Module 5 : MODERN PHYSICS
Lecture 23 : Black Body Radiation
Black Body Radiation :
  The frequency $ \nu=\omega/2\pi$ is given by
  $\displaystyle \nu = \frac{c}{2L}\sqrt{n_x^2+n_y^2+n_z^2}$
For a given frequency, the equation above represents a sphere of radius $ R = 2L\nu/c$ in the three dimensional space of $ n_x, n_y$ and $ n_z$ and each value of $ \nu$ represents a distinct point in this space. Since $ n_x, n_y, n_z$ can only take integral values, the number of points per unit volume is one. If we treat $ \nu$ as a continuous variable, the number of modes for frequency less than some given $ \nu$ is given by
 
$\displaystyle N(\nu)$ $\displaystyle =$ $\displaystyle 2\times \frac{1}{8} \frac {4\pi R^3}{3}$
$\displaystyle =$ $\displaystyle \frac{8\pi V}{3 c^3}\nu^3$
  where $ V$ is the volume of the cavity. In the above, the factor of 1/8 comes because we are restricted to the positive octant as $ n_x, n_y, n_z$ can only be positive. The factor of 2 takes into account the fact that there are two transverse modes. The number of modes in the frequency interval $ \nu$ and $ \nu+d\nu$ is
 
$\displaystyle N(\nu)d\nu$ $\displaystyle =$ $\displaystyle N(\nu+d\nu)-N(\nu)$
$\displaystyle =$ $\displaystyle \frac{8\pi V}{3 c^3}[(\nu+d\nu)^3-\nu^3]$
$\displaystyle =$ $\displaystyle \frac{8\pi V}{c^3}\nu^2d\nu$
 

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