Electric field of a continuously charged semicircle rod at center

AI Thread Summary
The discussion focuses on calculating the electric field at the center of a uniformly charged semicircular rod with a total charge of -7.50 µC. The electric field direction is established as pointing in the +x direction. The approach involves integrating the electric field contributions from small charge elements along the semicircle, taking into account the geometry of the setup. The calculations reveal that the x-component of the electric field cancels out to zero, while the y-component results in a non-zero value that can be expressed in terms of the charge density and radius. The final solution requires substituting the values for the radius and charge density to arrive at the electric field's magnitude and direction.
JosephK
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Homework Statement


A uniformly charged insulating rod of length 14.0 cm is bent into the shape of a semicircle. The rod has a total charge of -7.50\muC. Find (a) the magnitude and (b) the direction of the electric field at O, the center of the semicircle.


Homework Equations



d\overline{E} = \frac{k dq}{r^2}\widehat{r}


The Attempt at a Solution



This is a continuous charge distribution. The electric field points in the +x direction.

I made dq = \lambdad
and integrated
\overline{E} = \int\frac{k dq}{r^2}\widehat{r}

from 0 to l, where l is the length of the rod

This is incorrect because r is constant.
R can be found through geometry.

I did not understand how to use cos\theta.
I reasoned at the ends of the rod, the angle is 90.
I did not figure out what angle it is.
 
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Hi, if you don't mind, I made the effort to sketch your problem.
Now, if you take a look at the diagram, a small element of the field d\vec{E} is created by a minor element dl.
Since the rod's initial length was l, that remains the entire length of the arc. The radius of the circle is now, by l = pi*R, R = l/Pi;
A small element, a fraction of the semicircle is now, dl = R*d(theta);
Assuming a linear charge distribution: \lambda = \frac{Q}{l}, We arrive at the
following:
d\vec{E} = \frac{k}{r^2}dq, R is constant, as you said.
But there are components to the E field, on the x, y axes respectively, axes which can be chosed arbitrarily, but must be maintained.
Let's take, per convention, The horizontal as x, vertical as y(note, direction donward taken as positive!).
We then get dE_x = dE*cos(theta), dE_y = dE*Sin(theta).
Therefore:
<br /> \Large<br /> E_x = \displaystyle \int_0^E{dE\cos(\theta)} = \int_0^\pi{\frac{k\cos(\theta)}{R^2}\lambda R d\theta} = 0;<br />
<br /> \Large<br /> E_y = \displaystyle \int_0^E{dE\sin(\theta)} = \int_0^\pi{\frac{k\sin(\theta)}{R^2}\lambda R d\theta} = 2\frac{k}{R}\lambda<br />
Plug in R, and lambda above, and you're done!
Daniel
 

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