Step 1: The energy lost by the metal block will be used to melt the ice. The energy lost by the metal block is given by: \[ Q_{\text{metal}} = m \cdot c \cdot \Delta T \] where \( m = 120 \, g \), \( c = 0.12 \, cal/g ^\circ C \), and \( \Delta T = 100 ^\circ C - 0 ^\circ C = 100 ^\circ C \). \[ Q_{\text{metal}} = 120 \times 0.12 \times 100 = 1440 \, \text{cal} \]
Step 2: The energy required to melt the ice is: \[ Q_{\text{ice}} = m_{\text{ice}} \cdot L_f \] where \( L_f = 80 \, \text{cal/g} \) is the latent heat of fusion and \( m_{\text{ice}} \) is the mass of the ice melted.
Step 3: Since all the energy from the metal is used to melt the ice: \[ 1440 = m_{\text{ice}} \times 80 \] \[ m_{\text{ice}} = \frac{1440}{80} = 18 \, \text{g} \]
If the interval in which the real-valued function \[ f(x) = \log\left(\frac{1+x}{1-x}\right) - 2x - \frac{x^{3}}{1-x^{2}} \] is decreasing in \( (a,b) \), where \( |b-a| \) is maximum, then {a}⁄{b} =