Step 1: Use the first law of thermodynamics.
The first law of thermodynamics states that the change in internal energy (\( \Delta U \)) is equal to the heat (\( Q \)) supplied to the system minus the work (\( W \)) done by the system:
\[
\Delta U = Q - W
\]
For an isobaric process (constant pressure), the work done is given by:
\[
W = P \Delta V
\]
where \( P \) is the pressure and \( \Delta V \) is the change in volume.
Step 2: Use the relationship for heat in an isobaric process.
The heat supplied in an isobaric process is related to the change in temperature by:
\[
Q = n C_P \Delta T
\]
where \( C_P \) is the specific heat at constant pressure and \( n \) is the number of moles of the gas.
Now, we know that:
\[
\Delta U = n C_V \Delta T
\]
and the relationship between \( C_P \) and \( C_V \) is:
\[
C_P = C_V + R
\]
where \( R \) is the universal gas constant.
Step 3: Apply the adiabatic constant.
For an ideal gas, the adiabatic constant \( \gamma \) is the ratio of the specific heats:
\[
\gamma = \frac{C_P}{C_V}
\]
Given that \( \gamma = 1.4 \), we can relate \( C_P \) and \( C_V \) to solve for the heat given to the gas.
The work done in an isobaric process is related to the heat supplied by:
\[
Q = W + \Delta U
\]
Substituting the values for \( W = 100 \, \text{J} \) and solving for \( Q \), we get:
\[
Q = 100 + 250 = 350 \, \text{J}
\]
Thus, the heat given to the gas is 350 J.