If I is the current passing through a metallic resistor and H is the rate of Heat generated in the resistor at a constant temperature, then
A
H \(\alpha\) \(\frac{1}{I}\)
B
H \(\alpha\) \(\frac{1}{I^2}\)
C
H \(\alpha\) \(\sqrt1\)
D
H \(\alpha\) I2
E
none of the above