|
checkingNode id: 5496page |
|
22-06-18 15:06:12 |
n |
|
PROOFS-Archive Node id: 3486collectionTABLE OF CONTENTS
MORE SETS WILL APPEAR HERE SOON
- Two Lectures Given at Madurai Kamraj University
- Four Lectures Given at BS Abdur Rahman University Crescent Institute of Science and Technology
- Classical Mechanics --- Hyd Univ Summer Course (2018)
- Mechanics --- BITS Hyderabad (2014)
- Classical Mechanics -I ---- CMI (2019)
- Quantum Mechanics --- Hyd Univ. 2010
- Quantum Mechanics --- Hyd Univ Summer Course (2018-19)
- Quantum Field Theory --- IIT Bhubneshwar QFT (2015)
- This collection has a variety of archived teaching resources.
- Contributed by friends colleagues and by some of my teachers at different institutions.
- Resources of selected courses given by me at different institutions.
- The resources can be downloaded
- Online viewing of resources here is not supported.
|
|
|
22-06-18 15:06:21 |
n |
|
[QUE/EM-01008] --- EM-PROBLEMNode id: 5486pageTwo pith balls, each of mass 1.8 g, are suspended from the same point by silk threads each of length 20 cm. When equal charge Q is given to both the balls, they separate until the two threads become perpendicular. Find the charge $Q$ on each pith ball. |
|
22-06-18 12:06:30 |
n |
|
[QUE/EM-01011] --- EM-PROBLEMNode id: 5489pageAn alpha particle travels in a circular path of radius $0.45$m in a magnetic field with $B=1.2$ w/m$^2$. Calculate (i) its speed (ii) its period of revolution, and (iii) its kinetic energy. Mass of proton particle = \(1.67\times 10^{-27}\)kg \(\approx 4\times M_p= 4\times938.27\) MeV.
Solution :
- [(i)] the magnetic force \(eBv\) must be equal to the mass times acceleration. Therefore \begin{equation*} Bev = \frac{Mv^2}{R}, \end{equation*} where \(R\) is the radius of the circular orbit. Hence \begin{equation*} v= \frac{eBR}{M} = \frac{2\times1.6 \times10^{-19}\times 1.2 \times 0.45}{4\times 1.67\times 10^{-27}}\approx 2.7 \times10^7 \text{m/s}. \end{equation*}
- [(ii)] The time period is \begin{equation*} T = \frac{2\pi R}{v} = \frac{2\times3.14\times 0.45}{2.7\times10^7} \approx10^{-7} \text{ s}. \end{equation*}
- [(iii)] The kinetic energy is given by \begin{eqnarray}\nonumber \text{K.E.} &=& \frac{1}{2} M v^2= \frac{1}{2}\times (4\times 1.67 \times 10^{-27}) \times \big(2.7\times10^7\big)^2 \\\nonumber &=& 3.26\times 7.29 \times 10^{-13} \approx 23.7 \times 10^{-13} \text{J}. \end{eqnarray}
|
|
22-06-18 12:06:19 |
n |
|
[QUE/EM-01012] --- EM-PROBLEMNode id: 5490pageFind the direction and magnitude of \(\vec{E}\) at the center of a square with charges at the corners as shown in figure below. Assume that \(q= 1\times 10^{-8}\)coul, \(a=5\)cm. |
|
22-06-18 12:06:00 |
n |
|
[QUE/EM-01013] --- EM-PROBLEMNode id: 5491pageA "dipole" is formed from a rod of length \(2a\) and two charges \(+q\) and \(-q\). Two such dipoles are oriented as shown in figure at the end, their centers being separated by a distance \(R\). Calculate the force exerted on the left dipole and show that, for \(R>>a\), the force is approximately given by \[F=\frac{3p^2}{2\pi\epsilon_0R^4}\] where \(p=2qa\) is the dipole moment. |
|
22-06-18 12:06:26 |
n |
|
[QUE/EM-01014] --- EM-PROBLEMNode id: 5492pageFind the direction and magnitude of $\vec{E}$ at the center of a square with charges at the corners as shown in figure below. Assume that $ q= 1\times 10^{-8}$coul, $a=5$cm. |
|
22-06-18 12:06:16 |
n |
|
[QUE/EM-01016] --- EM-PROBLEMNode id: 5494pageAn electron moving with speed of $5.0\times 10^8$cm/sec is shot parallel to an electric field strength of $1.0\times 10^3 $nt/coul arranged so as to retard its motion.
- How far will the electron travel in the field before coming (momentarily) to rest ?
- how much time will elapse?
- If the electric field ends abruptly after $0.8$ cm, what fraction of its initial energy will the electron loose in traversing the field?
|
|
22-06-18 12:06:07 |
n |
|
Mathematical Physics :: Bundled LessonsNode id: 3760page
- Vector Algebra
- Ordinary Differential Equations
- Partial Differential Equations
- Complex Variables
- Vector Spaces
- Group Theory
- Orthogonal Polynomials
- Special Functions of Mathematical Physics
- General Topics
|
|
22-06-18 10:06:34 |
n |
|
[QUE/EM-04014] EM-PROBLEMNode id: 2391pageProve that the potential \(\phi(0)\) at the center of a charge-free spherical volume \(V\) is the equal to average of \(\phi(r)\) over the surface \(S\) of the sphere. Using
- Green’s reciprocity relation.
- Green's identity\[\iiint d^3r (f \nabla^2 g − g\nabla^2 f ) = \iint \hat{n} · (f \nabla g − g\nabla f) dS\]
|
|
22-06-17 21:06:04 |
n |
|
[2018QM/QUIZ-03]Node id: 2140page
Quantum Mechanics (2018) A Course Given at University of Hyderabad Assignments, Quiz, Test and Examination Papers
|
|
22-06-17 21:06:38 |
n |
|
[ALL-RESOURCES-ABOUT] Computing Cross Sections and Life times Node id: 3446path |
|
22-06-17 20:06:24 |
n |
|
[ALL-RESOURCES-ABOUT] Green Function Node id: 2725curated_content
- Basic Definiton A simple example
- Calculating Green Function
- Using Fourier Transform
- Free Particle Schrodinger Equation
- Green Function for Klein Gordon Equation
- EigenfunctionExpansion
- Separation of Variables; Example from electrodynamics
- Uniqueness Theorem; Method of Images
- ApplicationsConverting to an integral equationBoundary Value Problemsin EMTheoryRelation to Energy Eigenvalues and Eigenfunctions
- AND MORE
IMPORTANT EACH PART IS SELF CONTAINED. YOU CAN START READING ANY PART, and CONTINUE in ANY ORDER
|
|
22-06-17 20:06:23 |
n |
|
[EWY/EM-01002] How are the Electric and Magnetic Fields Created?Node id: 5479page |
|
22-06-13 11:06:28 |
n |
|
[QUE/EM-04001] --- EM-PROBLEM Node id: 2241pageSolve the problem of a point charge and a grounded conducting sphere by expanding the Coulomb potential of the point charge in spherical harmonics with respect to the center of the sphere, solving for the potential for each \(\ell\) and resumming. |
|
22-06-11 23:06:40 |
n |
|
[QUE/EM-03015] --- EM-PROBLEM Node id: 2266pageSix charges are placed at positions given below:
|
Charge |
Position |
|
Charge |
Position |
1 |
q |
(L, 0, 0) |
4 |
- q |
(-2L,0,0) |
2 |
2q |
(0, 2L, 0) |
5 |
- 2q |
(0, 0,3L) |
3 |
3q |
(0,- 2L, 0) |
6 |
- 3q |
(0,0,L) |
Compute the dipole moment of the system.
|
|
22-06-11 23:06:59 |
n |
|
[QUE/EM-03024] --- EM-PROBLEM Node id: 2380pageFind the interaction energy of two interpenetrating spheres of uniform charge density \(\rho_1\) and \(\rho_2\). Let the two spheres have equal radii \(a\) and let the separation of their centers be \(d< a\). Show that your answer gives the value expected for the limiting case s (a) \(d=0\), and \(d=a\).
Panofsky and Philips
|
|
22-06-11 23:06:06 |
n |
|
[QUE/EM-03022] --- EM-PROBLEM Node id: 2240pageThe permanent dipole moment of water molecule is given to be \(1.86\times10^{-18}\) esc-cm. How much work is done on water molecule if electric field is increased from zero to 100 volts/cm and the permanent dipoe is rotated from \(\theta=0\) to \(\theta=\pi\)? (Be careful about units.)
Atlee Jackson |
|
22-06-11 23:06:58 |
n |
|
[QUE/EM-02016]Node id: 5441pageTwo spheres each of radius $R$ are placed so that they partially overlap. The charge densities in the overlap region is zero and in the two non overlapping regions is $+\rho$ and $-\rho$ respectively as shown in figure. The separation between the centres of the spheres is $D$. Show that the electric field in the overlap region is constant.
\FigBelow{100,-35}{50}{0}{em-fig-02002}{Overlapping spheres}\\ |
|
22-06-11 13:06:48 |
n |
|
[QUE/EM-02013]Node id: 5440pageThe electric field due to a line segment of length $2a$, and carrying a uniform line charge $\lambda$, at a distance $d$ above the mid point is given by $$ E = \frac{1}{4\pi\epsilon_0} \, \frac{2\lambda a}{d \sqrt{d^2 +a^2}}$$ Use this result to find the electric field of a {\bf square lamina} (side $2s$), carrying uniform surface charge density $\sigma$, at a distance $z$ above the center of the disk. |
|
22-06-11 13:06:58 |
n |