(a) [image:11_image58.emf]
Hear received by end $A$, for melting of ice
$Q_{A} = \frac{K\ A(400 - 0)t}{\lambda \bullet x} = m\ L_{ice}$ …(i)
Heat received by end $B$, for vaporization of water
$Q_{B} = \frac{K\ A(400 - 100)t}{(10 - \lambda)x} = m\ L_{vap}$ …(i)
Dividing both equation, $\frac{\frac{400}{\lambda \bullet x}}{\frac{300}{(10 - \lambda)x}} = \frac{L_{ice}}{\ L_{vap}}$
$\Rightarrow \frac{4}{3}\frac{(10 - \lambda)}{\lambda} = \frac{80}{540} \Rightarrow \lambda = 9$