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[LECS/EM-03002]-Examples of Computation of Electric PotentialNode id: 5652pageWe give details of computation of potential for the following examples.
1. Uniformly Charged Ring
2. Uniformly Charged Disc
3. Thin Spherical Shell
4. Uniformly Charged Solid Sphere
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24-03-30 05:03:22 |
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[NOTES/QM-18005]Born ApproximationNode id: 4833page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$
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qm-lec-18005
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22-03-03 22:03:07 |
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[NOTES/EM-07005]-Torque on a Current Carrying LoopNode id: 5710page
An expression for torque on a current carrying loop in magnetic field is obtained. It is shown that the torque is given by \(\vec{\tau}=\vec{m}\times\vec{B}\), where \(\vec{m}\) is the magnetic moment of the loop. For a planar loop\(|\vec{m}|=\) current \(\times\) area.
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24-03-05 09:03:22 |
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[QUE/SM-08003] SM-PROBLEMNode id: 5090pageConsider a photon gas in two dimensions at temperature T in area A. Find the energy density $u(\omega)$ as a function of temperature and various physical constants. Show that the total energy is proportional to $T^3$. ( you can assume that the internal degree of freedom is 1.
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22-01-09 20:01:35 |
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[QUE/TH-02005] TH-PROBLEMNode id: 5196pageA wire undergoes an infinitesimal change from an initial
equilibrium state to a final equilibrium state, show that the
change of tension is equal to
$$
d\mathcal{J} = -\alpha A Y d\theta + {AY\over L} ~dL
$$
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22-01-16 17:01:39 |
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[2019CM/QUIZ-03]Node id: 5342pageClassical Mechanics June 24, 2019
Quiz-III
- Define spherically symmetric potential. [4]
- Plot effective potential for isotropic oscillator potential \(V(r)=\frac{1}{2}m \omega^2r^2\). Find the radius of circular orbit(s). [6]
- Under a rotation of coordinate axes about \(\hat{n}=\frac{1}{\surd 3}(1,1,1)\) by an angle \(\pi/3\) what will be the vectors representing the new axes?
.
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22-04-01 13:04:09 |
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[2008EM/HMW-09]Node id: 5406page |
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22-05-10 20:05:42 |
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[LECS/QM-24001] An Overview of Approximation Methods for Time Dependent Schrodinger EquationNode id: 5474page |
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22-06-05 15:06:13 |
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[1998TH/LNP-08] Lecture -8 Pure SubstancesNode id: 5550page |
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22-07-08 07:07:52 |
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[STR/CV-05001]-Summary of Points to be RememberNode id: 5620page |
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22-08-06 14:08:09 |
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[NOTES/QM-16003] Solution of Radial Equation for a Constant PotentialNode id: 4782page |
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22-03-07 19:03:52 |
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[NOTES/ME-06007]-no titleNode id: 5684page |
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22-08-14 19:08:52 |
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[NOTES/EM-10007]-Time Varying Fields ,Ampere's LawNode id: 5740page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$
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We explain how Maxwell's addition of a displacement current in the fourth equation.
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23-03-03 20:03:30 |
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TESING NODE 5022 LATEX CODE Node id: 5025page |
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21-12-08 20:12:16 |
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[QUE/TH-07002] TH-PROBLEMNode id: 5166pageFind the specific heat $C_H$ of a substance at constant enthalpy and show that it is equal to
$$ C_H\,=\,\frac{C_p}{1\,-\,\frac{T}{V}\times\left(\frac{\partial V}{\partial T}\right)_p} $$
where we are using the standard notation.
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22-01-13 18:01:19 |
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[QUE/SM-05003] SM-PROBLEMNode id: 5224pageConsider free fermions at temperature $T\,=\,300^o$ K. The Fermi energy is $5$ electron volt. Give a qualitative argument why the specific heat for such a system is linearly proportional to the temperature.
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22-01-23 20:01:23 |
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[NOTES/EM-03013] Electrostatic Energy of NucleiNode id: 5966pageThe electromagnetic contribution to the difference in binding energies of mirror nuclei is computed. The numerical values are compared with the binding energy difference
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23-10-22 15:10:26 |
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[PSET/EM-02002]Node id: 5437page |
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22-05-26 18:05:21 |
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[2003SM/LNP-23] Lecture 23 --- Ideal Bose GasNode id: 5522page |
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22-07-04 10:07:38 |
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[1998TH/LNP-18]-Carnot CycleNode id: 5588page |
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22-07-17 18:07:31 |
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