At \( 4^\circ C \), water exhibits anomalous expansion, meaning that its volume does not change with temperature under constant pressure:
\[
\left( \frac{\partial V}{\partial T} \right)_P = 0
\]
Since the heat capacities are related by:
\[
C_P - C_V = - T V \left( \frac{\partial P}{\partial T} \right)_V \left( \frac{\partial V}{\partial T} \right)_P
\]
when \( \left( \frac{\partial V}{\partial T} \right)_P = 0 \), it follows that \( C_P = C_V \).