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LECS/ME-ALL] Newtonian Mechanics --- No Frill LecturesNode id: 6269collectionAbout this collection: This is a collection of Lecture Notes on Electromagnetic Theory. An effort is made to keep the content focused on the main topics. There is no discussion of related topics and no digression into unnecessary details.
Who may find it useful: Any one who wants to learn, or refresh all topics, in standard two semester quantum mechanics courses.
Topics covered: The list of topics covered appears in the main body of this page. Click on any topic to see details and links to content pages.
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24-05-29 04:05:45 |
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[NOTES/TH-ALL] Thermodynamics --- Repository of Notes for LecturesNode id: 6207collection[toc:0]
About this collection: This is a collection of Lecture Notes on Electromagnetic Theory. An effort is made to keep the content focused on the main topics. There is no discussion of related topics and no digression into unnecessary details.
Who may find it useful: Any one who wants to learn, or refresh all topics, in standard two semester quantum mechanics courses.
Topics covered: The list of topics covered appears in the main body of this page. Click on any topic to see details and links to content pages.
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24-05-29 04:05:31 |
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[Solved/QM-22003] Quantum Mechanics Problem --- Barrier penetration Node id: 1092page |
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24-05-28 13:05:09 |
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[Solved/ODE-02005] Frobenius Method --- Case-IINode id: 1805page |
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24-05-27 22:05:24 |
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Prof. Pankaj Sharan :: Eight Lectures on Topics From Electrodynamics Course given at Jamia Milia IslamiaNode id: 472page |
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24-05-27 22:05:15 |
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[NOTES/CM-11004] Hamilton Jacobi Equation Node id: 6263page We derive the time dependent and time independent Hamilton Jacobi equations, amilton's characetrirstic function is introduced as solution of the time independent equation.
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24-05-25 21:05:33 |
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Radiation from an Accelerated Point ChargeNode id: 444pdf_document |
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Fields from a Point ChargeNode id: 443pdf_document |
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24-05-22 11:05:14 |
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Fields for Arbitrary Charge and Current DensitiesNode id: 442pdf_document |
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Green's Function for the Helmholtz and the Wave EquationsNode id: 441pdf_document |
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24-05-22 11:05:14 |
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Generalized FunctionsNode id: 439pdf_document |
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Maxwell's EquationsNode id: 438pdf_document |
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Units and DimensionsNode id: 436pdf_document |
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[NOTES/CM-10003] Four Types of Canonical TransformationsNode id: 6251page$\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ A canonical transformation is a change of variables \((q,p) \rightarrow (Q,P)\) in phase space such that the Hamiltonian form of equations of motion is preserved. Depending choice of independent variables we have four special cases of canonical transformations., Generating functions for the four cases are introduced and details of the four cases are discussed.
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24-05-20 16:05:33 |
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[NOTES/CM-10002] A Summary Finite Canonical TransformationsNode id: 6258page$\newcommand{\pp}[2][]{\frac{\partial#1}{\partial #2}}$
Important relations of four types of transformations are summarized.
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24-05-20 07:05:43 |
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[NOTES/CM-10008] Examples --- Canonical TransformationsNode id: 6249pageSeveral examples on canonical transformations are given.
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24-05-19 08:05:33 |
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some title hereNode id: 6233collection |
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DOC/ Preprocessing Latex source code file Node id: 6250page |
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[NOTES/CM-10007] Generator of a Canonical TransformationNode id: 6248pageThe definition finite and infinitesimal canonical transformation are given. Using the action principle we define the generator of a canonical transformation. $\newcommand{\pp}[2][]{\frac{\partial#1}{\partial #2}}\newcommand{\Label}[1]{\label{#1}}$
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24-05-19 05:05:47 |
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[NOTES/CM-10006] Two Simple Examples of Canonical TransformationsNode id: 6247page$\newcommand{\pp}[2][]{\frac{\partial#1}{\partial #2}}$
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24-05-18 20:05:43 |
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