Basic Bibliography: Program 1

Output 1

Basic Bibliography: Program 2

Output 2

Basic Bibliography: Program 3

Output 3

Basic Bibliography: Program 4

Output 4

Basic Bibliography: Program 5

\documentclass{book}
\usepackage{hyperref}
\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{graphicx}

\title{Introduction to Physics}
\author{}
\date{}

\begin{document}
	
	\maketitle
	
	\tableofcontents
	\newpage
	
	\chapter{Classical Mechanics}
	\section{Newton's Laws of Motion}
	\subsection{First Law}
	An object at rest stays at rest, and an object in motion stays in motion unless acted upon by a net external force.
	
	\subsection{Second Law}
	The acceleration of an object is directly proportional to the net force acting on it and inversely proportional to its mass.
	\begin{equation}
		F = ma
	\end{equation}
	
	\subsubsection{Example}
	If a force of 10 N acts on a 2 kg mass, the acceleration can be calculated as:
	\[
	a = \frac{F}{m} = \frac{10 \, \text{N}}{2 \, \text{kg}} = 5 \, \text{m/s}^2
	\]
	
	\section{Energy Conservation}
	The total mechanical energy in a closed system remains constant.
	
	\subsection{Kinetic Energy}
	The kinetic energy of an object is given by:
	\begin{equation}
		KE = \frac{1}{2}mv^2
	\end{equation}
	
	\chapter{Thermodynamics}
	\section{Laws of Thermodynamics}
	\subsection{Zeroth Law}
	If two systems are each in thermal equilibrium with a third system, then they are in thermal equilibrium with each other.
	
	\subsection{First Law}
	Energy cannot be created or destroyed, only transformed.
	\begin{equation}
		\Delta U = Q - W
	\end{equation}
	
	\chapter{Electromagnetism}
	\section{Electrostatics}
	\subsection{Coulomb's Law}
	The force between two charges is given by:
	\begin{equation}
		F = k \frac{|q_1 q_2|}{r^2}
	\end{equation}
	
	\subsection{Electric Field}
	The electric field \( E \) due to a point charge is defined as:
	\begin{equation}
		E = k \frac{|q|}{r^2}
	\end{equation}
	
	\chapter{Modern Physics}
	\section{Quantum Mechanics}
	\subsection{Wave-Particle Duality}
	Light exhibits both wave-like and particle-like properties.
	
	\subsection{Uncertainty Principle}
	The position and momentum of a particle cannot both be precisely measured at the same time.
	
	\section{References}
	\begin{thebibliography}{99}
		\bibitem{ref1} Halliday, D., Resnick, R., \& Walker, J. (2013). \textit{Fundamentals of Physics}. Wiley. \url{https://www.wiley.com/en-us/Fundamentals+of+Physics%2C+10th+Edition-p-9781119495267}
		\bibitem{ref2} Young, H. D., \& Freedman, R. A. (2014). \textit{University Physics}. Pearson. \url{https://www.pearson.com/store/p/university-physics/P100000934291}
		\bibitem{ref3} Feynman, R. P., Leighton, R., \& Sands, M. (1965). \textit{The Feynman Lectures on Physics}. Addison-Wesley. \url{https://www.feynmanlectures.caltech.edu}
	\end{thebibliography}
	
\end{document}

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