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[2019EM/MidSem-1]

Node id: 5350page

                                            Mid Semester Examination∗

B.Sc. IInd                                                                                           Sem MM: 30

  1. 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.
  2. 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 \(Q\). 
  3. 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} 
AK-47's picture 22-04-03 11:04:09 n

[2008EM/EVAL-QUIZ-02]

Node id: 5414page
AK-47's picture 22-07-11 16:07:44 n

[QUE/EM-01011] --- EM-PROBLEM

Node id: 5489page

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 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}
AK-47's picture 22-06-18 12:06:19 n

[2003SM/Eval-Test-I]

Node id: 5557page
AK-47's picture 22-07-10 06:07:37 n

[RCQ/CV-05002] Recalling Reasoning for Singular Points

Node id: 5627page
AK-47's picture 22-08-06 19:08:16 n

[NOTES/QM-16008] Spherically Symmetric Square Well

Node id: 4800page

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qm-lec-16008

AK-47's picture 22-03-07 20:03:18 y

[NOTES/ME-08007]-Equality of Inertial and Gravitational masses

Node id: 5691page
AK-47's picture 22-08-16 13:08:56 n

[LECS/EM-10001]-Maxwell’s Equation for Time Varying Fields

Node id: 5747page
AK-47's picture 22-09-03 18:09:15 n

[QUE/TH-02001] TH-PROBLEM

Node id: 5040page

Consider 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 $A_1$?

AK-47's picture 22-01-14 10:01:44 n

[QUE/TH-13004] TH-PROBLEM

Node id: 5175page

The 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}

AK-47's picture 22-01-13 17:01:57 n

Mechanics --- Notes for Lectures and Problems --- [ME-MIXED-LOT]

Node id: 5236collection
AK-47's picture 22-02-07 10:02:49 n

[2013EM/HMW-07]

Node id: 5381page
AK-47's picture 22-04-17 09:04:48 n

[PSET/EM-02001]

Node id: 5445page
AK-47's picture 22-05-26 19:05:56 n

[2003SM/LNP-06] Lecture-06--What is Thermodynamics and Statistical Mechanics

Node id: 5531page

We 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.

AK-47's picture 22-07-06 07:07:01 n

[1998TH/LNP-25]-Efficiency of Carnot Engine

Node id: 5595page
AK-47's picture 22-07-17 18:07:48 n

[NOTES/QM-10001] Representations in an Inner Product Space

Node id: 4719page

A 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.

AK-47's picture 24-06-22 11:06:31 n

[NOTES/QM-20003] Spin Wave Function

Node id: 4846page

$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ 
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qm-lec-20003

AK-47's picture 22-03-05 08:03:48 y

[LECS/EM-07002]-Magnetic Field of Currents

Node id: 5719page
AK-47's picture 22-08-23 17:08:43 n

21th-hmw-01

Node id: 4992page
AK-47's picture 21-11-26 19:11:03 n

[QUE/EM-02023] EM-PROBLEM

Node id: 5126page

Use 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.

AK-47's picture 22-01-09 21:01:52 n

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