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testing/debuggingNode id: 6007page\begin{equation} \frac{\mu_0}{4\pi} =10^{-7} \text{henry/meter} \end{equation} |
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23-11-07 06:11:55 |
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[SUM/EM-10001] Summary of Equations in Static and Dynamic SituationsNode id: 6001page |
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23-11-06 08:11:07 |
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[NOTES/EM-07003]-Biot Savart Law from Maxwell's equationsNode id: 5709page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
Starting form Maxwell's equations for magnetostatics, vector potential is introduced and the Biot-Savart Law is derived.
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23-11-05 07:11:57 |
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[NOTES/EM-07002]-Current ConservationNode id: 5708page
The equation of continuity for conservation of electric is derived. An expression for current in a wire is obtained in terms of number of electrons per unit volume.
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23-11-05 07:11:37 |
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[NOTES/EM-07001]-Electric CurrentNode id: 5707page
In this section we compute the leading term in the magnetic field of a current loop at large distances and obtain an expression for the magnetic moment of the loop.
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23-11-05 07:11:56 |
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[NOTES/EM-07017]Node id: 5997page
The magnetic moment for a point particle is shown to be related to the angular momentum \(\ell\) and is given by \begin{equation} \vec{m} = \frac{q}{2M}\vec{\ell} \end{equation}
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23-11-05 07:11:02 |
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[NOTES/EM-07004] Stokes TheoremNode id: 6000page
Relationship between the normal to a surface and the orientation of its boundary curve, as they should appear in Stokes theorem are explained.
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23-11-05 07:11:25 |
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[NOTES/EM-07021] Cross Product RuleNode id: 5999page |
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23-11-05 00:11:20 |
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[NOTES/EM-07014] Conservation Laws for Electromagnetic FieldsNode id: 5998page$\newcommand{\Tca}{\mathcal T}\newcommand{\Pca}{\mathcal P}$ |
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23-11-04 23:11:23 |
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[NOTES/EM-01001] Electromagnetic Theory --- RepositoryNode id: 5996collection
- This repository of NOTES in quantum mechanics.
- Created for internal use of PROOFS PROGRAM
- Primarily useful for content authors.
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23-11-04 15:11:10 |
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[NOTES/CM-01001] Classical Mechanics --- RepositoryNode id: 5995collection
- This repository of NOTES in quantum mechanics.
- Created for internal use of PROOFS PROGRAM
- Primarily useful for content authors.
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23-11-04 15:11:08 |
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[NOTES/QM-ALL] Quantum Mechanics --- REPOSITORYNode id: 5994collection
- This repository of NOTES in quantum mechanics.
- Created for internal use of PROOFS PROGRAM
- Primarily useful for content authors.
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23-11-04 14:11:57 |
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[NOTES/EM-07020] Charge ConservationNode id: 5993pageThe meaning of charge conservation is discussed. It is known to be mathematically represented by the equation of continuity. It is argued that special relativity requires that there should be a 'current' associated with every conserved quantity. |
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23-11-04 05:11:01 |
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[LECS/QM-ALL] Quantum Mechanics --- No Frill Lecture Notes Node id: 5874collectionAbout this collection: This is a collection of Lecture Notes on Quantum Mechanics. 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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23-11-03 14:11:26 |
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[NOTES/EM-07006]-Lorentz Force on a Current DistributionNode id: 5711pageStarting from Lorentz force per unit volume on a current carrying conductor due to magnetic field is shown to be \(\vec{j}\times\vec{B}\) |
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23-11-03 12:11:44 |
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[NOTES/EM-07019] Solving for Vector PotentialNode id: 5992page$ \newcommand{\Prime}{^\prime}$ |
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23-11-02 18:11:39 |
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[NOTES/EM-07018] Poisson Equation for Vector Potential.Node id: 5991page |
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23-11-02 18:11:21 |
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[NOTES/EM-04017] Magnetic Moment of a System of Point Particles Node id: 5990pageThe magnetic moment for a point particle is shown to be related to the angular momentum \(\ell\) and is given by \begin{equation} \vec{m} = \frac{q}{2M}\vec{\ell} \end{equation} |
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23-11-02 17:11:12 |
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[NOTES/EM-07016] Force on a Line and Volume Element of a WireNode id: 5989pageExpressions for force on line and volume elements of a current in magnetic field are derived. |
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23-11-02 16:11:52 |
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[NOTES/EM-07015] Current Density --- ExamplesNode id: 5988page |
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23-11-02 16:11:09 |
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