Electric field above the centre of a rectangle

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SUMMARY

The discussion centers on calculating the electric field above the center of a rectangle with dimensions 10 cm by 20 cm and a charge density of 4 μC/m². Participants utilize the formula for the electric field due to a line charge, E = 1/4πε₀ Q/r², and integrate over the rectangle's dimensions to find the resultant electric field at a height of 10 cm. The final electric field components are determined to be approximately 5.08 x 10⁵ N/C in the x-direction and 3.21 x 10⁵ N/C in the y-direction, leading to a total electric field vector at point P.

PREREQUISITES
  • Understanding of electric fields and charge distributions
  • Familiarity with integration techniques in physics
  • Knowledge of the formula for electric fields due to line charges
  • Basic concepts of vector addition in physics
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  • Study the derivation of the electric field from a finite line charge
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  • #61
That my answer is unreasonable because it is greater than that of the point charge calculation
 
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  • #62
says said:
That my answer is unreasonable because it is greater than that of the point charge calculation
Yes, there must be a mistake in your calculation for the rectangle. So, review the calculation to see if you can find an error. Could be a minor mistake somewhere.

Generally, it is a good idea to work the problem in symbols and wait until the end to plug in numbers.
 
  • #63
Ez = ∫ 2kλr / (y2+r2) [ 0.10 / (y2+r2+0.102)1/2 dy

k = 8.98*109
λ = 4*10-6
r = 0.10

Ez = ∫ 7184 / (y2+0.102) [ 0.10 / (y2+0.102+0.102)1/2 dy

Ez = ∫ 718.4 / (y2+0.01)(y2+0.02)1/2 dy

Ez = 71840tan-1(7.07107y / √(50y2+1))

substituting y=0.05 into the equation

Ez = 102149.75 N/C

I think of all the steps this may have been where the error is... Ez = ∫ 718.4 / (y2+0.01)(y2+0.02)1/2
 
  • #64
says said:
dEz = (kλdx / r2) z/r
Ez = 2kλz ∫ dx / (z2 + x2)3/2

where
z = √(y2+r2)

Ez = 2kλ/z[ x / (y2+r2) + x2)1/2] (bounds of integration are 0 and 0.10m)

Ez = 2kλr / (y2 + r2) [ 0.10 / ((y2+r2)+0.102)1/2]

k = 8.98*109
λ = 4.0*10-6
r = 0.10

Ez = 7184 / (y2 + 0.102) [ 0.10 / ((y2+0.102)+0.102)1/2]

Ez = [7184 / (y2 + 0.01)] [ 0.10 / ((y2+0.02)1/2]

Ez = ∫ [7184 / (y2 + 0.01)] [ 0.10 / ((y2+0.02)1/2] dy

Ez = 71840tan-1 [ 7.07107y / √(50y2+1)

Ez = 102149.75 N/C
I'm not sure, but it looks to me like you might have a mistake in plugging in the limits of y at the very end. You might check this.
 
  • #65
The limits of y are 0.05m and 0 though
 
  • #66
says said:
Ez = 71840tan-1(7.07107y / √(50y2+1))
I think this is OK.

substituting y=0.05 into the equation
Did you take care of both the upper and lower limits of y?

Ez = 102149.75 N/C
I don't get this answer when using your expression above with the limits for y.
 
  • #67
says said:
The limits of y are 0.05m and 0 though
Aren't the limits -0.05 m and + 0.05 m? Or did you replace the lower limit by 0 and include a factor of 2?
 
  • #68
Ez = 2kλr / (y2 + r2) [ 0.10 / ((y2+r2)+0.102)1]

I replaced the lower limit with 0 and included a factor of 2. :)
 
  • #69
says said:
I replaced the lower limit with 0 and included a factor of 2. :)
OK So, you would have

Ez = (2) 71840tan-1(7.07107(.05) / √(50(.05)2+1))

I don't get your answer when I evaluate this.
 
  • #70
TSny said:
OK So, you would have

Ez = (2) 71840tan-1(7.07107(.05) / √(50(.05)2+1))

I don't get your answer when I evaluate this.

I get 40378 N/C. Which is more reasonable.

If I've substituted 2 into the equation earlier though:

Ez = 2kλr / (y2 + r2) [ 0.10 / ((y2+r2)+0.102)1/2]

Should I be substituting 2 into the equation:

Ez = (2) 71840tan-1(7.07107(.05) / √(50(.05)2+1))

Or just leaving it as:

71840tan-1(7.07107(.05) / √(50(.05)2+1))
 
  • #71
You need to include the 2. This is the factor of 2 that comes from taking the lower limit to be 0.

Your answer of 40378 looks much better, but it is still different than what I'm getting. I get the argument of the inverse tangent function to be essentially 1/3. Do you agree?
 
  • #72
Yes. It's ~0.28
 
  • #73
says said:
Yes. It's ~0.28
I'm getting 0.3333, not 0.28.
 
  • #74
7.07107(.05) / √(50(.05)2+1)

0.3535535 / 1.125 = 0.3142

Closer. I'm not sure what happened with my first calculation...
 
  • #75
says said:
7.07107(.05) / √(50(.05)2+1)

0.3535535 / 1.125 = 0.3142

Closer. I'm not sure what happened with my first calculation...
The 1.125 is under a square root.
 
  • #76
says said:
If I've substituted 2 into the equation earlier though:

Ez = 2kλr / (y2 + r2) [ 0.10 / ((y2+r2)+0.102)1/2]

Should I be substituting 2 into the equation:

Ez = (2) 71840tan-1(7.07107(.05) / √(50(.05)2+1))

Or just leaving it as:

71840tan-1(7.07107(.05) / √(50(.05)2+1))
You did two integrations in which you replaced the lower limit with 0. So, overall, there will be two factors of 2.
 
  • #77
Ok, I get this now:

2*71840tan-1(0.333)
=46186 N/C
 
  • #78
OK, good.

If you are expected to round off to an appropriate number of significant figures, I'll let you think about that. But I agree with your answer now.
 
  • #79
How come the E field of an infinite sheet is much larger than the answer we calculated here? This perplexes me

E = λ / 2ε0

where
λ:charge density

E = 4*10-6 / [(2)(8.85*10-12)]
E = 225988 N/C
 
  • #80
says said:
How come the E field of an infinite sheet is much larger than the answer we calculated here? This perplexes me

E = λ / 2ε0

where
λ:charge density

E = 4*10-6 / [(2)(8.85*10-12)]
E = 225988 N/C
An infinite sheet at the same charge density is a lot more total charge!
OK, it's not as simple as that, but consider tiling the plane with 10cm x 20cm rectangles.
The point P is 10 cm from the sheet, and the centres of the next rectangles are, in one direction, only 40% further away. As you add in more surrounding tiles, is it that surprising that the total Ez field gets up to nearly 5 times as much?
 

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