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[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.
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22-06-11 13:06:58 |
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[2003SM/LNP-03] Lecture-03-- Uncertainty in StatisticsNode id: 5526pageFor an experiment whose outcomes of simple events 1,...n have probabilities \(p_1, p_2, ...p_n\), the uncertainty, \(H(p)\) ,is defined a
$$ H(p_1, p_2, .., p_n) = − \sum_n p_n \ln p_n $$
Some important properties of uncertainty are Taking several examples, several properties of the uncertainty are brought out. The uncertainty is maximum when all probabilities are equal. It is zero when one of the events has probability1 and all other events have zero probability. The uncertainty for case of two independent random variables is the sum of individual uncertainties. By means of examples, it is shown that increase (decrease) in uncertainty is associated with decrease (increase) in information.
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22-07-04 10:07:59 |
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[1998TH/LNP-21]-EntropyNode id: 5591page |
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22-07-17 18:07:23 |
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[NOTES/QM-09007] Interaction Picture of Quantum MechanicsNode id: 4710page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}\newcommand{\dd}[2][]{\frac{d#1}{d#2}}\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ The interaction picture, also known as Dirac picture, or the intermediate picture, is defined by splitting the Hamiltonian in two parts, the free and the interaction parts. In interaction picture equation of motion for the observables is free particle equation. The state vector satisfies Schrodinger equation with interaction Hamiltonian giving the rate of time evolution.
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24-03-24 19:03:00 |
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[NOTES/QM-18007] Validity of Born Approximation Square Well PotentialNode id: 4839page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ $\newcommand{\ket}[1]{\langle #1\rangle}$ qm-lec-18007
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22-03-04 22:03:04 |
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[NOTES/EM-07010]-Magnetic Field of a Current Distribution at a Large DistancesNode id: 5715page
For a volume distribution of current an expression for magnetization density,{\it i.e.} the magnetic moment per unit volume, is obtained. An expression for the magnetic field at large distances, in terms of magnetization density, is derived.
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23-03-03 20:03:07 |
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[QUE/EM-02007] EM-PROBLEMNode id: 5108pageThe 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.
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22-01-09 21:01:58 |
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[QUE/TH-02010] TH-PROBLEMNode id: 5201pageThe $U$-tube in Fig.-1 below, of uniform cross section 1 cm$^2$, contains mercury to the depth shown. The barometric pressure is 750 Torr. The left side of the tube is now closed at the top, and the right side in connected to a good vacuum pump. Assuming that the temperature remains constant answer the following questions.
- How far does the mercury level fall in the left side?
- What is final pressure of the trapped air?
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22-01-20 09:01:18 |
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[2008EM/EVAL-QUIZ-01B]Node id: 5411page |
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22-07-11 16:07:40 |
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[QUE/EM-01007] --- EM-PROBLEMNode id: 5485pageFor an alpha particle approaching a nucleus of charge \(Ze\) from a large distance with energy \(E>0\) and having impact parameter \(b\). Find the distance of closest approach as function of energy and impact parameter.
Answer {\(\frac{k+\sqrt{k^2+4E^2b^2}}{2E}\)}
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23-05-05 21:05:06 |
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[2003SM/Eval-Suppl]Node id: 5555page |
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22-07-10 06:07:17 |
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[NOTES/QM-09008] Perturbation Expansion in Interaction pictureNode id: 4711page
The equation \[i\hbar\frac{d U(t,t_0)}{dt} = H'_I(t) U(t,t_0).\] obeyed by the time evolution operator in the interaction picture is converted into an integral equation. A perturbative solution is obtained from the integral equation following a standard iterative procedure.
$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}\newcommand{\dd}[2][]{\frac{d#1}{d#2}}\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
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24-03-24 19:03:37 |
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[NOTES/QM-18011] Green Function for Perturbative Solution of ScatteringNode id: 4840page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ $\newcommand{\ket}[1]{\langle #1\rangle}$ qm-lec-18011
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22-03-04 22:03:06 |
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[NOTES/EM-07011]-Direction convention for Ampere’s LawNode id: 5716page
Direction convention for Ampere's law is explained
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23-03-03 20:03:34 |
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[QUE/EM-02008] EM-PROBLEMNode id: 5111pageA plane carries a uniform charge density $\sigma_0$ per unit area. A central circular hole is cut removing the charge in the circular disk. Find the electric field above the center of the hole at a distance $d$ from the center.
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22-01-09 21:01:47 |
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[QUE/TH-02011] TH-PROBLEMNode id: 5202pageFig.-2 shows five processes, $a-b,~b-c,~c-d,~d-a,~a-c$, plotted in the $P-v$ plane for an ideal gas in a closed system. Show the same processes (a) in the $P-T$ plane. (b) in the $T-v$
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22-01-20 09:01:44 |
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[2019EM/Final]Node id: 5349pageTIME :3hrs ELECTRODYNAMICS MM:100
End Semester Examination
ATTEMPT ANY FIVE QUESTIONS.
- Find the potential due to a sphere carrying a uniform polarization \(\vec{P}\). The centre of the sphere is at the origin and radius of the sphere is \(R\). What is the electric field at a point (i) inside the sphere (ii) outside the sphere?
- Give an example of a charge configuration such that its dipole moment is zero and quadrupole moment depends on the choice of origin.
- An 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 alpha particle = \(6.64424. 10^{-27}\)kg \(\approx 4\times M_p= 4\times938.27\) MeV.
- A circular coil is formed from a wire of length $L$ with $n$ turns. The coil carries a current $I$ and is placed in an external uniform magnetic field $B$. Show that maximum torque developed is $\displaystyle\frac{IBL^2}{4n\pi}$.
- Give examples of at least six results/concepts that require modifications in time varying situation. [4+5+5+6]
- Derive an expression for electrostatic energy of a charge distribution and hence show that electric field carries energy density \(\frac{\epsilon_0}{2}|\vec{E}|^2\).
- A conducting spherical shell carries a charge \(Q\), compute its electrostatic energy and hence obtain an expression for the capacitance of the shell.\hfill[10+10]
- A rod of mass $m$ and length $\ell$ and resistance $R$ starts from rest and slides on two parallel rails of zero resistance as shown in figure 1. A uniform magnetic field fill the area and is perpendicular and out of the plane of the paper. A battery of of voltage $V$ is connected as shown in the figure 1.
- Argue that the net EMF in the loop is $V = Bv\ell$ when the rod has speed $v$.
- Write down $F = m\big(\dfrac{dv}{dt}\big)$ and integrate it so show that \begin{equation*}\label{EQ01} v(t) =\frac{V}{B\ell}\Big(1- \exp\Big(- \frac{B^2\ell^2 t}{mR}\Big)\Big). \end{equation*} Hint: Find the limiting speed and separate that out from the total $v$.
- What happens when the direction of magnetic field is reversed? [8+8+4]
- Show that, in absence of charges and currents, the electric and magnetic fields obey wave equation.
- State and prove important properties of plane wave solutions.
- Obtain an expression for energy density and intensity of plane waves. [6+8+6]
- An infinite rectangular hollow pipe is bounded by the planes \(x=\pm a,y=0, y=b\). The pipe extends to infinity in positive as well as negative \(Z\)- directions. The sides \(y=0, x=\pm a\) are grounded and the the side \(y=b\) is held at constant potential \(\phi_0\). Show that the potential inside the pipe is \begin{equation*} \phi(x,y) = \phi_0\Big\{\frac{y}{b} +\frac{2}{\pi} \sum_{n=1}^\infty\frac{(-1)^n}{n} \frac{\cosh (n\pi x/b)}{\cosh(n\pi a/b)} \sin (n\pi y /b) \Big\} \end{equation*}
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22-04-03 11:04:05 |
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[2008EM/QUIZ-01B-ANS]Node id: 5412page |
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22-05-11 08:05:40 |
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[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.
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22-06-18 12:06:30 |
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[2003SM/Eval-Suppl]Node id: 5556page |
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22-07-10 06:07:37 |
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