Surface charge density due to point charge

AI Thread Summary
The discussion focuses on solving a problem involving surface charge density using the method of images. Participants express confusion over the lecturer's solution, particularly regarding the disappearance of the factor of 2sinθ and the role of ε in calculating surface charge density. It is clarified that the electric fields from both real and imaginary charges contribute to the overall field, and the vertical components combine due to their direction. The relationship between the electric field and surface charge density is highlighted, emphasizing the use of Gauss's theorem. Overall, the method of images is confirmed as a valid approach for this type of problem.
NewtonianAlch
Messages
453
Reaction score
0

Homework Statement


Using the method of images, solve the following

image.jpg

The Attempt at a Solution



I have very little idea on how to solve this. I looked up various methods online and none seem to be what the lecturer has used.

This is the solution he posted up, but as usual it is missing 300 steps and also seems to differ to the short answer he has given in the actual problem sheet, although I figured because of the 2 sin θ, the 2 and 4 cancel, leaving only 2 at the bottom. And ε disappears because for finding ρ (surface charge density) we multiply the E-field by ε.

However I don't understand how a 2sinθ came to be and then abruptly disappears.

Any help appreciated.

image.jpg
 
Physics news on Phys.org
The electric fields from the two charges (the real and the imaginary one) go along the lines in the sketch (one is marked with "E". The magnitude is calculated with the usual formula, and their vertical component is sin(theta) of their magnitude. You have two charges, both have their vertical component in the same direction, therefore you get a factor of 2 there.

To get rid of the angle, he uses sin(theta)=d/R. You can see the d in the numerator, and R is converted to sqrt(d^2+r^2) in the denominator. The factor of 2 seems to be missing there.
And ε disappears because for finding ρ (surface charge density) we multiply the E-field by ε.
Right.
 
If I may add, and pardon if it's superfluous info:
Two main ideas here:

1. E field just above a conducting surface is εE = σ where σ is surface charge density. The direction of E is normal to, and away from, the conductor if the surface charge density is +. This is easily shown using Gauss's theorem. If the surface charge is -, then the direction is into the plane.

2. The concept of imaging which is as shown on the proffered answer sheet. The basis is that the potetial anywhere along the sheet is constant (equipotential surface) if the image charge is added and the presence of the sheet ignored.
 
Thanks for the responses, I understand it clearly now!
 
TL;DR Summary: I came across this question from a Sri Lankan A-level textbook. Question - An ice cube with a length of 10 cm is immersed in water at 0 °C. An observer observes the ice cube from the water, and it seems to be 7.75 cm long. If the refractive index of water is 4/3, find the height of the ice cube immersed in the water. I could not understand how the apparent height of the ice cube in the water depends on the height of the ice cube immersed in the water. Does anyone have an...
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
Back
Top