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[QUE/TH-08008] TH-PROBLEM

Node id: 5219page

For a system, as in $Q[2]$, undergoing a process from state 1
to state 2 at constant pressure and temperature, show that the
maximum ``non'' $PdV$ work out put is given by
\begin{eqnarray}
|A_{TP}| \le G_1-G_2 &\qquad G=\text{Gibbs function}&
\end{eqnarray}

AK-47's picture 22-01-23 18:01:29 n

[NOTES/EM-02015] Proof of curl free nature of \(\vec E\)

Node id: 5960page


Starting from Coulomb's law a proof is given that the electric field of a system of point charges obeys the Maxwell's equation.
\[\nabla \times \vec E =0\]

AK-47's picture 23-10-12 19:10:59 n

[2019EM/HMW-04]

Node id: 5366page

Electrodynamics                                               March 26, 2019
                                                 Tutorial-IV

  1. A uniform magnetic field $\vec{B}$ fills a cylindrical volume of radius $R$ and a metal rod of length $L$ is placed in it as shown in the figure.If the magnitude $B$ is changing at the rate $\frac{dB}{dt}$ show that the emf that is produced by the changing magnetic field and that acts between the ends of the rod is given by $${\cal E} = \frac{dB}{dt}\frac{L}{2}\sqrt{R^2-\frac{L^2}{2}}$$ 
  • Two identical coils each having radius $R$ and $n$- turns are kept parallel and with a distance $d$ between the two.
    1. Find an expression for the magnetic field at a point on the common axis of the coils and at a distance $x$ from the mid-point between the coils.
    2. Show that if the separation of the coils is equal to $R$, the first and the second derivatives of $B$ w.r.t. $x$ vanish at the mid point. This produces nearly constant magnetic field near the mid point, WHY?
    3. For $R=5.0$cm, $I=50$amp,and 300 turn coils, plot the magnetic field as a function of $x$ in the range $x=-5$cm to $x=5$cm.
    .
  • A wooden cylinder of mass $m=0.5$kg, radius $R=3$cm, length $\ell=10$cm, is placed on an inclined plane. It has 10 turns of wire wrapped around it longitudinally so that the plane of the wire contains the axis of the cylinder and is parallel to the inclined plane, see . Assuming no friction, what is the current that will prevent the cylinder from rolling down the inclined plane in presence of a uniform magnetic field of 0.5T?. Describe what happens if the block is a rectangular instead of a cylindrical one? What will be the current that will prevent the block from moving down the plane?
  • A square wire of length $L$, mass $m$, and resistance $R$ slides without friction down parallel rails of negligible resistance, as in \Figref{em-fig-015}. The rails are connected to each other at the bottom by a resistanceless rail parallel to the wire so that the wire and rails form a closed rectangular conducting loop. The plane of the rails makes an angle $\theta$ with the horizontal, and a uniform vertical magnetic field $\vec{B}$ exists in the region.
    1. Show that the wire acquires a steady state velocity of magnitude $$v= \frac{mgR\sin\theta}{B^2 L^2\cos^2\theta}$$
    2. Show that the above result is consistent with conservation of energy.
    3. What changes will be necessary in the above results, if the direction of magnetic field is reversed?
  • A cylindrical shell of radius $R$, height $h$, and carrying a uniform surface charge density $\sigma$, rotates about its own axis with angular velocity $\omega$. Compute the magnetic field produced by the cylinder at a point on the axis
AK-47's picture 22-04-25 19:04:47 n

[2018EM/QUIZ-03]

Node id: 5430page
AK-47's picture 22-06-21 06:06:57 n

[1998TH/LNP-12]-Work in Thermodynamics

Node id: 5583page
AK-47's picture 22-07-17 11:07:46 n

Finite Dimensional Vector Spaces --- Notes for Lectures and Problems [VS-MIXED-LOT]

Node id: 4692collection

 

AK-47's picture 23-09-15 12:09:11 n

[NOTES/EM-03010]-Electric Field Inside an Empty Cavity in a Conductor

Node id: 5648page

Maxwell's equation, \(\text{curl}\vec{E}=0\), is used to prove that the electric field inside an empty cavity in a conductor is zero.

AK-47's picture 22-08-11 12:08:11 n

[NOTES/QM-18002] Perturbative Solution of Differential equation

Node id: 4829page

$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ 
$\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$
$\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$
$\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$
$\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$
$\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
$\newcommand{\ket}[1]{\langle #1\rangle}$
qm-lec-18002

AK-47's picture 22-03-04 22:03:27 y

[NOTES/EM-07001]-Electric Current

Node id: 5707page

The current density and its relation with the current in a circuit is explained.


 

AK-47's picture 24-03-02 07:03:06 n

[QUE/SM-09001] SM-PROBLEM

Node id: 5087page

Even though there is high density of electrons in a metal ( a large fraction are free to move, the mean free paths are long, of the order of $10^{_6}$m. Give a qualitative argument for such a long mean free path. Will the mean free path increase or decrease with the increase of temperature?

AK-47's picture 22-01-24 13:01:55 n

[QUE/TH-02002] TH-PROBLEM

Node id: 5193page

For a gas satisfying van de Waals equation
$$
\left(P+{a\over v^2}\right) (v-b) = R\theta
$$
show that the critical temperature $\theta_c$, critical pressure
$P_c$, and the critical volume are given by

$\theta_c =
{8a\over27Rb}~,~~P_c={a\over27b^2}~,~~v_c=3b\,.\,.$

 

AK-47's picture 22-01-16 17:01:29 n

[2019CM/Final-Part-B]

Node id: 5339page

       

                                                Classical Mechanics                      July 4, 2009                                                                                                                           


End Semester Examination::PART-B

Instruction:-Attempt any four questions. 

  1. Consider a particle of mass $m$ moving in two dimensions in a potential The equation of motion for small oscillations are given to be                                                   [4+4+4] \begin{eqnarray} m\ddot{x} =k \big( 5x + y \big)\\ m\ddot{y} =k \big( x + 5 y \big)\nonumber \end{eqnarray}
    1. Find the normal frequencies of vibration of normal modes.
    2. Obtain expressions for \(x,y\) in terms of normal coordinates.
    3. Write the Lagrangian \[{\Lsc} = \frac{m}{2}(\dot{x}^2+m\dot{y}^2) - \frac{k}{2}\big(5x^2+2xy +5y^2\big)\] in terms of normal coordinates and verify that it takes the form \[{\Lsc} = \frac{1}{2}(\dot{Q}_1^2+\dot{Q}_2^2) - \frac{1}{2}(\omega_1^2Q_1^2+\omega_2^2Q_2^2)\]
  2. Consider pendulum with a spring shown in figure. It oscillates in vertical plane like any simple pendulum.
    1. What is number of degrees of freedom? Which generalized coordinates will you use?[2+2+8]
    2. Write the Lagrangian for the system.
  3. A missile is fired from the origin with initial velocity \(u\) and at an angle \(\alpha\) with horizontal.                                                                                               [3+3+3+3] 
    1. Write the Lagrangian for the missile.
    2. Is there a cyclic coordinate? Which one? What is the conserved quantity associated with it?
    3. Is there any other conserved quantity?
    4. Using conserved quantities you have found, briefly indicate how a full solution can be obtained.
    • Show that                                                                                       [3+3+6] \begin{equation*} Q=-p ,\qquad P=q + Ap^2 \end{equation*} (where A is any constant) is a canonical transformation,
      1. [(i)] by evaluating \([Q,P]_{q,p}\)
      2. [(ii)] by expressing \(pdq-PdQ\) as an exact differential \(dF(q,Q)\). Hence find the type one generating function of the transformation. To do this, you must first use the transformation to express \(p,P\) in terms of \(q,Q\).
    • Use the relation \(F_2=F_1+PQ\) to find the type 2 generating function \(F_2(q,P)\),and check your result by showing that \(F_2\) indeed generates the transformation.
  4. Consider the motion in a spherically symmetric potential $$ V(r) = - V_0 \left( {3 R\over r } + {R^3\over r^3} \right)$$ If orbital angular momentum of the particle is given by $l^2 = 10 m V_0 R^2$, and answer the following questions.
    1. Plot the effective potential as a function of $r$                                       [3]
    2. What should be the energy of the particle so that it may move in a circular orbit? How many circular orbits are possible? Find the radius of the stable orbit.     [3+3+3]
AK-47's picture 22-04-03 11:04:23 n

[2008EM/HMW-06]

Node id: 5403page
AK-47's picture 22-05-13 17:05:01 n

[LECS/QM-24003] Fermi GOlden Rule

Node id: 5468page
AK-47's picture 22-06-05 15:06:21 n

[1998TH/LNP-05] Lecture -5 Zeroth Law and Temperature

Node id: 5547page
AK-47's picture 22-07-08 07:07:13 n

[NOTES/ME-06004]-Stable, Unstable and Neutral Equilibria

Node id: 5680page
AK-47's picture 22-08-14 18:08:39 n

[MOB/QM-08002]

Node id: 4897page
AK-47's picture 22-03-07 09:03:23 y

[NOTES/EM-10003]-Examples of flow of energy

Node id: 5736page

Energy stored in capacitor while it is being charged and the heat produced in a current carrying resistor are explained in terms of flow of energy as given by the Poynting theorem.

AK-47's picture 22-08-28 10:08:18 n

[ NOTES/QCQI-01003] Trace and Partial Trace

Node id: 5020page
AK-47's picture 22-04-08 13:04:46 y

[QUE/TH-06004] TH-PROBLEM

Node id: 5163page

CD consists of two adiabatic processes and an isobaric process and an isochoric process of a box of volume V containing perfect gas as shown below

AB is constant volume BC and DA and adiabatic and CD is at constant volume.
Calculate the efficiency of the engine in terms of $V_A$, $V_B$, $V_C$ and the ratio of specific heats $\gamma$.

Remark : The efficency depends upon the equation of state of the system. had we used some other system ( like a gas of photons, whose equation of state, we will discuss soon) the answer is different). Only for carnot's cycle, the efficency is independent of the system.)

 

AK-47's picture 22-01-13 18:01:39 n

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