(c) On keeping the temperature of the ends of tube at 0$℃$ and 273$℃$.
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Applying ideal gas equation
$\frac{p_{1}V_{1}}{T_{1}} = \frac{p_{2}V_{2}}{T_{2}} = \frac{p_{3}V_{3}}{T_{3}}$
$\frac{76 \times 45}{(273 + 31)} = \frac{p_{2} \times l}{(273 + 0)} = \frac{p_{3}(90 - l)}{273 + 273}$
$\frac{76 \times 45}{304} = \frac{p_{2} \times l}{273} = \frac{p_{3}(90 - l)}{546}$
I II III
From II and III
$\frac{p_{2} \times l}{273} = \frac{p_{3}(90 - l)}{546}$
(Mercury column is at rest, so pressure
difference $p_{2} - p_{3} = 0\ \Rightarrow p_{2} = p_{3})$
$\therefore$ $\frac{p_{2} \times l}{273} = \frac{p_{2}(90 - l)}{546}$
$\Rightarrow \ \ \ \ \ \ \ 2l = 90 - l\ \Rightarrow l = 30$ cm
From I and II
$\frac{76 \times 45}{304} = \frac{p_{2} \times 30}{273}$
$\Rightarrow \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ p_{2} = \frac{76 \times 45 \times 273}{30 \times 304}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ p_{2} = 102.4$