The charge flowing through a resistance R varies with time t as Q = at - bt-,where a and b are positive constants. The total heat produced in Ris (2016 NEET Phase- 1) O Mark for review later OPER

The charge flowing through a resistance R varies with time t as Q= at-bt^2 , where a and b are positive constants. The total heat produced in R is

The charge flowing through a resistance R varies with time t as Q = at - bt^(2) , where a and b are positive constants. The total heat produced in R is:

The charge flowing through a resistance R varies with time t as Q=at-bt^(2) , where a and b are positive constant. The total heat produced in R is

The charge flowing through a resistance R varies with time t as Q = at - bt^(2) . The total heat produced in R is

The charge flowing through a resistance R varies with time t as Q = at - bt^(2) . The total heat produced in R is

The charge flowing through a resistance R varies with time t as Q=at-bt^(2) , where a and b are positive constants The total heat produced in R is - (A) (a^3R)/(3b) (B) (a^3R)/(2b) (C) (a^3R)/(b) (D) (a^3R)/(6b)