The charge flowing through a resistance \( R \) varies with time as \( q = at - bt^2 \), where \( a, b \) are positive constants. The total heat produced in \( R \) is:
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To calculate the total heat produced in a resistor, use the formula \( H = \int I^2 R \, dt \), where \( I = \frac{dq}{dt} \).
The current is:
\[
I = \frac{dq}{dt} = a - 2bt
\]
The power dissipated is:
\[
P = I^2 R = (a - 2bt)^2 R
\]
The total heat produced is:
\[
H = \int P \, dt = \int (a - 2bt)^2 R \, dt = \frac{a^3 R}{6b}
\]
Thus, the total heat produced is \( \frac{a^3 R}{6b} \).