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[SCR/QM-23009] Hyperfine Structure of H- atom (4)Node id: 6073page |
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24-02-28 06:02:54 |
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[SCR/QM-23008] Theoretical Explanation of H Atom Fine Structure (14)Node id: 6072page |
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24-02-28 06:02:16 |
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[SCR/QM-23007] Observed Fine Structure of H AtomNode id: 6071page |
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24-02-28 06:02:26 |
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[SCR/QM-23011] Time Indep Perturb Theo --- Second Order Non Degenerate Case (7)Node id: 6070page |
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24-02-28 06:02:37 |
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[SCR/QM-23005] Time Independent Perturation Theory Second Order Degenerate Case (6)Node id: 6069page |
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24-02-28 06:02:12 |
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[SCR/QM-23004] Time Independent Perturation Theory First Order Degenerate Case (7)Node id: 6068page |
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24-02-28 05:02:21 |
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[LECS/QM-23004] Fine Structure of Hydrogen Atom (9)Node id: 6067page |
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24-02-28 05:02:34 |
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[SCR/QM-23001] PerturbationTheory --- Overview (6)Node id: 6065page |
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24-02-28 05:02:01 |
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[SCR/QM-23002] First Order Non-degenerate Theory (14)Node id: 6066page |
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24-02-28 04:02:48 |
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1.3 Postulates of QM --- Lectures given at Hyd Univ-2024 Refresher Course in PhysicsNode id: 6058page |
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24-02-26 06:02:20 |
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[LECS/EM-07001] Current and Current ConservationNode id: 5718page |
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24-02-23 22:02:04 |
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[LECS/EM-02003] Gauss LawNode id: 6025page
- The flux of electric field through a surface in defined as a surface integral and the statement of Gauss law is given.
- A few examples of computing the electric field using Gauss law and symmetry of the problem are discussed.
- A simple and intuitive proof of Gauss law is given following Feynman lectures. The task of proving Gauss law for arbitrary charge distribution is reduced to the problem proving the Gauss law for a single point charge by appealing to the superposition principle.
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24-02-23 20:02:40 |
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[LECS/EM-02002] Solved Examples --- Computation of Electric FieldNode id: 6035pageSolved Examples --- Computation of Electric Field
- Electric Field due to a Uniformly Charged Disk
- Electric Field of a Uniformly Charged Spherical Shell
- Field due to a Uniformly Charged Ring
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24-02-23 19:02:47 |
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A Site For Teachers, Learners and AuthorsNode id: 270pageThis site hosts an authoring environment. E-learning content creators can create, organize and share their learning content here. (Not for content monetization). You can only share the links of your content published here.
Main features of the authoring environment:
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24-01-28 10:01:29 |
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[QFRM/EM-01001] Electric Dipole in Uniform Electric FieldNode id: 6054page |
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24-01-25 12:01:54 |
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[WART/EM-07004] Is B always curl free in a region where the current is zero?Node id: 6053page |
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24-01-15 05:01:01 |
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[Help and Info] Copying and pasting Latex Source Codes.Node id: 6051page |
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24-01-05 08:01:22 |
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[NOTES/CM-2009] What is a Cyclic Coordinate?Node id: 6042pageCyclic coordinate, a useful concept in Lagrangian dynamics, is defined and is shown to give rise to a conservation law. $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ |
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23-12-27 23:12:49 |
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[NOTES/CM-02010] Lagrangian for Conservative ForcesNode id: 6041pageThe Lagrangian for conservative systems is defined as \(L=T-V\) and the Euler Lagrange equations take the form \begin{equation*} \frac{d}{dt}\frac{\partial{L}}{\partial\dot{q_k}}-\frac{\partial{L}}{\partial{ q_k}}=0. \end{equation*} |
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23-12-27 23:12:08 |
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[NOTES/CM-02011] Lagrangian For Velocity Dependent ForcesNode id: 6040pageFor systems for which the generalized forces can be derived from a generalized potential \(U\), the Lagrangian can be defined as \(L=T-U\) and the Euler Lagrange equations take the form \begin{equation*} \frac{d}{dt}\frac{\partial{L}}{\partial\dot{q_k}}-\frac{\partial{L}}{\partial{ q_k}}=0. \end{equation*} |
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23-12-27 23:12:44 |
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