]

[tex]C_2{e^\frac{C_2}{\lambda}} - 5\lambda{e^\frac{C_2}{\lambda}} + 5\lambda = 0[/tex]

[tex]let x = \frac{C_2}{\lambda} = \frac{hc}{{k_B}T\lambda}[/tex]

[tex]x{\lambda}e^x - 5{\lambda}e^x + 5{\lambda} = 0[/tex]

[tex]x = 5 - \frac{5}{e^x} = 5(1 - e^{-x})[/tex]

Now I substitute back for x = hc/(kT&lambda;) and get:

[tex]\frac{hc}{{k_B}T{\lambda}} = 5(1 - {e^\frac{-hc}{{k_B}T{\lambda}}})[/tex]

Oy!

This, amazingly, is exactly the expression I'm supposed to end up with (for part a), according to the answer in the book.

But how does this show that
[tex]T\lambda = constant[/tex]

and how do I solve for this constant?
 
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Well, this is kind of cheesy but:

You've got x = 5(1-e-x)

So plug that into a graphing calculator

(y = x-5(1-e-x), find x where y = 0)

Then you can write &lambda;T = hc/(kx), plugging in that value for x to find the value of the constant.

I think there is a better way to find that answer, but I'm not a mathematician and I don't remember it. Do you think that's good enough?
 
The equation is transcendental. You have no choice but to solve it numerically.

As for how it's constant, the entire right hand of the equation is a constant and all but T and [itex]\lambda[/itex] are constants on the left.

cookiemonster
 
Yes, thanks, I did finally realize that everything but
T and lambda are constant so T*lambda must be constant.

But when I solve with the calculator
x = 5(1-e^(-x))
it gives me x=0
which, come to think of it, seems perfectly correct.

Except, it makes no sense, because how can it be that
[tex]\frac{hc}{{k_B}T{\lambda}} = 0[/tex]
?
 
It can't! That's why you have to discard that solution. It's impossible to get [itex]\frac{hc}{{k_B}T{\lambda}} = 0[/itex] because hc clearly is not zero. There is, however, another solution.

Try plotting y = x and y = 5(1-e^(-x)) on the same screen and find where the two intersect.

cookiemonster
 
Originally posted by cookiemonster
The equation is transcendental. You have no choice but to solve it numerically.

As for how it's constant, the entire right hand of the equation is a constant and all but T and [itex]\lambda[/itex] are constants on the left.

cookiemonster

Oh, right. I guess I'm not as cheesy as I thought. What a shame, I really like cheese.
 
That works -- after a bit of trial and error I get x = 4.965 as a pretty good approximation. That will let me solve for T&lambda;

Is that the "usual" technique for solving equations of this form?

How would you solve it if you didn't have a graphing device?
 
I'd probably use bisection.

I'd guess that it lies between 4 and 5, test if the function y = 5(1-e^(-x)) - x crosses the x-axis between these points. y(4) is positive and y(5) is negative. Try y(4.5). If it's positive (it is), then we have a new lower bound, since the function crosses between 4.5 and 5. So try 4.75. You get the idea.

cookiemonster
 
Thanks, but I like your graph trick better. :wink:

Hope I remember it the next time a problem like this comes up.

PS:
James, if you graph
(y = x-5(1-e^(-x)), find x where y = 0)
on your calculator, you get (0,0).
(At least, that's all I get on mine.)
 
Last edited:
  • #10
To solve this equation you could use an itterative method. You first assume the exponential term is small so that
[itex] \frac{hc}{\lambda_mk_BT}=5[/itex]
Then you put that in as the argument of your exponent to get the next itteration of
[itex] \frac{hc}{\lambda_mk_BT}=5(1-e^{-5})[/itex]
and continue this to get the root to desired accuracy.
 
  • #11
Super!

It seems to take just a few iterations to get a good result, with very little thinking involved. What could be better?

Thanks.
 
  • #12
Originally posted by gnome
Thanks, but I like your graph trick better. :wink:

Hope I remember it the next time a problem like this comes up.

PS:
James, if you graph
(y = x-5(1-e^(-x)), find x where y = 0)
on your calculator, you get (0,0).
(At least, that's all I get on mine.)

Really? I've got zero crossings at the origin and at x = 4.9651142317
(please forgive the obscene # of decimal places; I've got a root finder on my calculator (it probably uses Newton-Raphson or some other iterative method to find the root)). The function looks kind of like a v tilted to the right.

Anyway, none of that's important now since you solved it already. I hope I didn't add confusion.
 
  • #13
Not at all, James. Your suggestions are always appreciated. How were you to know that I have a crappy calculator?
 

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