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A line of positive charge is formed into a semicircle of radius R 80.0 cm, as shown in the figure below. The charge per unit length along the semicircle is given by the expression λ-, cos@). The total charge on the semicircle is 13.0 μC. Calculate the total force on a charge of 2.00 μC placed at the center of curvature magnitude direction Select
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Answer #1

The total charge on the semi circle is given to be  13mu C.

That is  C=int lambda dl

lambda=lambda _{0}cos( heta )

dl = rde

C=int lambda _{0}cos( heta )rd heta

For one quadrant (ie from y axis to x axis), since the charge distribution is dependent on theta, we can find the charge in one half of this semi cirlce and then multiply it with 2 to get the total charge.

so

13

13 1.6 8 = 0

13

Now, the x component of the force experienced by the 2mu C by the component of the semi circle to the left of y axis and to the right of y axis will be the same, but in opposite direction. Therefore, they will cancel out each other. So only the y component of the force will remain( this is because cos(-0) cos(θ) but sin(- heta )=-sin( heta ) , thus cancels each other out).

The y component force is given by the equation

F_{y}=int rac{1}{4pi epsilon _{0}}rac{lambda dl*2.00mu C}{R^{2}}cos( heta)

cos (0)do 4TE0 here we substituted the value for dl as we took earlier.

* 1.6 * 0.8]· (1 + cos20)

solving, we get

F_{y}=0.8281N

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