The charge flowing through a resistance R varies with time t as Q=at-bt2 where a and bare positive constants. The total heat produced in R is
a3R2b
a3Rb
a3R6b
a3R3b
Given, Q=at-bt2∴I=dQdt=a-2bt
At t=0,Q=0, I=a
Also, I=0 at t=a/2b
Total heat produced in resistance R,
H=∫0a/2bI2Rdt=R∫0a/2b(a-2bt)2dt
=R∫0a/2ba2+4b2t2-4abtdt=Ra2t+4b2t33-4abt220a/2b
=Ra2×a2b+4b23×a38b3-4ab2×a24b2=a3Rb12+16-12=a3R6b