Answer:
From
figure \[\cos \theta
=\frac{l_{1}^{2}+l_{2}^{2}-l_{3}^{2}}{2{{l}_{1}}{{l}_{2}}}\]
or \[l_{1}^{2}+l_{2}^{2}-l_{3}^{2}=2{{l}_{1}}{{l}_{1}}\cos
\theta \]
Differentiating
both sides, we get
\[2{{l}_{1}}d{{l}_{1}}+2{{l}_{2}}d{{l}_{2}}-2{{l}_{3}}d{{l}_{3}}\]
\[=2{{l}_{2}}d{{l}_{1}}\cos
\theta +2{{l}_{1}}d{{l}_{2}}\cos \theta -2{{l}_{1}}{{l}_{2}}\sin \theta d\theta
\]
or \[{{l}_{1}}d{{l}_{1}}+{{l}_{2}}d{{l}_{2}}-{{l}_{3}}d{{l}_{3}}=({{l}_{2}}d{{l}_{1}}+{{l}_{1}}d{{l}_{2}})\]
\[\cos
\theta -{{l}_{1}}{{l}_{2}}\sin \theta \,\cos d\theta \]
When
rods are heated, their lengths are increased. The change in the lengths of the
rods is given by
\[d{{l}_{1}}={{l}_{1}}{{\alpha
}_{1}}\,\Delta T,\,d{{l}_{2}}={{l}_{2}}{{\alpha }_{1}}\Delta T\] and \[d{{l}_{3}}\]\[={{l}_{3}}{{\alpha
}_{2}}\Delta t\]
Also,
\[\theta ={{60}^{o}}\]
Put
these values in eqn. (i), we get
\[l_{1}^{2}{{\alpha
}_{1}}\Delta T+l_{2}^{2}{{\alpha }_{1}}\Delta T-l_{3}^{2}{{\alpha }_{2}}\Delta
T\]
\[=(l_{2}^{2}{{\alpha
}_{1}}\Delta T+l_{1}^{2}{{\alpha }_{1}}\Delta T)\cos
{{60}^{o}}-{{l}_{1}}{{l}_{2}}\sin {{60}^{o}}d\theta \]
Also
\[{{l}_{1}}={{l}_{2}}={{l}_{3}}=l\]
\[\therefore
\]\[2{{\alpha }_{1}}{{l}^{2}}\Delta T-{{\alpha }_{2}}{{l}^{2}}\Delta
T={{l}^{2}}{{\alpha }_{1}}\Delta T-\frac{{{l}^{2}}\sqrt{3}}{2}d\theta \]
or \[d\theta
=\frac{2({{\alpha }_{2}}-{{\alpha }_{1}})\Delta T}{\sqrt{3}}\]
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