Electric field due to a flat hollow disk

madafo3435
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Homework Statement
A charge distribution with a uniform positive charge surface density + σ is formed by a circular section of radii R1 and R2.
Relevant Equations
Charges to continuous charge distributions
I would like if my procedure is correct ...

Due to the symmetry of the problem, I only worry about the vertical coordinate of the field, so I will work with the magnitude of the field, and I will treat the problem in polar coordinates.

##E= \int_{R_1} ^ {R_2} \int_{0} ^ {\pi} \frac {\sigma sen(\theta)}{4\pi \epsilon _0 r^2} rd\theta dr = \frac {\sigma}{4\pi \epsilon _0} \int_{R_1}^{R_2} \frac {2}{r} dr = \frac {\sigma}{2\pi \epsilon _0} ln(\frac {R_2}{R_1})##

## \therefore \vec{E} = \frac {\sigma}{2\pi \epsilon _0} ln(\frac {R_2}{R_1}) \hat{\jmath} ##
I attach a picture of the problem below.

Is this correct?
 

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It appears to me you are on the right track, but is the problem asking for the E field at the center of the semicircles?

Can you explain why sinθ and not cosθ?
 
CPW said:
It appears to me you are on the right track, but is the problem asking for the E field at the center of the semicircles?

Can you explain why sinθ and not cosθ?

Because the direction of ##\vec{E}## is given by ##cos(\theta )\imath + sen(\theta )\jmath ## and due to the fixedness and uniformity, the as a component in ##\imath ## total is canceled

Do you agree with me?
 
I agree. Nice work.
But with y-axis up in your figure, shouldn't you include a minus sign in your vector answer?
 
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CPW said:
I agree. Nice work.
But with y-axis up in your figure, shouldn't you include a minus sign in your vector answer?
Thanks for your appreciation
 

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