Chargé is a commune in the Indre-et-Loire department in central France.
Chargé is a small town near Amboise. The Rock 'in Chargé festival has revitalized the village since 2006
I'm just going to skip some of the step since I only need help with understanding the last part.
After rearranging the equation stated at "Relevant equation" (and skipping some steps) we will get:
E * 4*pi*e0*R^2 = integral pv * 4*pi*R^2 dR
E = 1/(4*pi*e0*R^2) * 4*pi * integral pv*R^2 dR
E =...
There must be something I'm not understanding about capacitors in series.
I know that we can treat them as one equivalent capacitor with:
(1) with 1/Ceq,
(2) same Q as anyone of the capacitors,
(3) and add up the Vs for the sum total V across them.
If the equivalent capacitor (Ceq) would...
Hello guys!
When talking about electrochemistry what is the difference between saying "electron transfer" and "vectorial electron transfer". It seems to me that "vectorial electron transfer" is just another fancy way of saying "electron transfer" but I am not quite sure if there is a kind of...
I was wondering if there is a way to deduce the solution of the potential of a charge outside a sphere given by the image method, though Green functions. Because of a Dirichlet condition (GD(R,r')=0), I know that a solution can be written as GD=Go+L, where ∇2L=0. But in order to approach this...
So is it becouse the material or becouse the fact that the balloon is the object that moves and the hair is static. and does every two objects that been grabed together will nacessrly continues each other.
and also why does the minos of a bttary doesn't stick to the flower
Hi,
I have a charge q1 = -10 * 10^9. The the coordinatesare (3,4)m.
I found the electric field vector that is (-2160i -2880j) n/c.
My questions is if I add a charge q2 to the the coordinates(0,0) is the electric field stay the same?
Hello
So here is my question
Not so sure how to approach this question
This is what I have worked out so far which is the magnetic field strength of the solenoid, not sure if this comes in helpful though
Thanks for any help!
The correct answer is B, but I am not sure why.
I have a few confusions regarding this problem. First of all, I had thought that we cannot use Gauss' Law to determine the flux through a SIDE of a cube since Gauss' Law only works for SURFACES. How can we determine how an electric field pierces a...
The answer according to the key is C. I thought the answer would be E since the electric field inside a conductor is always zero. Can someone explain why the answer is C?
In my most recent post, I tried to investigate the V(r) verses “r” for several charge distributions on conductive paper. The discussion there made me realize that the common conductive paper activity is not suitable for doing that. Nevertheless, I am interested in doing projects where I can find...
I am needing clarification for a concept. I understand that electrons carry a negative charge and that protons carry a positive charge. I also understand that a plastic rod picks up electrons when I rub it with a piece of wool. From the conservation of charge, the piece of wool must have a...
"a charge smaller than e has not been found.
if one determines the amount of charge on any charged body like a
charged sphere or charged drop) or any charged particle
(like positron, a-particle)
or any ion, then its charge is always found to be an integral multiple of e,
i.e., e,3e; 4e,...
No...
My answer was +Q/3.
I was assuming that the charges would distributed themselves completely.
But, apparently, I'm wrong?
For example, if there were 12##e^-##s on Sphere C, then, in the first step in the system: the ##e^-##s would balance out until each sphere has 4 ##e^-##s each?
What am I...
Firstly, I would like to check if I drew the diagram correctly:
I'm unsure of the question's phrasing in this case.
Should if the drawing is correct,
(i)
When radius is 1cm, charge enclosed = -10mC
When radius is 3cm, charge enclosed is -10+10 +5? I'm unsure where the 5mC is here in this...
Since it is stated that ##E'_x = E_x##, I am going to set a special case where ##z' = z = 0##, ##E_x## in (5.10) reduces to,
##E_x = \frac{1}{4 \pi \epsilon_0}\frac{Q}{x^2}##
However, ##E'_x## in (5.13) reduces to,
##E'_x = \frac{1}{4 \pi \epsilon_0}\frac{Q}{\gamma^2 x'^2}##
There is an...
I have a question relating DAC architectures. The guts of the question are really to do with capacitors and charge. I want to see if my understanding is correct. This is not a homework question or anything, just thinking about how the circuit interacts.
Setup:
Consider the following setup...
Suppose we have an accelerometer carrying a charge. The charge density everywhere in the instrument is uniform, or at least what I mean to say is, the charge on any component is proportional to that component's mass. Now, in an inertial reference frame, we place the accelerometer in an electric...
I found two formulas to calculate the work done. One is with this path integral:
## W_{AB}## = W(## r_A,r_B ##)=q* ## \int_{r_A}^{r_B} E*dr ##
but here is the one I tried to use:
## W_{AB}## = q*Δ U = q*(## \frac {kQ} {r_A} ## - ## \frac {kQ} {r_B} ## )
Now here's my problem, what are...
I have in my notes the charge conjugation operator converts the spinnor into its complex conjugate ,
##
C\begin{pmatrix}
\varepsilon \\ \eta
\end{pmatrix}=\begin{pmatrix}
\varepsilon^{*}{} \\ \eta ^{*}
\end{pmatrix}##when applied to gamma matrix from dirac equation does it do the same...
Based on the conditions, I found that $$V(x)=\frac{a^2}{\pi^2} ρ_0sin(πx/a)$$ would be a solution to Laplace's equation for $$|x|\leq a$$
and $$V(x)=cx+d$$, where c and d are constants. From the boundary conditions, $$\frac{dV(a)}{dx}=\frac{a}{\pi} ρ_0cos(πa/a)=ac$$, $$c=\frac{a\rho}{\pi}$$ and...
This is not really homework, but I'm having trouble understanding it intuitively. I came across this when learning about the space charge layer of a diode. The solution I know simply uses the 1D form of Gauss's law: ##\vec{\nabla} \cdot \vec{E}## = ##\dfrac{\rho}{\epsilon_0}## becomes...
I first tried to use the Gauss' law equation E.A = q/ε0 to find the total charge enclosed. The answer came out to be q(enclosed) = 4πqε0e^(-4r). So for r approaching infinity, q(enclosed) approached 0.
Next, I tried the equation ∇·E = ρ/ε0, calculated rho to be -4qε0e^(-4r)/r^2 and total...
If for example I have two charged particles q_1 , q_2 with distance 'r' between them, then:
The potential energy that results from particle q_1 exerting force on particle q_2 is $$ k\frac{q_1 q_2}{r} $$
If I do the same process for particle q_2:
The potential energy that results...
I tried to calculate the time the charged particle will take to reach the plane using the a and using d=1/2at² and found the t to be equal to root(4εmd/σq).
I guess the time period of oscillation will be double of t (by symmetry), i.e. 2root(4εmd/σq). I don't know if this is correct.
[moderators note: moved from technical forum, so no template]
Summary: I can't tell where the mistake in my process is. The computer keeps telling me I am wrong.
The Question:
What is the electric field at point 1 in the figure? Give your answer in component form.(Figure 1)Assume that a =...
I am performing some calculations but struck with confusion whether I am doing it correct or wrong due to contradictions of these calculations on different calculators websites. I hope here someone will help me with the validation of my calculations.
Battery Capacity = 150 Ah
Battery...
Thus I assume that one slab has positive charge Q1
and the other slab has negative charge Q2 = -Q1
There are 4 cases for the electric field:
1. x <= -a
2. -a <= x <= 0
3. 0 <= x <= a
4. a <= x
The general case:
Charge Density ##\rho = \frac {Q} {V}##
Flux of E ##\phi_e = \oint \vec E \cdot d...
In most standard exposition of (the mean-field theory of) charge density wave (CDW), phase and amplitude fluctuations are introduced as the collective excitations. Kohn anomaly in the acoustic phonon dispersion is also mentioned as temperature goes from the above till the CDW transition...
I begin by calculating the flux to be the flux of the cylinders lateral surface, which equals E*2*pi*p*h (p is the radius)
The other two surfaces have E ortogonal to dA, so their flux is 0.
Using Gauss law together with the calculated flux above, I get
Flux = Q/e
Flux = E*2*pi*p*h
Solve for E...
I am trying to use the Method of images for this configuration, But somehow I don't know where should I put the imaginary charge. I know the on the surface of the conductor the potential must be zero and the imaginary charge should be other side of the conductor but that's all I cay..
Can I sum up the potential due to all positive line charges and all negative line charges separately, with the boundary condition being at the edge of my unit cell, the potential should be the same and inside the metal there is a contant potential?
Imagine a massless (or very light-weight) charge that is glued to a rod undergoing sinusoidal motion along an axis. The acceleration of this charge produces electromagnetic waves, which can be harvested for energy, and this energy can be used to power the continued sinusoidal motion as well as...
This is an online HW question so maybe my digits are just off from rounding or something, but I don't know why I am not finding the correct answer. I got Q = 6.9e-8 as the magnitude of charge on each plate.
I basically just needed to calculate the original capacitance of this capacitor using c...
I was not able to derive the charge on the capacitor. But then, I arbitrarily assumed ##\phi=B.A## (Dot product of Magnetic field and Area)
Then, proceeding as follows,
##\phi=BA\cos(\omega_0 t)##
##\frac{d\phi}{dt}=−BA\omega_0\sin(\omega_0 t)##
Now at ##t=0, \phi=BA\cos(0)=BA##
Therefore...
Step 1 make a graph y-axis = current in amperes and x-axis = time in seconds
step 2 beginning from 1A there is a slope of 1A/s for 4 seconds and then no change for another 3s
step 3 the amount of coulombs is equal to the area under that graph, so 27 coulombs? is it right?
Relevant Equations:
Angular momentum density stored in an electromagnetic field: $$\vec{l}_{em} = \epsilon_0[\vec{r} \times (\vec{E} \times \vec{B})]$$
Electric field of an electric charge: $$\frac{q_e}{4\pi\epsilon_0}\frac{r - r'}{|r - r'|^3}$$
Magnetic field of a magnetic charge...
So I was reading Jackson's discussion on Image charge method of a grounding sphere.
He first assumed an image charge q inside Sphere with radius a, so the potential for real change and image charge is .
The by set potential equal to 0 at x=a, he solved q' and y'
Then he can get potential...
The textbook says
' A conducting sphere shell with radius R is charged until the magnitude of the electric field just outside its surface is E. Then the surface charge density is σ = ϵ0 * E. '
The textbook does show why. Can anybody explain for me?
Setup: Let ##\hat{\mathbf{e}}_1,\hat{\mathbf{e}}_2,\hat{\mathbf{e}}_3## be the basis of the fixed frame and ##\hat{\mathbf{e}}'_1,\hat{\mathbf{e}}'_2,\hat{\mathbf{e}}'_3## be the basis of the body frame. Furthermore, let ##\phi## be the angle of rotation about the ##\hat{\mathbf{e}}_3## axis...
I'm not sure how to proceed with this, but here are my findings/hypothesis:
First we find the electric field contributed by the plate with ##E=\frac{\lambda}{2\pi r\epsilon_{0}}## where r=2?
After finding out the electric field, is it safe to assume I can find the acceleration of the point...
Okay, I am not even sure how to startr with this question. But here's my theory:
First I will need to the electric field produced by the ring using the formula:
##E = k\frac{\lambda a}{(x^2+a^2)^{3/2}}##
After finding out electric field produced by ring, am I supposed to find out the...