Step 1: Understanding the Concept
At constant pressure, heat supplied is \(Q=nC_p\Delta T\), while the rise in internal energy is \(\Delta U=nC_v\Delta T\).
Step 2: Fraction
\(\dfrac{\Delta U}{Q}=\dfrac{C_v}{C_p}=\dfrac{1}{\gamma}\).
Step 3: Calculation
For a monatomic gas \(\gamma=\dfrac{5}{3}\), so the fraction is \(\dfrac{3}{5}\). The remaining \(\dfrac{2}{5}\) is spent as work of expansion.
Final Answer:
The fraction of heat that increases internal energy is 3/5.
\[ \boxed{\text{(A) }\dfrac{3}{5}} \]