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 \[ \boxed{17.2 \, \text{kJ}} \]
The internal energy of air in $ 4 \, \text{m} \times 4 \, \text{m} \times 3 \, \text{m} $ sized room at 1 atmospheric pressure will be $ \times 10^6 \, \text{J} $. (Consider air as a diatomic molecule)
An ideal gas has undergone through the cyclic process as shown in the figure. Work done by the gas in the entire cycle is _____ $ \times 10^{-1} $ J. (Take $ \pi = 3.14 $) 