An initially stress-free massless elastic beam has length $L$ and circular diameter $d\ll L$, with both ends fixed between rigid walls. Material constants are Young’s modulus E and thermal-expansion coefficient $\alpha$. When uniformly heated slowly, its buckling temperature rise is proportional to
Restrained expansion causes compression $N=EA\alpha\Delta T$. Fixed-fixed Euler buckling occurs at $N_{cr}=4\pi^2EI/L^2$. Equating them yields $\Delta T_{cr}=4\pi^2I/(A\alpha L^2)$. For a circular section, $I/A=d^2/16$, giving $\Delta T_{cr}=\pi^2d^2/(4\alpha L^2)$. With other parameters fixed, this is proportional to $d^2$, B.
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