When you make ice cubes, the entropy of water
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Solution
Entropy (Δs) is the disorder, it decreases when water changes to ice-cube
ΔS = ΔQ⁄T
We consider a thermodynamic system. If ΔU represents the increase in its internal energy and W the work done by the system, which of the following statements is true?
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Solution
From first law of thermodynamics,
ΔH =Δu + w
In adiabatic process ΔH = 0
∴ Δu = – w
In a Carnot engine efficiency is 40% at hot reservoir temperature T.For efficiency 50%, what will be the temperature of hot reservoir?
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Solution
Which of the following statements about a thermodynamic process is wrong ?
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Solution
For adiabatic process Q = 0.
By first law of thermodynamics,
Q =ΔE + W
⇒ ΔEint= – W.
A system goes from A to B via two processes I and II as shown in figure. If ΔU1 and ΔU2 are the changes in internal energies in the processes I and II respectively, then
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Solution
Change in internal energy do not depend upon the path followed by the process. It only depends on initial and final states i.e.,
ΔU1 = ΔU2
In the given (V – T) diagram, what is the relation between pressure P1 and P2 ?
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Solution
A gas is taken through the cycle A→ B→ C→ A, as shown in figure. What is the net work done by the gas ?
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Solution
Wnet= Area of triangle ABC = 1⁄2AC × BC
= 1⁄2 × 5 × 10-3 × 4 × 105 = 1000 J
An ideal gas goes from state A to state B via three different processes as indicated in the P-V diagram :
If Q1, Q2, Q3 indicate the heat a absorbed by the gas along the three processes and ΔUQ1, ΔU2, ΔU2 indicate the change in internal energy along the three processes respectively, then
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Solution
Initial and final condition is same for all process
ΔU1 = ΔU2= ΔU3
from first law of thermodynamics
ΔQ= ΔU + ΔW
Work done
ΔW1 > ΔW2 > ΔW3(Area of P.V. graph)
So ΔQ1 > ΔQ2 > ΔQ3
A thermodynamic system is taken through the cycle ABCD as shown in figure. Heat rejected by the gas during the cycle is
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Solution
∵ Internal energy is the state function.
∵ In cyclie process; ΔU= 0
According to 1st law of thermodynamics
ΔQ = ΔU + W
So heat absorbed
ΔQ= W= Area under the curve
= – (2V) (P) = – 2PV
So heat rejected = 2PV
A mass of diatomic gas(γ= 1.4) at a pressure of 2 atmospheres is compressed adiabatically so that its temperature rises from 27°C to 927°C. The pressure of the gas in final state is
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Solution