Blackbody Radiation
#Physics
When light is emitted from a hot body due to the thermal excitations wiggling charges in the object
Topics
$\displaystyle U=\frac{\pi ^{2}}{15(\hbar c)^{3}}V\tau ^{3}$
- Energy for a blackbody
$\displaystyle \sigma=\frac{4\pi ^{2}V\tau ^{3}}{45(\hbar c)^{3}}$
- Entropy for a blackbody
$\displaystyle N_{\gamma}=\frac{2}{\pi ^{2}}\left( \frac{\tau}{\hbar c} \right)^{3}V\zeta(3)\approx \frac{\sigma}{3.6}$
- Number of photons in a certain volume
- $\displaystyle \zeta$ is the Riemann Zeta function
$\displaystyle n_{D}=\left( \frac{6N}{\pi} \right)^{1/3}$
- Debye number
- Gives the max $\displaystyle k$ for $\displaystyle N$ particles
$\displaystyle U=3N\tau=\hbar v_{\text{sound}}\left( \frac{\pi}{L} \right)n$
- Energy for phonons
Applications
- Toaster
- Sun
- IR Thermometry
- Imaging
- CMB ($\displaystyle 2.7\mathrm{\text{ }K}^\circ$)
- Blackholes/Hawking Radiation
- Unruh Radiation
- Voltage/coment noise across resistor Johnson-Nyquist noise (1D bbody radiation)