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[NOTES/EM-04002] Poisson Equation in Cylindrical coordinates$\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\PP}[2][]{\frac{\partial^2#1}{\partial #2^2}}$ |
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23-10-25 06:10:18 |
[NOTES/EM-03016] Electric Potential of Finite Charged Line SegmentThe electric potential due to charge spread uniformly on a finite line segment is computed.The electric potential due to charge spread uniformly on a finite line segment is computed. |
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23-10-22 18:10:24 |
2019-CM-I @ CMI :: All Lessons |
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22-08-27 10:08:11 |
LEC/QM-Mod24 Approximation Schemes for Time Dependent ProblemsQuantum Mechanics Lecture Notes-24
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22-08-25 23:08:36 |
\(\S 17.1\) Statement of the ProblemQuantum Mechanics Lecture Notes-17 HOME PAGE
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22-08-25 09:08:56 |
[ARA-G001-PATH ]All Resources About Green FunctionGreen function is defined and a simple example is presented.
Examples include Green function for Poisson equation, Helmholtz equation, Heat equation, Wave Equation and Schrodinger equation. |
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22-08-10 06:08:21 |
[SUNDAY-PHYSICS/CV-LEC-04] Taylor Series Expansion |
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22-08-09 23:08:48 |
[Sample PDF Document WITH TOC] Defining Electric and Magnetic FieldsTABLE OF CONTENTS
The electric field is defined as the force experienced by a unit positive charge in the direction of the electric field. A charge moving in magnetic field experiences a force perpendicular to the velocity and the magnetic field. The fields are defined in terms of the force experienced by a unit positive charge as described below.
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22-06-28 12:06:20 |
[LEC/QM-23001] Non degenerate perturbation theory |
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22-05-28 22:05:56 |
[LEC/QM-23003] Application to fine structure of hydrogen atom |
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22-05-28 20:05:11 |