Since the spheres attract initially, they carry charges of opposite nature, say q1 and q2. Magnitude of force, F=14πε0q1q2r2
Here,
r=25cm=25×10−2m
F=1.725 N
∴1.728=9×109q1q2(25×10−2)2
or q1q2=12×10−12 .....(1)
When the spheres are connected by a conducting connecting wire, charges on them redistribute so as to attain a common electric potential. If q′1 and −q′2 are the charges after redistribution, equality of electric potential requires
14πε0q′1r=14πε0q′1R
[Potential on surface V=14πε0qR′,where R is the radius]
Since there is no loss of charge during redistribution, the total charge on the system remains the same.
Here,
q′1+q′2=q1+(−q2)=q1−q1
but q′1=q′2
∴ q′1=q′2=q1−q22
The charges are now observed to repel with a force 0.576 N.
∴ 14πε0q′1+q′2r2=0.576
or
9×109(q1−q22)(25×10−2)2=0.576
∴ q1−q2=4×10−6 ....(2)
Substituting q2 from Eq. (2) in Eq. (1)
q1(q1−4×10−6)=12×10−12
q21−(4×10−6)q1−12×10−12=0
Solving, the roots are 6×10−6 C and −2×10−6 C
Hence, the two charges are 6×10−6 C and −2×10−6 C.