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[2003SM/LNP-01] Lecture 01--Probability

Node id: 5524page

The basic notions of probability theory, simple events, sample space and ensemble, are introduced. The probability of compound events, independent events and joint and conditional probability are defined. Examples are given to illustrate the basic concepts.

AK-47's picture 22-07-03 23:07:09 n

[1998TH/LNP-19]-Carnot Heat Engine

Node id: 5589page
AK-47's picture 22-07-17 18:07:05 n

[NOTES/QM-09005] Schr\"{o}dinger Picture ---- Important Points

Node id: 4708page

The time evolution of a general quantum system is reviewed in an abstract setting. The eigen states of energy are seen to have all properties that make them qualify for being called stationary states.The stationary states have the property that all observable quantities remain constant in time.


AK-47's picture 24-03-24 05:03:08 n

[NOTES/ME-02002]-The SO(3) Group

Node id: 5657page
AK-47's picture 22-08-17 16:08:27 y

[NOTES/EM-07008]-Magnetic Vector Potential

Node id: 5713page

The vector potential is introduced using the Maxwell's equation \(\nabla \times \vec{B}=0\) and the equation \( \nabla \times \vec{B} = \mu_0 \vec{j}\) is derived. The expression for the magnetic field is obtained as volume integral, the Biot Savart law, is derived. The expressions for the magnetic field for the surface current and the line current are given.


 

AK-47's picture 23-03-03 20:03:21 n

[QUE/SM-08004] SM-PROBLEM

Node id: 5093page

Show that the number of photons in a cavity at temperature $T$ and having a unit volume is
$$ N\,=\, j \left(\frac{kT}{\hbar c}\right)^3 $$
where $j$ is a numerical constant.

Use the above result to show that the specific heat of a photon gas in proportional to $T^3$

AK-47's picture 22-01-09 20:01:49 n

[QUE/TH-02008] TH-PROBLEM

Node id: 5199page

An approximate equation of state of a real gas at moderate
pressures, devised to take into account of the finite size of the
molecules, is $P(v-b)=R\theta$, where $R$ and $b$ are constants.
Show that

\begin{equation*}
\beta = {1/\theta\over 1+bP/(R\theta)}~~,~~~~\chi =
{1/P\over1+bP/(R\theta)}
\end{equation*}

AK-47's picture 22-01-16 17:01:49 n

[2019CM/HMW-02]

Node id: 5345page

  Classical Mechanics                              June 1,2009

   Tutorial-II

 

  • For a pendulum with a light rod, as in Fig (a), and pendulum with spring Fig(b), assume that each system can move in all possible ways in space with a fixed point of suspension at the origin. Answer the following questions
    • Write the Lagrangian
    • Identify cyclic coordinates, conserved quantities, if any.
    • Obtain the Lagrangian in small amplitude approximation.
    • Obtain the normal coordinates and normal modes of vibration.
  • Set up the Lagrangian for double pendulum consisting of two masses $m_1$ and $m_2$ connected to light bars of lengths $L_1$ and $L_2$ as shown in figure of Double Pendulum.  Use the notation \[ M_2=\mu M_1, L_2=kL_1, g=\nu^2 L_1.\] Obtain the expressions for the following quantities in terms of \(\mu, k ,\nu\).
    • The equation which determines the normal frequencies.
    • Choose \(\mu=\frac{3}{4}, k=\frac{5}{7}\) and find the frequencies of normal modes of vibration.
    • Determine the matrix \(S\) relating the angles to the normal coordinates \begin{equation} \begin{pmatrix} \theta \phi \end{pmatrix} = S \begin{pmatrix}Q_1 Q_2 \end{pmatrix} \end{equation}
    • Verify that the Lagrangian in terms of the normal coordinates takes the form \begin{equation} L = \frac{1}{2}\dot{Q}_1^2 + \frac{1}{2}\dot{Q}_2^2 - \frac{1}{2}\omega_1^2Q_1^2 - \frac{1}{2}\omega_2^2Q_2^2 \end{equation}
  • Two systems are shown in {Springs123A}(a) and (b) below.In Fig (a) we have three masses connected to by two springs.The masses can move only along the line joining the three masses.In Fig (b) there are two masses connected by three springs and the system is kept on a smooth horizontal table. One end of each of the two outer springs is tied to fixed nails. The system can can move in all possible ways on the table.

     Set up the Lagrangian and obtain the frequencies of small oscillations.
AK-47's picture 22-04-03 11:04:03 n

[NOTES/EM-07004] Stokes Theorem

Node id: 6000page

Relationship between the normal to a surface and the orientation of its boundary curve, as they should appear in Stokes theorem are explained.


 

AK-47's picture 23-11-05 07:11:25 n

[2008EM/QUIZ-01A]

Node id: 5409page
AK-47's picture 22-05-11 07:05:55 n

[1998TH/LNP-11] Lecture -11 Work in Thermodynamics

Node id: 5553page
AK-47's picture 22-07-08 07:07:50 n

[ACQ/CV-05001] Understanding Relation Between Existence of Derivative and Being Analytic

Node id: 5623page
AK-47's picture 22-08-07 05:08:18 n

[NOTES/ME-08003]-Effect of Earth's Rotation --Centrifugal Force

Node id: 5687page
AK-47's picture 24-04-08 07:04:57 n

[NOTES/QM-25003] Charged Particle in E.M. Field

Node id: 4931page

$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ 
$\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$
$\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$
$\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$
$\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$
$\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
$\newcommand{\ket}[1]{\langle #1\rangle}$
qm-lec-25003

AK-47's picture 22-03-12 18:03:00 y

[NOTES/EM-10008]-Maxwell's Equations for Time Varying Fields and Ampere's Law

Node id: 5743page

Several concepts and results valid for static fields need revision when one is considering the situation of time varying fields. Some of these are discussed here


 

AK-47's picture 23-03-03 20:03:05 n

[NOTES/QCQI-03003] Density Matrix of Mixed State

Node id: 5028page
AK-47's picture 22-04-07 13:04:02 y

[QUE/TH-09001] TH-PROBLEM

Node id: 5169page

Consider the following expressions for entropy. Which ones can possibly be a fundamental equation and which ones violate one or more of postulates II,III and IV?

  • $S\,=\,K_1\left(NVU\right)^{1/3}$
  • $ S\,=\,K_2\left(\frac{NU}{V}\right)^{2/3} $
  • $ S\,=\,K_3\left(\frac{V^3}{NU}\right)$
  • $ S\,=\,N{\rm{\ln}}\left(\frac{UV}{N^2K_4}\right)$

$K_i$'s are positive constants so that dimensions match. $S,U,N,V $ are the entropy, internal energy, number of particles and volume respectively.

AK-47's picture 22-01-13 18:01:44 n

[QUE/SM-04026] SM-PROBLEM

Node id: 5227page

Consider a perfect gas having N particles obeying Maxwell- Boltzmann statistics and is in equilibrium at temperature $T$. Find the average of $\epsilon^r$ ( $r$ is a real number) where $\epsilon $ is the energy of a single particle.

AK-47's picture 22-01-23 20:01:26 n

[NOTES/EM-03020] Proof of Gauss Law from Maxwell's Equations

Node id: 5969page

A vector calculus proof of Gauss law is given starting from the Maxwell's equation \(\text{div} \vec E=\frac{\rho}{\epsilon_0}\)

AK-47's picture 23-10-22 21:10:11 n

[2013EM/HMW-03]

Node id: 5377page
AK-47's picture 22-04-17 09:04:54 n

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