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[2019EM/MidSem-1]Node id: 5350page Mid Semester Examination∗
B.Sc. IInd Sem MM: 30
- A circular disk of radius \(R\) carries a surface charge density \(\sigma=kr\). Find the potential at a point on the axis of the disk and distance \(d\) from the center of the disk.
- Two grounded infinite conducting planes are kept along the \(XZ\) and \(YZ\) planes, see Fig.2. A charge \(Q\) is placed at (4,3) find the force acting on the charge \(Q\).

- Solve the boundary value problem in volume \(V\) bounded by semi-infnite planes (i) Plane 1:\(XZ\) plane extending to infinity in positive \(z\) and both positive and negative \(x\) directions.(ii)Plane 2: Another plane parallel to Plane 1 obtained by translating it to \(y=L\)(iii)Infinite strip: A strip lying in \(XY\) plane between \(0\le y \le L\). The boundary conditions required to be satisfied are \begin{equation} \phi(x,y,z)= \begin{cases} 0 & \text{for } y=0 \text{ and all } x, z\\ 0 &\text{for } y=L \text{ and all } x, z\\ 0 & \text{ as } z \to \infty \\ \cos(3\pi y/L) \sin(5\pi y/L) & \text{ for } z=0 \text{ and } 0\le y \le L \end{cases} \end{equation}

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22-04-03 11:04:09 |
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[2008EM/EVAL-QUIZ-02]Node id: 5414page |
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22-07-11 16:07:44 |
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[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}
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22-06-18 12:06:19 |
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[2003SM/Eval-Test-I]Node id: 5557page |
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22-07-10 06:07:37 |
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[RCQ/CV-05002] Recalling Reasoning for Singular PointsNode id: 5627page |
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22-08-06 19:08:16 |
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[NOTES/QM-16008] Spherically Symmetric Square WellNode id: 4800page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ qm-lec-16008
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22-03-07 20:03:18 |
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[NOTES/ME-08007]-Equality of Inertial and Gravitational massesNode id: 5691page |
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22-08-16 13:08:56 |
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[LECS/EM-10001]-Maxwell’s Equation for Time Varying FieldsNode id: 5747page |
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22-09-03 18:09:15 |
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[QUE/TH-02001] TH-PROBLEMNode id: 5040pageConsider a closed cylinder whose walls are adiabatic. The cylinder is divided into three equal parts $A_1$, $A_2$ and $A_3$ by means of partitions $S_1$ and $S_2$, which can move along the length of the cylinder without friction. The partition $S_1$ is adiabatic and $S_2$ is conducting. Initially, each of the three parts contain one mole of Helium gas, which can be treated as an ideal gas, is at pressure $P_0$, temperature $T_0$ and volume $V_0$. Assume the specific heat at constant volume $C_v\,=\,\frac{3R}{2}$ and the specific heat at constant pressure $C_p\,=\,\frac{5R}{2}$. Now, heat is supplied to the to the left most partition $A_1$ till the temperature in part $A_3$ becomes $T_3\,=\,\frac{9T_0}{4}$ Find the final volume, pressure and temperature in terms of $V_0$, $P_0$ and $T_0$. Assume the entire process is quasistatic. \vskip 3mm 3. ( Continuation of problem 2)
(a) What is work done by the gas in $A_1$ ?
(b) What is the heat supplied to the gas in $A_1$?

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22-01-14 10:01:44 |
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[QUE/TH-13004] TH-PROBLEMNode id: 5175pageThe fundamental equation for a system is given by \begin{equation*} u = \Lambda \frac{s^{3/2}}{v^{1/2}} \end{equation*} where \(\Lambda\) is a constant. Prove the following equations \begin{eqnarray} T &=& \frac{5}{2} \frac{\Lambda S^{3/2}}{NV^{1/2}}\\ P V^{2/3} &=& N \frac{N \Lambda 2^{1/2}}{5*{3/2}} T^{5/3}\\ \mu &=& - \Big(\frac{2}{5}\Big)^{5/2} \frac{2}{\Lambda ^{2/3}} \Big(\frac{V}{N}\Big)^{1/3} T^{5/3}. \end{eqnarray}
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22-01-13 17:01:57 |
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Mechanics --- Notes for Lectures and Problems --- [ME-MIXED-LOT]Node id: 5236collection |
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22-02-07 10:02:49 |
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[2013EM/HMW-07]Node id: 5381page |
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22-04-17 09:04:48 |
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[PSET/EM-02001]Node id: 5445page |
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22-05-26 19:05:56 |
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[2003SM/LNP-06] Lecture-06--What is Thermodynamics and Statistical MechanicsNode id: 5531pageWe begin with scope of thermodynamics and emphasize wide range of its applications. Thermodynamics takes a macroscopic view of a physical system. It laws are based on experience. Statistical mechanics is a microscopic view of physical systems and is based on established laws of classical and quantum mechanics.
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22-07-06 07:07:01 |
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[1998TH/LNP-25]-Efficiency of Carnot EngineNode id: 5595page |
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22-07-17 18:07:48 |
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[NOTES/QM-10001] Representations in an Inner Product SpaceNode id: 4719pageA brief account of representations in a finite dimensional vector spaces is presented. The use of an ortho norrnal basis along with Dirac notation makes all frequently used formula very intuitive. The formulas for representing a vector by a column vector and an operator by matrices are given. The results for change of o.n. bases are summarized.
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24-06-22 11:06:31 |
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[NOTES/QM-20003] Spin Wave Function Node id: 4846page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ $\newcommand{\ket}[1]{\langle #1\rangle}$ qm-lec-20003
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22-03-05 08:03:48 |
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[LECS/EM-07002]-Magnetic Field of CurrentsNode id: 5719page |
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22-08-23 17:08:43 |
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21th-hmw-01Node id: 4992page |
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21-11-26 19:11:03 |
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[QUE/EM-02023] EM-PROBLEMNode id: 5126pageUse Gauss's law to find the electric field inside a uniformly charged solid sphere of radius \(R\) and carrying charged density $\rho$. State facts other than Gauss's law which you might have used in your answer.
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22-01-09 21:01:52 |
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