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HydrodynamicsNode id: 39page |
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23-10-30 07:10:25 |
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Elastic Deformations of a Solid BodyNode id: 38page |
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23-10-30 07:10:54 |
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Dynamics of a Solid BodyNode id: 37page |
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23-10-30 07:10:28 |
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Universal GravitationNode id: 36page |
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23-10-30 07:10:40 |
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Laws of Conservation of Energy, Momentum, and Angular MomentumNode id: 35page |
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23-10-29 07:10:48 |
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[LES/EM-07001] Currents and Current ConservationNode id: 5985collection |
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23-10-29 06:10:20 |
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[NOTES/EM-04010] Energy of Charged Capacitor and Force Between the PlatesNode id: 5984pageThe electrostatic energy stored in electric field is given by \[\mathcal E = \frac{\epsilon_0}{2}\int |\vec E|^2 d^3r.\] In this article a few selected applications of the above expression for electrostatic energy to the problems involving capacitors are discussed. |
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23-10-27 12:10:10 |
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[NOTES/EM-04011] Systems of Several ConductorsNode id: 5983pageTaking examples of a spherical capacitor, we show how the capacitance can be computed using the linearity of relation between the potentials and charges of conductors. |
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23-10-27 11:10:55 |
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[NOTES/EM-04014] Electric Potential in Presence of ConductorsNode id: 5982pageThe Maxwell's equations imply that the electric potential \(\phi\) obeys Poisson equation \(\nabla^2 \phi = -\rho/\epsilon_0,\) where \(\rho\) is the charged density. |
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23-10-27 10:10:42 |
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[NOTES/EM-04013] Example --- The Method of ImagesNode id: 5981pageThe solution of a thick shell and a point charge problem by the method of images is outlined. |
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23-10-27 10:10:34 |
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The Fundamental Equation of DynamicsNode id: 34page |
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23-10-26 08:10:00 |
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KinematicsNode id: 33page |
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23-10-25 23:10:54 |
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Thermal Radiation. Quantum Nature of LightNode id: 4291page$\newcommand\lambdabar{ \raise2.5pt{\moveright5.0pt\unicode{0x0335}}\moveleft1pt\lambda }$ |
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23-10-25 23:10:28 |
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Test Collection :: Like a section of a bookNode id: 5980collection |
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23-10-25 22:10:35 |
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[NOTES/EM-04005] Uniqueness Theorems --- ExamplesNode id: 5975pageThe solution of Poisson equation in a region, is unique for a specified charge density and under given boundary conditions. The uniqueness theorem is explained by means of several simple examples. |
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23-10-25 19:10:01 |
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[NOTES/EM-04009] The Method of ImagesNode id: 5979page
The method of images makes use of The uniqueness of solutions to boundary value problem makes it possible to relate solution of a given problem in a region \(R\)to another problem with same charge density and boundary conditions. The basic working of the method of images exploits this by for probles involving conductors. It relates the given problem to another problem without conductors but with a set of image charges chosen in a manner that meets the requirement of the uniqueness theorem. The solution to the second problem then provides the desired solution.
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23-10-25 19:10:31 |
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[NOTES/EM-04008] The Method of Images --- ExamplesNode id: 5978pageIn this section the solution of a boundary value problem involving a point charge and a grounded conducting sphere is obtained using the method of images. |
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23-10-25 18:10:57 |
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[NOTES/EM-04007] The Method of ImagesNode id: 5977pageThe solution of a potential for a point charge and a grounded infinite plane conductor is given, without any details, using the method of images. |
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23-10-25 16:10:10 |
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[NOTES/EM-04006] Uniqueness Theorems Node id: 5976pageUniqueness theorems for solutions of Laplace equation are stated and proved. |
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23-10-25 15:10:43 |
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[NOTES/EM-04004] Electric Field Near a Charged ConductorNode id: 5974pageGauss law is used to determine the electric field near the surface of a conductor is obtained in terms of the surface charge density. |
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23-10-25 09:10:49 |
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