
dϕ=2πyμ0iady
ϕ=2πμ0ia∫xx+aydy=2πμ0ia[ln(x+a)−lnx]
E.m.f=−dtdϕ=−2πμ0ia[x+a1dtdx−x1dtdx]
=2πμ0iax(x+a)a.v=2πμ0.x(x+a)ia2v=2×10−7×0.1×0.21×(0.12×10)=1μV
Alternative method:
Consider two sides which are perpendicular to the velocity as case of motional e.m.f.

E=E1−E2=(B1–B2)Vl
=2πμ0I(x1−x+a1)Vl
=2×10−7×1(0.11−0.21)×10×0.1
=10−6V=1μV