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Packages for Newbies --- Quantum Field Theory

Node id: 3918collection

Lectures

Problem Sessions

Problem Sessions will start appearing here in near future

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Planned course for Newbies

AK-47's picture 21-09-14 18:09:55 n

[2003SM/LNP-14] Lecture-14--Equipartition of Energy

Node id: 5539page

In this lecture we derive law of equipartition of energy under the assumption that the energy is quadratic function of some variable such as coordinates and momenta. The classical theory of specific heat of gases is given and the Einstein model of taking quantum corrections is briefly discussed. A comparison of the classical and quantum model with experiments is given.

AK-47's picture 22-07-07 07:07:20 n

[1998TH/LNP-34]-Applications of Kinetic Theory of Gases

Node id: 5603page
AK-47's picture 22-07-17 19:07:53 n

[NOTES/QM-11004] Time Reversal Symmetry

Node id: 4732page

Time reversal operation in quantum mechanics of one particle is discussed.

AK-47's picture 24-06-23 18:06:29 n

[NOTES/ME-02011]-no title

Node id: 5671page
AK-47's picture 22-08-14 10:08:37 y

[NOTES/EM-09006]-Faraday's Law and Maxwell's Second Equation

Node id: 5727page

The Maxwell's equations for static fields get modified by additional terms when the field vary with time slowly. These modifications are describe here.

AK-47's picture 22-08-24 16:08:31 n

21Th-ProbSet7

Node id: 5004page
AK-47's picture 21-11-29 19:11:38 n

[QUE/TH-01002] TH-PROBLEM

Node id: 5152page

A bimetallic strip of total thickness $x$ is straight at temperature $T$. What is the radius of curvature of the strip,
$R$, when it is heated to temperature $T + ∆T$ ? The coefficients of linear expansion of the two metals are $α_1$ and $α_2$ ,
respectively, with \(α_1 > α_2 \). Assume each metal has thickness \(x/2\), and that \(x << R.\)

AK-47's picture 22-01-13 18:01:05 n

[QUE/TH-07007] TH-PROBLEM

Node id: 5213page

 A mass $m$ of a liquid at a temperature $T_1$ is mixed with an
equal mass of the same liquid at a temperature $T_2$. The system is
thermally isolated. Show that the entropy change is given by
$$
2m\,C_p\,\ln\left({(T_1+T_2)/2\over\sqrt{T_1T_2}}\right)
$$
and prove that this is necessarily positive.

AK-47's picture 22-01-23 11:01:59 n

[NOTES/EM-01011] $\vec B$ vs $\vec H$ --- Naming convention.

Node id: 5953page

We will call \(\vec B\) field as magnetic field when no medium is present.\\ In presence of a magnetic medium, \(\vec B\) will be called magnetic flux density or  magnetic induction. The field \(vec H\) will called  magnetic intensity or magnetic field intensity

AK-47's picture 23-09-30 03:09:36 n

[2019EM/QUIZ-08]

Node id: 5360page

Electrodynamics                                                Apr 19, 2019
                                     Quiz-VIII

 

Question 1:
A student was asked to find the electric field inside
a uniformly polarized sphere. The following answer was received.

Sample Answer:


The answer to the above question as given in Griffiths is

\(\vec{E}=-\frac{\vec{P}}{3\epsilon_0}\)

  1. Give your comments why is this answer wrong?
  2. Give a counter example showing that the conclusion arrived by the student is incorrect.
  3. Give steps to derive the correct answer

Question 2:
Consider a parallel plate capacitor with plates having charges \(Q\) and \(-Q\). An insulating medium fills the region between the plates. Assuming that the linear dimensions of the plates are much larger than the separation between the plates, draw a diagram to show

  1. the distribution of free charges on the plates.
  2. distribution of the bound charges on the surface of the dielectric material.
  3. Use Gauss law to obtain \(\vec{D}\). Use your result for \(\vec{D}\) and obtain \(\vec{E}\), the potential difference between the plates and the capacitance.
AK-47's picture 22-04-04 17:04:06 n

[2018EM/HMW-03]

Node id: 5424page
AK-47's picture 22-06-21 08:06:16 n

[NOTES/EM-02005] Flux of $\bar{E}$ and Using Gauss law

Node id: 5577page

The flux of electric field is defined and As a simple example, the flux of the electric field due to a point charge at the center of a sphere is explicitly computed. Other cases are briefly mentioned an statement of Gauss law is given.

AK-47's picture 23-10-02 12:10:31 n

Quantum Mechanics --- Notes for Lectures and Problems [QM-MIXED-LOT]

Node id: 4671collection

NOTES FOR LECTURES

 

 


 TABLE OF CONTENTS


 

  • [QM-01] Classical Theories Revisited
  • [QM-02] A Quick Review of Vector Spaces 
  • [QM-03] Inner Product Spaces 
  • [QM-04]* Infinite Dimensional vector spaces
  • [QM-05] 30 years that shook Physics 
  • [QM-06] Postulates of Quantum Mechanics 
  • [QM-07] Canonical Quantization 
  • [QM-08] Eigenvalues Using Commutators 
  • [QM-09] Time Development
  • [QM-10] Coordinate and Momentum Representation
  • [QM-11] Time Dependent Schrodinger Equation
  • [[QM-12] Free Particle and Particle in Box
  • [QM-13] Energy Eigenvalue Problems in One Dimension
  • [QM-14] Reflection and Transmission
  • [QM-15] Problems in Two Dimensions
  • [QM-16] Spherically Symmetric Potential Problems
  • [QM-17] Angular Momentum in Quantum Mechanics
  • [QM-18] Scattering -- Three Dimensions
  • [QM-19] Method of Partial Waves
  • [QM-20] Spin and Identical Particles
  • [QM-21] Variation Method
  • [QM-22] WKB Approximation
  • [QM-23] Time Independent Perturbation Theory
  • [QM-24] Approximation Methods for Time Dependent Problems
  • [QM-25] Semi-Classical Theory of Radiation

 

 

QUESTIONS

AK-47's picture 22-05-30 11:05:24 n

[NOTES/EM-03004]-The Electric Stress Tensor

Node id: 5641page

An expression for the electric stress tensor is derived for a charge distribution in a volume \(V\). The surface integral of the stress  tensor gives the total electric force on the  charge in the volume \(V\).

AK-47's picture 23-10-17 14:10:45 n

[NOTES/QM-17004] Recurrence Relations for CG Coefficients

Node id: 4817page

$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ 
$\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$
$\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$
$\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$
$\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$
$\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
$\newcommand{\ket}[1]{\langle #1\rangle}$
qm-lec-17004

AK-47's picture 22-03-04 09:03:38 y

[NOTES/ME-14007]-Parallel Axes Theorem

Node id: 5701page
AK-47's picture 22-08-16 16:08:43 n

[NOTES/EM-12001]-Lorentz transformations

Node id: 5757page

The basic equations of Maxwell's theory are written down in relativistic notation. Using Lorentz transformations of the potentials, the expressions of the scalar and vector potentials of a point charge moving with a uniform velocity are obtained.


 

AK-47's picture 23-03-03 21:03:55 n

[QUE/SM-03005] --- SM-PROBLEM

Node id: 5069page

A system consists of three particles and each particle can exist in five possible states. Find the total number of microstates and the number of microstates that energy level has two particles assuming

  • the particles are non-identical
  • are identical bosons
  • are identical fermions.
AK-47's picture 22-01-09 20:01:30 n

[QUE/TH-13002] TH-PROBLEM

Node id: 5187page

a) An ion of mass m and electric charge e is moving in a dilute gas of molecules with which it collides. The mean time between collisions is $\tau$. Let there be a uniform electric field $E$ along the x-axis. Show that the mean distance travelled by the ion is
$$ \frac{Ee}{m}\tau^2$$
assuming the velocity of the ion is zero immediately after collision.

AK-47's picture 22-01-14 13:01:21 n

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