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author | priyanka | 2015-06-24 15:03:17 +0530 |
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committer | priyanka | 2015-06-24 15:03:17 +0530 |
commit | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (patch) | |
tree | ab291cffc65280e58ac82470ba63fbcca7805165 /572/CH3/EX3.7/c3_7.sce | |
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initial commit / add all books
Diffstat (limited to '572/CH3/EX3.7/c3_7.sce')
-rwxr-xr-x | 572/CH3/EX3.7/c3_7.sce | 50 |
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diff --git a/572/CH3/EX3.7/c3_7.sce b/572/CH3/EX3.7/c3_7.sce new file mode 100755 index 000000000..1bcfaf5d3 --- /dev/null +++ b/572/CH3/EX3.7/c3_7.sce @@ -0,0 +1,50 @@ +//(3.7) One pound of air undergoes a thermodynamic cycle consisting of three processes.Process 1ā2: constant specific volume Process 2ā3: constant-temperature expansion Process 3ā1: constant-pressure compression. At state 1, the temperature is 300K, and the pressure is 1 bar. At state 2, the pressure is 2 bars. Employing the ideal gas equation of state, (a) sketch the cycle on pāv coordinates. (b) determine the temperature at state 2, in K; (c) determine the specific volume at state 3, in m3/kg.
+
+//solution
+
+//variable initialization
+T1 = 300 //temperature in state 1 in kelvin
+P1 = 1 //pressure in state 1 in bar
+P2 = 2 //pressure in state 2 in bar
+
+R = 287 //gas constant of air in SI units
+v1 = (R*T1)/(P1*10^5) //specific volume in state 1
+P = linspace(1,2,100)
+for i = 1:100
+ v(1,i) = v1
+end
+
+plot2d(v,P,rect=[0,0,5,2.5]);
+
+T2 = (P2*10^5*v1)/R
+v3 = (R*T2)/(P1*10^5)
+vv = linspace(v1,v3,100)
+plot(vv,P1)
+
+function[out]= f(inp)
+ out = (R*T2)/inp
+endfunction
+
+VV = linspace(v1,v3,100)
+for j = 1:100
+ pp(1,j) = f(VV(1,j))/(10^5)
+end
+plot2d(VV,pp)
+xtitle("","v","p(bar)")
+
+printf('the temperature in kelvin in state 2 is:\n\t T2 = %f',T2)
+printf('\n\nthe specific volume in state 3 in m^3/kg is \n\t v = %f',v3)
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