The power dissipated in a resistor is given by the formula:
\[
P = \frac{V^2}{R}
\]
For two identical resistors, the heat produced in parallel and series configurations is as follows:
For parallel connection, the effective resistance is \( R_{\text{eff}} = \frac{R}{2} \), and the power is:
\[
P_{\text{parallel}} = \frac{V^2}{R/2} = 2 \frac{V^2}{R}
\]
For series connection, the effective resistance is \( R_{\text{eff}} = 2R \), and the power is:
\[
P_{\text{series}} = \frac{V^2}{2R}
\]
Now, the ratio of heat produced in parallel to series is:
\[
\frac{P_{\text{parallel}}}{P_{\text{series}}} = \frac{2 \frac{V^2}{R}}{\frac{V^2}{2R}} = 4
\]
Thus, the ratio of heat produced is \( 4 : 1 \).