$A$ compressive force, $F$ is applied at the two ends of a long thin steel rod. It is heated, simultaneously, such that its temperature increases by $\Delta T$. The net change in its length is zero. Let $l$ be the length of the rod, $A$ its area of cross-section, $Y$ its Young's modulus, and $\alpha$ its coefficient of linear expansion. Then, $F$ is equal to

  • A
    $l^2 Y \alpha \Delta T$
  • B
    $l A Y \alpha \Delta T$
  • C
    $A Y \alpha \Delta T$
  • D
    $\frac{A Y}{\alpha \Delta T}$

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