Magnitude of the electric field

AI Thread Summary
The discussion centers on calculating the electric field at the origin due to a uniformly charged semi-circular rod. The participants clarify the relationship between the length of the rod, the charge density, and the electric field components. The direction of the electric field is confirmed to be in the negative y-direction, with x-components canceling out. There is a focus on integrating the electric field contributions from small charge elements, with suggestions to express arc length in terms of angles for accurate integration. Overall, the calculations and relationships between variables are refined to arrive at the correct expression for the electric field.
Rijad Hadzic
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Homework Statement


http://imgur.com/a/g5acE

# 34

A plastic rod of length L = .24 cm is uniformly charged with a total charge of 12 x 10^-6 C.

The rod is formed into a semi circle with its center at the origin of the xy plane. What are the magnitude and direction of the electric field at the origin?

Homework Equations


kQ/r^2 = E

The Attempt at a Solution



Ok so can anyone tell me if this statement is correct:

1) Because I'm given L = .24 m, and the circumfrence of a circle is 2pir, since I have a semi circle I can set .24m = pi r, now r = .24m/pi

Going forward assuming that is true...:

The direction of the field is -j hat. Because the x components cancel out.

I consider a small piece of the rod I will call ds that has charge dQ. dQ = \Lambda ds correct?

Anyways the magnitude of the electric field at a, E, is going to be 2dEsin(theta) because its getting its Y component from both sides of the Y axis.so I have E = 2dEsin(theta)

dE = kdQ / r^2

so I have

E = 2*k*dq*sin(thetha) / r^2

but dQ = \Lambda ds

so

E = (2*k*\Lambda * ds * sin(theta) ) / r^2

now I integrate ds from 0 to (pi * r ) / 2

so I get (pi*r)/2 after integrating

E = (*k*\Lambda * sin(theta) * pi * r ) / r^2

pi * r * lambda are = Q, right?

so now I have

E = kQ sin(theta) / r^2

The reason sin(theta) wasn't in my integration was because the change of the angle has no impact on the E right?

But sin(theta) = y / r

so now I'm left with

E = kQy / r^3But I have a feeling this is wrong. I can plug in for k, Q, and r^3, I'm not really sure what to do with y...
 
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I think I'm wrong when I say that sin(theta) doesn't have an impact on E, because it does? Since the electric field is stronger as y is closer to 0?

So at the step

E = 2*k*\Lambda * sin(theta) / r^2 , I find sin(theta) to be = y/r, so I get E = 2*k*\Lambda * ds * y / r^3

but how am I suppose to integrate y and ds ??
 
Rijad Hadzic said:
1) Because I'm given L = .24 m, and the circumfrence of a circle is 2pir, since I have a semi circle I can set .24m = pi r, now r = .24m/pi
Yes.

The direction of the field is -j hat. Because the x components cancel out.
Yes

I consider a small piece of the rod I will call ds that has charge dQ. dQ = \Lambda ds correct?
Yes, assuming ##\Lambda## is the linear charge density.

Anyways the magnitude of the electric field at a, E, is going to be 2dEsin(theta) because its getting its Y component from both sides of the Y axis.

Putting in the factor of 2 here is not a good idea. You are considering one element of charge dQ.

so

E = (2*k*\Lambda * ds * sin(theta) ) / r^2

The left side would be ##dE_y## and you could add a negative sign to the right side to indicate that the y component is negative. Again, I would drop the factor of 2 here.

now I integrate ds from 0 to (pi * r ) / 2
The arc length s and the angle θ are related. So, you should be able to write ds in terms of dθ and integrate with respect to θ. It's at this point that you can put in a factor of 2 and integrate over half the semicircle.
 
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TSny said:
Yes.

The arc length s and the angle θ are related. So, you should be able to write ds in terms of dθ and integrate with respect to θ. It's at this point that you can put in a factor of 2 and integrate over half the semicircle.
ok so

dE = dE_y sin(thetha)

dE_y = (k)(\Lambda) (ds ) / r^2

dE = (k)(\Lambda) (ds ) sin(theta) / r^2

since s = (r)(theta) and ds = rdThetha

E = (k)(\Lambda) (2)\int {sin(thetha) d(theta)} / r ^2

int sin thetha = -cos evaluate from 0 to pi/2 you get one thus

E = (k)(\Lambda)(2) / r^2

correct??

set lambda = Q/L so i have

E = (k)(\Lambda)(2) / (r^2) (L)

I still feel like I am doing something wrong :(, am I?
 
Rijad Hadzic said:
ok so

dE = dE_y sin(thetha)
Shouldn't the symbols ##dE_y## and ##dE## be switched here?

since s = (r)(theta) and ds = rdThetha

E = (k)(\Lambda) (2)\int {sin(thetha) d(theta)} / r ^2
Looks like you forgot the r in rdθ.

int sin thetha = -cos evaluate from 0 to pi/2

you get one thus

E = (k)(\Lambda)(2) / r^2

correct??
You are off by a factor of ##r## on the right side.
set lambda = Q/L so i have

E = (k)(\Lambda)(2) / (r^2) (L)
You can express L in terms of r and simplify. Should that be ##\Lambda## or ##Q## in your final result?
You almost have it.
 
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