integrate that shit you raging fucking nigger faggot! the direction should be obvious from the symmetry of the semicircle. the field will go directly away from it. any field perpendicular to that will be canceled out by the other side of the semicircle. so you only have to work for one component of the field.
also, eat a dick and do you own homework.
also, saging the top thread
also, you're a nigger.
also, bahhh i dunno
fuck off
Name:
Anonymous2009-09-20 23:40
I haven't done something like this since mid last semester, but I assume this is an integration problem.
Consider a small segment of the charge bar dQ. dQ will equal the total charge Q times the fraction of the total arc it encompases, or dθ/π (dQ = dθ/π). Then consider the electric field from a similar infinitesimal segment of the bar, or dE = kdQ/|r|² * (-r^), where E and r are vectors. |r| = 0.14 m and -r^ = cosθ(-i) + sinθ(-j), so we get dE = -kdQ/0.14² * [cosθ(i) + sinθ(j)], and to simplify the RHS we get -0.14²dE/k = [cosθ(i) + sinθ(j)]*dQ.
Recall dQ= Q*dθ/π, so we get 0.14dE/kQ = cosθdθ/π(i) + sinθdθ/π(j)
We then integrate from θ = 0 to θ = π, so...
-0.14²E/kQ = [sin(π)/π - sin(0)/π](i) + [-cos(π)/π + cos(0)/π](j)
-0.14²E/kQ = [0/π - 0/π](i) + 1/π * [1+1](j)
-0.14²E/kQ = 0(i) + 2/π (j)
E = -2kQ/πr² (j) => E = -2(8.99*10^9)(-7.50*10^-6)/(0.14²π)(j), which will be positive, meaning the positive test charge in the middle of the semicircle would be attracted straight towards the point of the circle directly 'above' it.