Step 1: Recall the formula for work done.
Work done at constant pressure is: \[ w = -P \Delta V \]
Step 2: Calculate the change in volume.
Initial volume = \(V_i = 8 \, \text{dm}^3\) Final volume = \(V_f = 4 \, \text{dm}^3\) \[ \Delta V = V_f - V_i = 4 - 8 = -4 \, \text{dm}^3 \]
Step 3: Substitute values.
Given pressure: \(P = 43 \, \text{bar}\) \[ w = - (43) \times (-4) \, \text{dm}^3 \cdot \text{bar} \] \[ w = 172 \, \text{dm}^3 \cdot \text{bar} \]
Step 4: Convert units.
Since \(1 \, \text{dm}^3 \cdot \text{bar} = 100 \, J\): \[ w = 172 \times 100 = 17200 \, J \] \[ w = 17.2 \, \text{kJ} \]
The work done is \[ \boxed{17.2 \, \text{kJ}} \]
Which of the following best represents the temperature versus heat supplied graph for water, in the range of \(-20^\circ\text{C}\) to \(120^\circ\text{C}\)? 
In the following \(p\text{–}V\) diagram, the equation of state along the curved path is given by \[ (V-2)^2 = 4ap, \] where \(a\) is a constant. The total work done in the closed path is: 