To calculate the change in internal energy of the system, we can use the first law of thermodynamics, which is given by the equation:
\[ \Delta U = Q - W \]
where:
- \(\Delta U\) is the change in internal energy,
- \(Q\) is the heat added to the system (negative when heat is removed),
- \(W\) is the work done by the system (positive when work is done on the system).
In this case:
- The system (the balloon) loses heat, so \(Q = -0.657 \text{ kJ} = -657 \text{ J}\) (since \(1 \text{ kJ} = 1000 \text{ J}\)).
- The atmosphere does work on the balloon, \(W = -385 \text{ J}\) (because work is done on the system).
Now we can plug these values into the equation:
\[ \Delta U = Q - W = (-657 \text{ J}) - (-385 \text{ J}) \]
This simplifies to:
\[ \Delta U = -657 \text{ J} + 385 \text{ J} = -272 \text{ J} \]
Now, we express the result in three significant figures:
\[ \Delta U = -272 \text{ J} \]
Thus, the change in internal energy of the system is:
\[ \Delta U = -272 \text{ J} \]