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[PNET/CV-05001] Existence of derivative, analytic property, singular points etc.Node id: 5630pageThe 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,
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22-08-06 21:08:34 |
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[NOTES/QM-16010] Classical Motion in Three Dimensions Spherically symmetric potentialsNode id: 4802page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ qm-lec-16010
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22-03-07 20:03:42 |
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[NOTES/ME-08009]-How good is a frame as inertial framesNode id: 5693page |
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22-08-16 13:08:02 |
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[LECS/EM-10003] -- Energy Conservation ---- Poynting Theorem Node id: 5749pageUsing 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.
$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
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22-09-10 16:09:51 |
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[QUE/SM-02001] SM-PROBLEMNode id: 5054pageConsider 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
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22-01-14 10:01:53 |
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[QUE/TH-06006] TH-PROBLEMNode id: 5179pageConsider 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 $S$
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22-01-14 09:01:31 |
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[2013EM/HMW-09]Node id: 5383page |
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22-04-17 10:04:00 |
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[2003SM/LNP-08] Lecture-08--Basic assumptions of statistical mechanicsNode id: 5533pageStatistical mechanics is based on the fundamental assumption that all microstates of an isolated system are equally
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22-07-06 07:07:13 |
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[1998TH/LNP-27]-TdS equationsNode id: 5597page |
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22-07-17 18:07:27 |
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[NOTES/QM-10003] A Summary of Coordinate and Momentum RepresentationNode id: 4721page $\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}\newcommand{\matrixelement}[3] \langle#1|#2|#3\rangle} \newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}\newcommand{\dd}[2][]{\frac{d#1}{d#2}}\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ A tabular comparison of coordinate and momentum representations is presented.
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24-06-22 06:06:37 |
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[NOTES/QM-20005] Identical Particles in Quantum MechanicsNode id: 4848page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ $\newcommand{\ket}[1]{\langle #1\rangle}$ qm-lec-20005
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22-03-05 08:03:58 |
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[LECS/EM-07004]-Vector PotentialNode id: 5721page |
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22-08-23 17:08:45 |
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21Th-ProbSet3Node id: 4995page |
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21-12-04 07:12:21 |
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[QUE/SM-05001] SM-PROBLEM Fermi Dirac DistributionNode id: 5146pageShow 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]
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22-01-07 09:01:25 |
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[QUE/TH-06012] TH-PROBLEMNode id: 5207pageA 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.
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22-01-23 10:01:49 |
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[2019EM/QUIZ-01]Node id: 5354pageElectrodynamics 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.
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22-04-04 13:04:32 |
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[2018EM/Final-A]Node id: 5418page |
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22-06-21 08:06:30 |
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[QUE/EM-01016] --- EM-PROBLEMNode id: 5494pageAn 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?
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22-06-18 12:06:07 |
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[2003SM/HMW-03]Node id: 5561page |
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22-07-10 06:07:16 |
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[NOTES/EM-03001]-Computation of Electric PotentialNode id: 5634pageThe 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.
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23-10-17 14:10:31 |
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