Find the charge Q that should be placed at the centre of a square of side 6.20 cm with four identical positive charges of 1.40 µC at each corner, so that the whole system is in equilibrium.
take the top left particle then the force exerted on it due to
the top right charge is:
F(tr) = k*q^2 / r^2 - to the left ;
where k is 1/(4*Pi*s) I've used s to denote the permittivity of
free space, and k is approx = 8.988*10^9Nm^2/c^2. And r = the
distance between the charges.
Now due to the bottom left charge it is F(bl) = k*q^2 / r^2 -
upwards.
The resultant of these two forces is F(1) = sqrt( F(tr)^2+F(bl)^2
)
F(1) = sqrt( 2(k*q^2 / r^2 )^2) = sqrt(2)*k*q^2 / r^2 -
up/left
Now we also have the bottom right charge. If the distance to this
charge is R then R = sqrt(r^2+r^2) = sqrt(2)*r
so F(br) = k*q^2 / R^2 = k*q^2 / 2r^2 - up/left
which is the same direction as F(1)
Therefore the overall force on the top teft charge is
F = F(1) + F(br)
F = [sqrt(2)*k*q^2 / r^2] + [k*q^2 / 2r^2]
F = [(2sqrt(2)+1)*k*q^2] / 2r^2
This is the same force experienced by all the q-charges due to the
other q charges
Now for Q the force it excerts of the top left q must be of equal
magnitude but in the opposite direction. Since it is
at the centre of the square and since the force vectors due to the other q's are pointing away from the centres we
know that Q must be negaitive. Since we know this we can simply
find the magnitude of Q by:
Now F(Q) = F
However the distance to Q = 1/2 the distance to the bottom right q; So r(Q) = sqrt(2)*r / 2
k*q*Q / (sqrt(2)*r/2)^2 = [(2sqrt(2)+1)*k*q^2] / 2r^2
Simplifying: 4Q / 2r^2 = (2sqrt(2)+1)*q / 2r^2
Q = [2sqrt(2)+1]*q/4
Q = [2sqrt(2)+1]*(1.40*10^-6)/4 = 1.33*10-6
However we said Q must be negative, so
Q = 1.33uC
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