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2644 records found.

Title+Summary	Name	Date
[MORE/EM-09001] Ballastic Galvanometer Node id: 5438page	kapoor	22-08-14 17:08:56	n
[NOTES/ME-06003]-Time Period of Oscillations--Method-1 Node id: 5678page	AK-47	22-08-14 10:08:20	n
[NOTES/ME-02003]-Euler Angles Node id: 5658page	AK-47	22-08-14 10:08:22	n
[NOTES/ME-02007]-Einstein Summation Convention Node id: 5667page	AK-47	22-08-14 10:08:19	n
[NOTES/ME-02008]-Active and Passive Rotation Node id: 5668page	AK-47	22-08-14 10:08:29	n
[NOTES/ME-02009]-Vectors as geometrical objects Node id: 5669page Convention about vectors is described. Different different symbols are used for vectors without reference to any axis, components of vector w.r.t. a system of coordinate axes, column vector notation for components	AK-47	22-08-14 10:08:24	n
[NOTES/ME-02011]-no title Node id: 5671page $\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1\|#2\|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1\|#2\|#1\rangle}$ $\newcommand{\xbf}{\bf x}$	AK-47	22-08-14 10:08:37	y
[NOTES/ME-06001]- Application of Energy Conservation Law Node id: 5672page $\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1\|#2\|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1\|#2\|#1\rangle}$	AK-47	22-08-14 10:08:50	y
[NOTES/ME-02010]-Rotation of Vector about an Arbitrary Axis Node id: 5670page	AK-47	22-08-14 10:08:35	y
[NOTES/ME-06002]-Using graph of $V(x)$ to find motion Node id: 5675page	AK-47	22-08-14 09:08:58	n
[NOTES/ME-06002b]-Using graph of $V(x)$ to find motion Node id: 5677page	AK-47	22-08-14 09:08:44	y
[NOTES/ME-06001a]-Energy Conservation Node id: 5673page $\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1\|#2\|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1\|#2\|#1\rangle}$	AK-47	22-08-14 09:08:56	y
[NOTES/ME-06001b]-Using energy conservation to reduce solution to quadratures Node id: 5674page	AK-47	22-08-14 09:08:39	y
[LSN/ME-12002] Motion in Spherically Symmetric Potentials Node id: 4140page	shivahcu	22-08-13 23:08:11	n
Sample Video Page Node id: 5665video_page This is page with text as well as a screen recording. Screen recording of Problem Solving	kapoor	22-08-12 11:08:43	n
Sample Video Page Node id: 5663video_page	kapoor	22-08-12 11:08:15	n
[INDEX-TEACH&LEARN/ME] Newtonian Mechanics Node id: 5661page TEACHING AND LEARNING Quick Review of prerequisites Kinematics in Different Coordinate Systems Newton's Laws Work and Energy Simple Harmonic Motion, Small Oscillations Noninertial Frames, Pseudo Forces Centre of Mass and Linear Momentum Rotational Motion Decomposition of Kinetic Energy and Angular Momentum Two Body Problem Multi particle System Kinematics of Rigid Body Rigid Body Dynamics	kapoor	22-08-11 22:08:00	y
[INDEX-TEACH&LEARN/ME] Newtonian Mechanics Node id: 5660page	kapoor	22-08-11 22:08:24	n
[INDEX-TEACH&LEARN/EM] Electromagnetic Theory Node id: 5659page Electric and Magnetic Fields Electrostatics Electric Potential and Electrostatic Energy Conductors in Electric field Maxwell's Equations in Dielectric Boundary Value Problems in Presence of Dielectric Media Magnetic Field Magnetostatics of Magnetic Media Electromagnetic Induction Maxwell's Equations in Time Varying Situations Electromagnetic Waves Relativistic Electrodynamics Potentials and Fields of a Moving Point Charge Radiation	kapoor	22-08-11 22:08:52	y
Check Code Node id: 5638page $\newcommand{\mid}{\|}$ $\newcommand{\label}[1]{}$ \begin{eqnarray} W_2&=&\frac{q_1q_2}{4\pi\epsilon_0\mid\bar{r_1}-\bar{r_2}\mid} \label{eq2}\\ W_3&=&\frac{q_1q_3}{4\pi\epsilon_0\mid\bar{r_1}-\bar{r_3}\mid}+\frac{q_2q_3}{ 4\pi\epsilon_0\mid\bar{r_3}-\bar{r_2}\mid} \label{eq3}\\ W_4&=&\frac{q_1q_4}{4\pi\epsilon_0\mid\bar{r_1}-\bar{r_4}\mid}+\frac{q_2q_4}{ 4\pi\epsilon_0\mid\bar{r_2}-\bar{r_4}\mid}+\frac{q_3q_4}{4\pi\epsilon_0\mid\bar{r_3 }-\bar{r_4}\mid} \label{eq4}\\ W_k&=&\frac{q_k}{4\pi\epsilon_0}\Sigma_{i=1}^{k-1}\frac{q_i}{\mid\bar{r_i}-\bar{ r_k}\mid} \label{eq5}\\ W&=&W_1+W_2+W_3+\ldots+W_n\\ \label{eq6} &=&\frac{1}{4\pi\epsilon_0}\sum_{k=1}^n\sum_{i=1}^{k-1}\frac{q_iq_k}{ \mid\bar{r_i}-\bar{r_k}\mid} \label{eq7}. \end{eqnarray}	AK-47	22-08-11 16:08:13	n

Convention about vectors is described. Different different symbols are used for vectors without reference to any axis, components of vector w.r.t. a system of coordinate axes, column vector notation for components

$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$
$\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$
$\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$
$\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$
$\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$
$\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$

$\newcommand{\xbf}{\bf x}$

This is page with text as well as a screen recording.
Screen recording of Problem Solving

TEACHING AND LEARNING

Quick Review of prerequisites
Kinematics in Different Coordinate Systems
Newton's Laws
Work and Energy
Simple Harmonic Motion, Small Oscillations
Noninertial Frames, Pseudo Forces
Centre of Mass and Linear Momentum
Rotational Motion
Decomposition of Kinetic Energy and Angular Momentum
Two Body Problem
Multi particle System
Kinematics of Rigid Body
Rigid Body Dynamics

Electric and Magnetic Fields
Electrostatics
Electric Potential and Electrostatic Energy
Conductors in Electric field
Maxwell's Equations in Dielectric
Boundary Value Problems in Presence of Dielectric Media
Magnetic Field
Magnetostatics of Magnetic Media
Electromagnetic Induction
Maxwell's Equations in Time Varying Situations
Electromagnetic Waves
Relativistic Electrodynamics
Potentials and Fields of a Moving Point Charge
Radiation

$\newcommand{\mid}{|}$

$\newcommand{\label}[1]{}$

\begin{eqnarray}
W_2&=&\frac{q_1q_2}{4\pi\epsilon_0\mid\bar{r_1}-\bar{r_2}\mid} \label{eq2}\\
W_3&=&\frac{q_1q_3}{4\pi\epsilon_0\mid\bar{r_1}-\bar{r_3}\mid}+\frac{q_2q_3}{
4\pi\epsilon_0\mid\bar{r_3}-\bar{r_2}\mid} \label{eq3}\\
W_4&=&\frac{q_1q_4}{4\pi\epsilon_0\mid\bar{r_1}-\bar{r_4}\mid}+\frac{q_2q_4}{
4\pi\epsilon_0\mid\bar{r_2}-\bar{r_4}\mid}+\frac{q_3q_4}{4\pi\epsilon_0\mid\bar{r_3
}-\bar{r_4}\mid} \label{eq4}\\
W_k&=&\frac{q_k}{4\pi\epsilon_0}\Sigma_{i=1}^{k-1}\frac{q_i}{\mid\bar{r_i}-\bar{
r_k}\mid} \label{eq5}\\
W&=&W_1+W_2+W_3+\ldots+W_n\\ \label{eq6}
&=&\frac{1}{4\pi\epsilon_0}\sum_{k=1}^n\sum_{i=1}^{k-1}\frac{q_iq_k}{
\mid\bar{r_i}-\bar{r_k}\mid} \label{eq7}.
\end{eqnarray}

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Browse & Filter

[MORE/EM-09001] Ballastic Galvanometer

[NOTES/ME-06003]-Time Period of Oscillations--Method-1

[NOTES/ME-02003]-Euler Angles

[NOTES/ME-02007]-Einstein Summation Convention

[NOTES/ME-02008]-Active and Passive Rotation

[NOTES/ME-02009]-Vectors as geometrical objects

[NOTES/ME-02011]-no title

[NOTES/ME-06001]- Application of Energy Conservation Law

[NOTES/ME-02010]-Rotation of Vector about an Arbitrary Axis

[NOTES/ME-06002]-Using graph of $V(x)$ to find motion

[NOTES/ME-06002b]-Using graph of $V(x)$ to find motion

[NOTES/ME-06001a]-Energy Conservation

[NOTES/ME-06001b]-Using energy conservation to reduce solution to quadratures

[LSN/ME-12002] Motion in Spherically Symmetric Potentials

Sample Video Page

Sample Video Page

[INDEX-TEACH&LEARN/ME] Newtonian Mechanics

[INDEX-TEACH&LEARN/ME] Newtonian Mechanics

[INDEX-TEACH&LEARN/EM] Electromagnetic Theory

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