From fd18bff4e44a5db95eb5a329b1a0550de4fa967e Mon Sep 17 00:00:00 2001 From: Abhishek Yadav <85741764+Abhishek8322@users.noreply.github.com> Date: Wed, 30 Jun 2021 12:13:56 +0530 Subject: [PATCH] Add files via upload --- me20b008.tex | 25 +++++++++++++++++++++++++ 1 file changed, 25 insertions(+) create mode 100644 me20b008.tex diff --git a/me20b008.tex b/me20b008.tex new file mode 100644 index 0000000..27c272b --- /dev/null +++ b/me20b008.tex @@ -0,0 +1,25 @@ + +\begin{document} +\section{Abhishek Yadav} +\subsection{Planck's Radiation Law} +\begin{equation} + \rho(\nu,T)={\frac{8 \pi h \nu^3}{c^3}} {\frac{1}{\exp_k^{\frac{h \nu}{k_BT}} - 1}} + \label{eqn:1} +\end{equation} +The Planck's Law describes the energy density of electromagnetic radiation emitted by a black body in thermal equilibrium at a given Temperature T, and there is no net flow of matter or energy between the body and its environment. +The equation~\ref{eqn:1} depicts mathematical form of the Plank's Law. \\ +Here \\ +$\rho$ - Energy Density \\ +$\nu$ - Frequency of radiation emitted \\ +$k_B$ - Boltzmann Constant \\ +k - Kaniadakis Parameter \\ +T - Temperature \\ +The equation shows the fequency dependency of the the energy density ~\cite{meb008}.The ~\ref{fig:me20b008} shows the graph of variation of energydensity vs frequency. +\begin{figure}[h] + \begin{center} + \includegraphics[width=200pt,height=200pt]{me20b008.eps} + \end{center} + \caption{Variation of energy density with the frequency, for the different values of Kaniadakis Parameter} + \label{fig:me20b008} +\end{figure} +