We are given that ice and water are in equilibrium at 273.15 K and 1 atm pressure. This is the melting point of ice.
The Clausius-Clapeyron equation describes the relationship between pressure and temperature for phase transitions:
$$ \frac{dP}{dT} = \frac{\Delta H}{T \Delta V} $$
For the ice-water transition, $ \Delta H $ is the enthalpy of fusion (positive), and $ \Delta V = V_{\text{water}} - V_{\text{ice}} $. Since ice is less dense than water, $ V_{\text{ice}} > V_{\text{water}} $, so $ \Delta V < 0 $.
Therefore, $ \frac{dP}{dT} < 0 $. This means that an increase in pressure will lower the melting point of ice.
Since the temperature is kept constant at 273.15 K and the pressure is increased, the ice will start to melt to form water. This is because at the higher pressure, the temperature is above the new melting point.
Conclusion: The amount of ice will decrease.
Final Answer:
The final answer is $ \text{The amount of ice decreases.} $
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is: