Phy5645/UV catastrophe problem2: Difference between revisions

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(Submitted by Team 4-Yuhui Zhang)  
(Submitted by Team 4-Yuhui Zhang)  
Try to use Boltzman-Maxwell statistics to deduce Plank Formula. (We have to consider quantum energy spectrum as Plank did.)
Try to use Boltzman-Maxwell statistics to deduce Plank Formula. (We have to consider quantum energy spectrum as Plank did.)


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</math>
</math>


So, the average particle number in  
So, the average particle number in <math>
 
<math>
h\upsilon  
h\upsilon  
</math> energy state is <math>
</math> energy state is <math>
\frac{1}{{e^{\frac{{h\upsilon }}{{kT}}}  - 1}}
\frac{1}{{e^{\frac{{h\upsilon }}{{kT}}}  - 1}}
</math>. (This is just the result of Bose-Einstein statistics.)
</math>. (This is just the result of Bose-Einstein statistics.)
so:
so:


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</math>,  
</math>,  


this reflect the phenomenon of black body irradiation, which is called Plank Formula.
this reflects the phenomenon of black body irradiation, which is called Plank Formula.

Latest revision as of 15:55, 30 November 2009

(Submitted by Team 4-Yuhui Zhang)

Try to use Boltzman-Maxwell statistics to deduce Plank Formula. (We have to consider quantum energy spectrum as Plank did.)

If the energy spectrum is: , , , ...

Then use Boltzman-Maxwell statistics:

So, the average particle number in energy state is . (This is just the result of Bose-Einstein statistics.)

so:

,

this reflects the phenomenon of black body irradiation, which is called Plank Formula.