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When the state of a system changes from `A` to `B` adiabatically the work done on the system is `322` joule. If the state of the same system is changed from `A` to `B` by another process, and heat required is `50` calories of heat is required then find work done on the system in this process? `(J = 4.2 J//cal)`

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To solve the problem step by step, we will use the first law of thermodynamics and the properties of internal energy. Here’s the detailed solution: ### Step 1: Understand the Adiabatic Process In the adiabatic process from state A to state B, the work done on the system is given as 322 joules. Since it is an adiabatic process, there is no heat transfer (ΔQ = 0). ### Step 2: Apply the First Law of Thermodynamics for the Adiabatic Process The first law of thermodynamics states: \[ \Delta Q = \Delta U + \Delta W \] Since ΔQ = 0 for the adiabatic process, we can write: \[ 0 = \Delta U + \Delta W \] This implies: \[ \Delta U = -\Delta W \] Given that the work done on the system (ΔW) is 322 joules, we have: \[ \Delta U = -322 \text{ joules} \] Thus, the change in internal energy (ΔU) is: \[ \Delta U = 322 \text{ joules} \] ### Step 3: Understand the Second Process In the second process from A to B, it is given that 50 calories of heat is required. We need to find the work done on the system in this process. ### Step 4: Convert Calories to Joules To convert the heat from calories to joules, we use the conversion factor: \[ 1 \text{ calorie} = 4.2 \text{ joules} \] Thus, for 50 calories: \[ \Delta Q = 50 \text{ calories} \times 4.2 \text{ J/cal} = 210 \text{ joules} \] ### Step 5: Apply the First Law of Thermodynamics for the Second Process Now, we apply the first law of thermodynamics again for the second process: \[ \Delta Q = \Delta U + \Delta W \] Substituting the known values: \[ 210 \text{ joules} = 322 \text{ joules} + \Delta W \] ### Step 6: Solve for Work Done (ΔW) Rearranging the equation to find ΔW: \[ \Delta W = 210 \text{ joules} - 322 \text{ joules} \] \[ \Delta W = -112 \text{ joules} \] ### Conclusion The work done on the system in the second process is: \[ \Delta W = -112 \text{ joules} \] This indicates that work is done by the system in the second process. ---

To solve the problem step by step, we will use the first law of thermodynamics and the properties of internal energy. Here’s the detailed solution: ### Step 1: Understand the Adiabatic Process In the adiabatic process from state A to state B, the work done on the system is given as 322 joules. Since it is an adiabatic process, there is no heat transfer (ΔQ = 0). ### Step 2: Apply the First Law of Thermodynamics for the Adiabatic Process The first law of thermodynamics states: \[ \Delta Q = \Delta U + \Delta W \] ...
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