Gaussian infinite sheet, electric field

In summary: How many regions does the space to the right of the far right plate cover?In summary, three thin charged sheets with different charge densities are placed parallel to each other. The electric field in regions A and B can be found by summing the electric field of each individual sheet. The distance between the sheets does not affect the electric field. For the potential difference between the two outer sheets, the distance between the sheets does matter and the electric field from all sheets must be taken into account. The final answer for the potential difference is -8.46*10^12 volts.
  • #1
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Homework Statement


three thin charged sheets are placed parallel to each other as shown:

far left sheet, charge density = +10C/m^2
middle sheet, charge density = -25C/m^2
far right sheet, charge density = -10C/m^2

|<--2m (A) -->|<-----4m (B) ------>|

a) what is the electric field in regions A and B?
b) what is the difference in potential between the two outer sheets? neglect thickness of sheets

Homework Equations



electric field at conductor surface = sigma/epsilon_o where sigma = charge density, epsilon_o = 8.85*10^-12 constant

electric flux = E (*) A where (*) is dot product, E is electric field, A is area of surface

charge enclose q_encl = sigma*A

The Attempt at a Solution



i've only tried part a:

what does it mean in the regions A and B, do i find the electric field of each sheet and then sum them up? how do distances between sheets factor in?

find the electric flux of the far left sheet, which is circle through the center of the sheet a la cookie cutter, and since there are two sides, there are two areas

electric flux = 2AE
sigma = +10C/m^2
q_encl = 10(2A)

let electric flux = q_encl/epsilon_o
so 2AE = sigma*A/epsilon_o ---> E = sigma/ 2*epsilon_o = 10/(2(8.85*10^-12)) = 5.65*10^11 N/C

that was the electric field for the far left sheet, i would do the same thing for the middle sheet but do i need to it to the far right sheet too for part a?

electric field middle sheet = -25/(2(8.85*10^-12)) = -1.41*10^12 N/C

electric field far right sheet = -10/(2(8.85*10^-12)) = -5.56*10^12 N/C

so the electric field for a and b = electric field( far left + middle + far right) = -1.41*10^12 N/C

how do the distances between the sheets come into play? ---> the 2m and 4m

also could you give me a quick run down on what i need to do for part b.

for part b since deltaV = -[integral(E*dr)] from r_a to r_b. do i let r_a = 0m and r_b = 6m ?

thanks
 
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  • #2
The strength of the electric field outside the infinite sheet is independent of the distance from the sheet. So the distance between the sheets doesn't matter when you are computing the E field. All you have to do is make sure you add the E fields in the correct directions. And, yes, for the potential difference the distance do matter. You integrate the E field over the separation between the sheets.
 
  • #3
part b:

since electric potential difference V_ab = -[integral(E_net*dr)] from r_b to r_a where r_b = 6m, r_a = 0m and E_net = -1.41*10^12

V_ab = -1.41*10^12(6 - 0) = -8.46*10^12 volts

correct?
 
  • #4
You need to combine the electric field from ALL of the sheets. There are four different regions that could have four different E fields. Do they? What is it in each region? How many regions does the space between the two outer plates cover?
 

What is a Gaussian infinite sheet?

A Gaussian infinite sheet is a theoretical model used in physics to represent a thin, infinitely large sheet with a uniform distribution of electric charge. It is often used as a simplified model to study the behavior of electric fields and their interaction with other charged objects.

What is an electric field?

An electric field is a physical field that surrounds electrically charged particles and exerts a force on other charged particles within its reach. It is represented by vectors that describe the direction and magnitude of the force at any given point.

How is the electric field calculated for a Gaussian infinite sheet?

The electric field for a Gaussian infinite sheet can be calculated using Gauss's Law, which states that the electric flux through a closed surface is equal to the charge enclosed by that surface divided by the permittivity of free space. For an infinite sheet, the electric field is constant and perpendicular to the sheet's surface, and its magnitude is equal to the surface charge density divided by the permittivity of free space.

What is the direction of the electric field for a Gaussian infinite sheet?

The electric field for a Gaussian infinite sheet is always perpendicular to the surface of the sheet. This means that the electric field lines are parallel to each other and extend infinitely in both directions away from the sheet.

How does the electric field vary with distance from a Gaussian infinite sheet?

The electric field strength decreases with distance from a Gaussian infinite sheet. The electric field is inversely proportional to the distance from the sheet, meaning that the farther away an object is from the sheet, the weaker the electric field will be. However, the direction of the electric field remains the same regardless of the distance from the sheet.

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