Question #78936

I kg of a fluid expands reversibly according to a linear law from 4.2 bar to 1.4 bar; the initia] and final volumes are 0.004 m) and 0.02 m). The fluid is then cooled reversibly at constant pressure, and finally compressed reversibly according to a law po = constant back to the initial conditions of 4.2 bar and 0.004 m '. Calculate the work done in each process and the net work of the cycle. Sketch the cycle on a. p-v diagram,

Expert's answer

Answer on Question #78936, Physics / Molecular Physics | Thermodynamics

Question. 1kg1 \, kg of a fluid expands reversibly according to a linear law from 4.2 bar to 1.4 bar; the initial and final volumes are 0.004m30.004 \, m^3 and 0.02m30.02 \, m^3 . The fluid is then cooled reversibly at constant pressure, and finally compressed reversibly according to a law pV=constantpV = \text{constant} back to the initial conditions of 4.2 bar and 0.004m30.004 \, m^3 . Calculate the work done in each process and the net work of the cycle. Sketch the cycle on a pVp - V diagram.

Given. m=1m = 1 kg; p1=4.2p_1 = 4.2 bar =4.2105= 4.2 \cdot 10^5 Pa; p2=1.4p_2 = 1.4 bar =1.4105= 1.4 \cdot 10^5 Pa; V1=0.004V_1 = 0.004 m³; V2=0.02V_2 = 0.02 m³.

Find. W12,W23,W31,W?W_{12}, W_{23}, W_{31}, W - ?

Solution


W12W_{12} (area of the trapezoid) =12(p1+p2)(V2V1)=12(4.2105+1.4105)(0.020.004)=4480J= \frac{1}{2} (p_1 + p_2)(V_2 - V_1) = \frac{1}{2} (4.2\cdot 10^5 +1.4\cdot 10^5)(0.02 - 0.004) = 4480J

The work done by the fluid.


W23(a r e a o f t h e r e c t a n g l e)=p2(V3V2)W _ {2 3} (\text {a r e a o f t h e r e c t a n g l e}) = p _ {2} \left(V _ {3} - V _ {2}\right)p3V3=p1V1a n dp3=p2p _ {3} V _ {3} = p _ {1} V _ {1} \text {a n d} p _ {3} = p _ {2}V3=p1p2V1=4.21051.41050.004=0.012m3V _ {3} = \frac {p _ {1}}{p _ {2}} V _ {1} = \frac {4 . 2 \cdot 1 0 ^ {5}}{1 . 4 \cdot 1 0 ^ {5}} 0. 0 0 4 = 0. 0 1 2 m ^ {3}W23=1.4105(0.0120.02)=1120JW _ {2 3} = 1. 4 \cdot 1 0 ^ {5} (0. 0 1 2 - 0. 0 2) = - 1 1 2 0 J


The work done on the fluid.


W31=V3V1pdV=V3V1mMRTVdV=mMRTlnV1V3=p3V3lnV1V3=p1V1lnV1V3=4.21050.004ln0.0040.012==1845J\begin{array}{l} W _ {3 1} = \int_ {V _ {3}} ^ {V _ {1}} p d V = \int_ {V _ {3}} ^ {V _ {1}} \frac {m}{M} \frac {R T}{V} d V = \frac {m}{M} R T \ln \frac {V _ {1}}{V _ {3}} = p _ {3} V _ {3} \ln \frac {V _ {1}}{V _ {3}} = p _ {1} V _ {1} \ln \frac {V _ {1}}{V _ {3}} = 4. 2 \cdot 1 0 ^ {5} \cdot 0. 0 0 4 \cdot \ln \frac {0 . 0 0 4}{0 . 0 1 2} = \\ = - 1 8 4 5 J \\ \end{array}


The work done on the fluid.


W=W12+W23+W31=448011201845=1515JW = W _ {1 2} + W _ {2 3} + W _ {3 1} = 4 4 8 0 - 1 1 2 0 - 1 8 4 5 = 1 5 1 5 J


The work done by the fluid.

Answer. W12=4480JW_{12} = 4480J ; W23=1120JW_{23} = -1120J ; W31=1845JW_{31} = -1845J ; W=1515JW = 1515J .

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