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[PNET/CV-05001] Existence of derivative, analytic property, singular points etc.

Node id: 5630page

The attached file is a collection of questions taken from NET/CSIR/GATE/JEST and other similar examinations
The questions concern:

  • Existence of derivative
  • Computation of limit
  • Checking if a function is analytic or not
  • Properties of real and imaginary parts of an analytic function
  • Finding real part (or imaginary part) if the other one is given.

KEY CONCEPTS

Existence of derivative, Analytic function, Limit, Cauchy Riemann equations,

 

 

AK-47's picture 22-08-06 21:08:34 n

[NOTES/QM-16010] Classical Motion in Three Dimensions Spherically symmetric potentials

Node id: 4802page

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qm-lec-16010

AK-47's picture 22-03-07 20:03:42 y

[NOTES/ME-08009]-How good is a frame as inertial frames

Node id: 5693page
AK-47's picture 22-08-16 13:08:02 n

[LECS/EM-10003] -- Energy Conservation ---- Poynting Theorem

Node id: 5749page

Using time dependent Maxwell's equations and considering a charge distribution moving under influence of the electric and magnetic fields, an equation for rate of change of mechanical work done on the charges is derived, see EQ12. This equation is local conservation law of energy. It says that the rate of the sum of change energy of e.m. fields and work done in a volume \(V\) equals to the flow of energy through the boundary of the volume \(V\). The flow though the boundary is given by the Poynting vector \(\vec{S}\) defined in EQ10.

AK-47's picture 22-09-10 16:09:51 n

[QUE/SM-02001] SM-PROBLEM

Node id: 5054page

Consider a 2 dimensional phase space ( $q,p$) with a rectangular region defined by four corners as shown.
If the region ABCD is the phase space region at time time t = 0 , find the region $A'B'C'D'$ at time t given the Hamiltonian is
$$ H\,=\,\frac{p^2}{2m}\,-\, m a q $$
and explicitly verify that the area is constant. Take the coordinates of A,B,C and D as $(q_A,p_A)\,,\,(q_B,p_A)\,,\,(q_B,p_C)$ and $(q_A,p_C)$ respectively

AK-47's picture 22-01-14 10:01:53 n

[QUE/TH-06006] TH-PROBLEM

Node id: 5179page

Consider a paramagnetic system, with variables magnetization $M$, the magnetic field $B$ and absolute temperature $T$. ( We assume it's dependence on pressure as negligible). The equation of state is ( which will be obtained from statistical mechanics later in the course) is
$$ M\,=\,C\frac{B}{T}, $$
where $C$ is a constant ( referred to as the Curie constant, who had experimentally obtained this relation.
The system's internal energy is ( for a one-dimensional system)
$$ U\,=\,-MB.$$
The work done on the system by external surrounding is $-MdB$

(a) Write the expression for $DQ$ in terms of $dM$ and $dB$

(b) Write the equation for entropy change $dS$ in terms of $dM$ and $dB$

(c) Obtain the entropy $S$

AK-47's picture 22-01-14 09:01:31 n

[2013EM/HMW-09]

Node id: 5383page
AK-47's picture 22-04-17 10:04:00 n

[2003SM/LNP-08] Lecture-08--Basic assumptions of statistical mechanics

Node id: 5533page

Statistical mechanics is based on the fundamental assumption that all microstates of an isolated system are equally

AK-47's picture 22-07-06 07:07:13 n

[1998TH/LNP-27]-TdS equations

Node id: 5597page
AK-47's picture 22-07-17 18:07:27 n

[NOTES/QM-10003] A Summary of Coordinate and Momentum Representation

Node id: 4721page


A tabular comparison of  coordinate and momentum representations is presented.

AK-47's picture 24-06-22 06:06:37 n

[NOTES/QM-20005] Identical Particles in Quantum Mechanics

Node id: 4848page

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$\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
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qm-lec-20005

AK-47's picture 22-03-05 08:03:58 y

[LECS/EM-07004]-Vector Potential

Node id: 5721page
AK-47's picture 22-08-23 17:08:45 n

21Th-ProbSet3

Node id: 4995page
AK-47's picture 21-12-04 07:12:21 n

[QUE/SM-05001] SM-PROBLEM Fermi Dirac Distribution

Node id: 5146page

Show from calculating
$$ \frac{\Delta S}{\Delta E}\,=\,\frac{1}{T}\,=\,k\beta$$
for the case of Fermi-Dirac distribution,
$$ \Omega_{FD}\,=\,\Pi_{i=1}^\infty\left({}^{g_i}C_{N_i}\right) $$
[ notation as used in the class ]. Also for the case of equilibrium we have
$$ N_i\,=\,\frac{g_i}{e^{\alpha+\beta\epsilon_i}\,+\,1} $$
Hint: Consider changes only in two levels say with energies $\epsilon _1$ and $\epsilon_2$. Then argue that the result so obtained is independent of the choice of levels]

AK-47's picture 22-01-07 09:01:25 n

[QUE/TH-06012] TH-PROBLEM

Node id: 5207page

A cannot engine is operated between two heat reservoir of 400 K and 300 K

  • [(a)] If the engine receives 122 Cal from reservoir at 400 K in each cycle, how many calories does it reject to the reservoir at 300 K.
  • [(b)] If the engine is operated as a refrigerator and receives 1200 Cal from reservoir at 300 K, how many Calories does it deliver at 400 K
  • [(c)] How much work is done by the engine in each case.
AK-47's picture 22-01-23 10:01:49 n

[2019EM/QUIZ-01]

Node id: 5354page

Electrodynamics                                                  April 3, 2022
                                            Quiz-I

 Two grounded infinite conducting planes are kept along the XZ and Y Z planes, see Fig.2. A charge q is placed at (4,3) find the force acting on the charge q.

AK-47's picture 22-04-04 13:04:32 n

[2018EM/Final-A]

Node id: 5418page
AK-47's picture 22-06-21 08:06:30 n

[QUE/EM-01016] --- EM-PROBLEM

Node id: 5494page

An electron moving with speed of $5.0\times 10^8$cm/sec is shot parallel to an electric field strength of $1.0\times 10^3 $nt/coul arranged so as to retard its motion.

  • How far will the electron travel in the field before coming (momentarily) to rest ?
  • how much time will elapse?
  • If the electric field ends abruptly after $0.8$ cm, what fraction of its initial energy will the electron loose in traversing the field?
AK-47's picture 22-06-18 12:06:07 n

[2003SM/HMW-03]

Node id: 5561page
AK-47's picture 22-07-10 06:07:16 n

[NOTES/EM-03001]-Computation of Electric Potential

Node id: 5634page

The curl free nature of the electric field in electrostatics implies existence of a potential,\(\phi(\vec(r))\), from which the electric field can be derived as \(\vec{E}=-\nabla \phi\). The potential at a point is just the work done in moving a unit point charge from infinity to its current position.

AK-47's picture 23-10-17 14:10:31 n

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