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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 ) $\frac{\alpha_1 + \alpha_2}{2}, \alpha_1 + \alpha_2$
( B ) $\frac{\alpha_1 + \alpha_2}{2}, \frac{\alpha_1 + \alpha_2}{2}$
( 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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