Step 1: Recall the first law of thermodynamics.
\[
dU = \delta Q - p\,dV
\]
where \(U\) is internal energy, \(p\,dV\) is expansion work.
Step 2: Define enthalpy.
\[
H = U + pV \quad \Rightarrow \quad dH = dU + p\,dV + V\,dp
\]
At constant pressure, \(dp = 0\). Hence,
\[
dH = dU + p\,dV.
\]
Step 3: Connect with heat transfer.
From first law:
\[
dU = \delta Q - p\,dV.
\]
Substituting,
\[
dH = (\delta Q - p\,dV) + p\,dV = \delta Q.
\]
Step 4: Conclude.
Thus, in an isobaric process, heat added is equal to the enthalpy change.
\[
\boxed{\Delta Q_p = \Delta H}
\]
Step 5: Example check (ideal gas).
For 1 mole ideal gas at constant \(p\):
\[
\Delta H = nC_p\Delta T \quad \Rightarrow \quad Q_p = nC_p\Delta T.
\]
This matches the standard thermodynamic relation.