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Python Code for extracting patternNode id: 696blogUses lists and slicing in python
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19-12-28 03:12:56 |
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Curated video contentNode id: 3548video_page |
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22-04-02 23:04:50 |
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[QUE/TH-07009] TH-PROBLEMNode id: 5215pageTen grams of water at 20$^\circ$C is converted into ice at -10$^\circ$C at constant atmospheric pressure. Assuming the heat capacity per gram of liquid water to remain constant at 4.2 J/g\,K, and that of ice to be one half of this value, and taking the heat of fusion of ice at 0$^\circ$C to be 335 J/g, calculate the total entropy change of the system.
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22-01-23 11:01:19 |
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[NOTES/EM-02010] Gauss Law and Use of SymmetryNode id: 5956pageGauss law aloe is not sufficient to determine the electric field for a given system.To determine electric field using Gauss law the symmetry of problem plays an important role by determining the direction of the electric field in given problem.
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23-10-18 19:10:36 |
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[2019EM/QUIZ-10]Node id: 5362pageElectrodynamics Apr 8, 2019 Quiz-X
- At the upper surface of the Earth’s atmosphere, the time-averaged magnitude of the Poynting vector \(<S> =1.35^10^{W/m}^2\) is referred to as
the solar constant.
- Assuming that the Sun’s electromagnetic radiation is a plane sinusoidal wave, what are the magnitudes of the electric and magnetic fields?
- What is the total time-averaged power radiated by the Sun? The mean Sun-Earth distance is \(R =1.50\times10^{11}\) m .
- Following equation contains the complete information about the electromagnetic wave \begin{equation*} \vec{E}(z,t)=E_0\sin(kz-\omega t)\hat{i} \end{equation*} Find the directions of wave propagation, wavelength, frequency, speed of propagation, magnetic field, the Potynting vector and the intensity of the wave.
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22-04-04 17:04:27 |
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[2018EM/HMW-05]Node id: 5426page |
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22-06-21 08:06:40 |
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[NOTES/EM-01003]-Thomson’s parabola methodNode id: 5507pageThe parabola method was used to measure charge to mass ratio of the electron by measuring the deflection of the electrons when they pass through a uniform electric field. The method is described here and an expression for \(e/m\) in terms of the deflection of the electron.
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23-03-17 18:03:37 |
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[NOTES/EM-02007]-Maxwell's Equations for Electrostatics-INode id: 5579pageThe Gauss law of electrostatics follows from the Coulomb’s law for a point charge and superposition principle. The Gauss law along with the Gauss divergence theorem of vector calculus imply Maxwell’s first equation \(\nabla\cdot\bar{E}=\rho/\epsilon_0\) for electrostatics
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23-10-10 20:10:14 |
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[NOTES/QM-09002] Time Variation of Average ValuesNode id: 4679page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
Assuming time development of states to be given by \[i\hbar \dd[\ket{\psi, t}]{t} = H \ket{\psi t}, \] an equation for time variation of average value of a dynamical variable is derived. Classical correspondence is used to identify the generator of time evolution with Hamiltonian. A dynamical variable not depending explicitly on time is a constant of motion if it commutes with the Hamiltonian.
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24-06-22 09:06:35 |
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[NOTES/EM-03006]-Electrostatic Energy of a Uniformly Charged Solid SphereNode id: 5643page The electrostatic energy of a uniformly charged solid sphere is computed by computing the energy required to bring infinitesimal quantities and filling up the sphere.
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23-10-18 13:10:39 |
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[NOTES/QM-17005] States Using Ladder OperatorsNode id: 4819page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$ $\newcommand{\ket}[1]{\langle #1\rangle}$ qm-lec-17005
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22-03-04 09:03:06 |
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[NOTES/ME-14010]-Tennis Racket TheoremNode id: 5703page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
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22-08-17 16:08:14 |
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[NOTES/QM-25005] Einstein $A$ and $B$ CoefficientsNode id: 4974page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}\newcommand{\dd}[2][]{\frac{d#1}{d#2}}\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}\newcommand{\average}[2]{\langle#1|#2|#1\rangle}\newcommand{\ket}[1]{\langle #1\rangle}$
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24-04-09 14:04:32 |
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[LECS/EM-10004]-Conservation and Flow of Energy of Electromagnetic FieldsNode id: 5760page |
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22-09-11 13:09:22 |
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[QUE/SM-06001] SM-PROBLEMNode id: 5072pageConsider a photon gas in two dimensions at temperature T in area A. Find the energy density $u(\omega)$ as a function of temperature and various physical constants. Show that the total energy is proportional to $T^3$. ( you can assume that the internal degree of freedom is 1
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22-01-13 16:01:48 |
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[QUE/TH-01004] TH-PROBLEMNode id: 5189page
Express the temperatures given below in $^\circ C,R$, and $^\circ F$. Write your answers in form of table.
- (a) Triple point of Hydrogen 13.81 K
- (b) Boiling point of Ne 27.102 K
- (c) Boiling point of Oxygen 90.188 K
- (d) Melting point of zinc 692.664
- (e) Melting point of gold 1337.58
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22-10-17 15:10:45 |
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[2008EM/HMW-02]Node id: 5399page |
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22-05-10 16:05:40 |
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[2003SM/LNP-18] Lecture-18--Grand Canonical Ensemble — Summary and ApplicationsNode id: 5543pageThe main result for grand canonical ensemble are summarized. The Planck’s law and the Stephan Boltzmann law for black body radiation are derived.
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22-07-07 07:07:35 |
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[1998TH/LNP-39]-Statistical Mechanics of an Ideal GasNode id: 5607page |
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22-07-17 19:07:25 |
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[NOTES/ME-06002]-Using graph of $V(x)$ to find motionNode id: 5675page |
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22-08-14 09:08:58 |
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