Two conductors have the same resistance at $0\,^{\circ}C$ but their temperature coefficients of resistance are $\alpha_1$ and $\alpha_2$. The respective temperature coefficients of their series and parallel combinations are nearly

  • A
    $\frac{\alpha_1 + \alpha_2}{2}, \frac{\alpha_1 + \alpha_2}{2}$
  • B
    $\frac{\alpha_1 + \alpha_2}{2}, \alpha_1 + \alpha_2$
  • C
    $\alpha_1 + \alpha_2, \frac{\alpha_1 + \alpha_2}{2}$
  • D
    $\alpha_1 + \alpha_2, \frac{\alpha_1 \alpha_2}{\alpha_1 + \alpha_2}$

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