Heat produced in a wire of resistance $R$ due to current flowing at constant potential difference is proportional to
A$\frac{1}{{{R^2}}}$
B$\frac{1}{R}$
C$R$
D${R^2}$
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B$\frac{1}{R}$
b (b) At constant p.d., heat produced $ = \frac{{{V^2}}}{R}\,i.e.\,H \propto \frac{1}{R}$
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