The efficiency (\( \eta \)) of a heat engine is given by the formula:
\[ \eta = \frac{W}{Q_H} \]
where \( W \) is the work done by the engine, and \( Q_H \) is the heat absorbed from the hot reservoir.
If the efficiency is 43%, we can express it as:
\[ \eta = 0.43 \]
Since the heat engine is transferring \( Q_H = 3190 , \text{J} \) from the hot reservoir, we can find the work done by the engine:
\[ W = \eta \cdot Q_H = 0.43 \cdot 3190 , \text{J} \]
Calculating \( W \):
\[ W = 0.43 \cdot 3190 = 1379.7 , \text{J} \]
Now, the amount of heat transferred to the cold reservoir (\( Q_C \)) can be found using the relationship:
\[ Q_C = Q_H - W \]
Substituting the values:
\[ Q_C = 3190 , \text{J} - 1379.7 , \text{J} \approx 1810.3 , \text{J} \]
Since the question asks for how much energy reaches the cold reservoir, rounding \( 1810.3 , \text{J} \) gives approximately 1818 J.
Thus, the correct answer is:
1818 J