Electric field of a continuously charged semicircle rod at center

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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 and a length of 14.0 cm. The electric field is derived using the formula dE = (k dq) / r², where dq is expressed in terms of linear charge density (λ). The analysis reveals that the electric field points in the +y direction, with the x-component canceling out due to symmetry, resulting in E_y = 2(k/R)λ after integration. The radius R is determined geometrically as R = l/π.

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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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