C C C C C ⎫ C D X Y Z ⎪ C = C + e + e , C = C − e , C = C − e , K = , K = , K = ⎪⎬ A, 0 A R1 R3 Y, 0 Y R2 Z, 0 Z R3 R1 C C R2 C C R3 C C ⎪ A B B C A X ⎭ and a set of unknown variables: > Vars := indets(Eqns,name); Vars := { C , C , C , C , C , C , C , C , C , C , e , e , e , C , C , C , C , K , K , K } C, 0 C D, 0 D X, 0 X B B, 0 A, 0 A R1 R2 R3 Y, 0 Y Z, 0 Z R1 R2 R3 The number of degrees of freedom follows directly > DegFree := nops(Vars)-nops(Eqns); Case 1 > Specs[1] := C[A,0]=1.5; > Specs[2] := C[B,0]=1.5; > Specs[3] := seq(C[i,0]=0,i=[C,D,X,Y,Z]); DegFree := 10 Specs := C = 1 A, 0 Specs := C = 2 B, 0 1.5 1.5 Specs := C = 0 , C = 0 , C = 0 , C = 0 , C = 0 3 C, 0 D, 0 X, 0 Y, 0 Z, 0 At <strong>the</strong> conditions of interest <strong>the</strong> reaction equilibrium coefficient has <strong>the</strong> following values > Kvals := {K[R1] = 1, K[R2]=2.63, K[R3]=5}; Kvals := { K = 1 , K = 2.63 , K = 5} R1 R2 R3 We now augment <strong>the</strong> set of equations with <strong>the</strong> set of specifications > AllEqns:=Eqns union {seq(Specs[k],k=1..3),op(Kvals)}; ⎧ ⎪ AllEqns := ⎪⎨ C = 1.5 , C = C − e + e , C = C − e , C = C − e + e , ⎪ B, 0 C, 0 C R1 R2 D, 0 D R1 X, 0 X R2 R3 ⎩ C = B, 0 + + C B e R1 C C C D e , C = C + e + e , C = C − e , C = C − e , K = , K = 1 , R2 A, 0 A R1 R3 Y, 0 Y R2 Z, 0 Z R3 R1 C C R1 A B C C C X Y Z K = 2.63 , K = 5 , K = , K = , C = 1.5 , C = 0 , C = 0 , C = 0 , C = 0 , R2 R3 R2 C C R3 C C A, 0 C, 0 D, 0 X, 0 Y, 0 B C A X ⎫ ⎪ C = 0⎪⎬ Z, 0 ⎪ ⎭ and ask <strong>Maple</strong> <strong>to</strong> solve <strong>the</strong> problem > result:=solve(AllEqns,Vars); result := { C = 0 , C = 0 , C = 0 , C = 0 , C = 0 , C = -.3879574470 , C = -.3207318471 , C, 0 D, 0 X, 0 Y, 0 Z, 0 B X C = 1.072193162 , C = 1.136496132 , e = 1.072193162 , %3 , C = .2564288777 , K = 5. , C = .8157642847 , D Z R1 C R3 Y e = 1.136496132 , e = .8157642847 , C = -.7086892941 , %2 , %1 , K = 1. } , { R3 R2 A R1 e = .9256703707 + .1402769617 I , C = 0 , C = 0 , C = 0 , C = 0 , C = 0 , %3 , K = 5. , R2 C, 0 D, 0 X, 0 Y, 0 Z, 0 R3 Page 22
C = .9256703707 + .1402769617 I , e = 1.727932631 + .1181659648 I , C = 1.727932631 + .1181659648 I , Y R3 Z e = .2016941637 − .07686691417 I , C = − .7239762070 − .2171438759 I , R1 C C = − .8022622599 + .02211099693 I , C = − .4296267943 − .04129905063 I , X A C = .3726354656 − .06341004756 I , C = .2016941637 − .07686691417 I , %2 , %1 , K = 1. } , { C = 0, B D R1 C, 0 C = D, 0 0 , C = 0 , C = 0 , C = 0 , %3 , K = 5. , e = 1.727932631 − .1181659648 I , X, 0 Y, 0 Z, 0 R3 R3 C = .3726354656 + .06341004756 I , C = − .7239762070 + .2171438759 I , C = − .8022622599 − .02211099693 I , B C X e = .9256703707 − .1402769617 I , e = .2016941637 + .07686691417 I , C = .9256703707 − .1402769617 I , R2 R1 Y C = − .4296267943 + .04129905063 I C = A D , .2016941637 + .07686691417 I , C = , Z 1.727932631 − .1181659648 I %2 , %1 , K = 1. } , { C = 0 , C = 0 , C = 0 , C = 0 , C = 0 , %3 , K = 5. , e = -.8625720556 , R1 C, 0 D, 0 X, 0 Y, 0 Z, 0 R3 R1 C = 3.783668561 , C = 2.489900223 , C = -.8625720556 , C = -1.421096505 , e = 2.489900223 , B Z D Y R3 e = -1.421096505 , C = -3.910996728 , C = .5585244494 , C = -.1273281670 , %2 , %1 , K = 1. } , { R2 X C A R1 C = C, 0 0 , C = 0 , C = 0 , C = 0 , C = 0 , %3 , K = 5. , e = .6779864947 − .06771720101 I , D, 0 X, 0 Y, 0 Z, 0 R3 R3 C = − .1082051188 − .6351221223 I , C = − .2577874160 + .03181297494 I , e = .6752088514 + .3334675486 I , B C R1 C = .9329962674 + .3016545737 I , e = .9329962674 + .3016545737 I , C = .1468046539 − .2657503476 I , Y R2 A C = .6752088514 + .3334675486 I , C = .2550097727 + .3693717747 I , C = .6779864947 − .06771720101 I , D X Z %2 , %1 , K = 1. } , { C = 0 , C = 0 , C = 0 , C = 0 , C = 0 , %3 , K = 5. , R1 C, 0 D, 0 X, 0 Y, 0 Z, 0 R3 e = .6779864947 + .06771720101 I , e = .6752088514 − .3334675486 I , C = .6779864947 + .06771720101 I , R3 R1 Z C = .6752088514 − .3334675486 I , C = .9329962674 − .3016545737 I , C = − .2577874160 − .03181297494 I , D Y C C = − .1082051188 + .6351221223 I C = B A , .1468046539 + .2657503476 I , e = , R2 .9329962674 − .3016545737 I %2 , %1 , C = .2550097727 − .3693717747 I , K = 1. } , { C = 0 , C = 0 , C = 0 , C = 0 , C = 0 , X R1 C, 0 D, 0 X, 0 Y, 0 Z, 0 %3 , K = 5. , %2 , %1 , K = 1. , C = .3630593987 , C = .5975408420 , e = .05222650742 , R3 R1 A X R1 C = -1.630028428 , e = 1.682254936 , C = 1.084714094 , C = .05222650742 , C = 1.682254936 , C R2 Z D Y C = -.2344814433 , e = 1.084714094 } , { C = 0 , C = 0 , C = 0 , C = 0 , C = 0 , %3 , K = 5. , B R3 C, 0 D, 0 X, 0 Y, 0 Z, 0 R3 %2 , %1 , K = 1. , C = .2474609670 , e = .7011220209 , C = .1766927072 , C = .4241536742 , R1 B R1 X A C = .7011220209 , C = .3747243049 , C = .5514170121 , e = .3747243049 , e = .5514170121 , D Z Y R3 R2 C = .1497050089} C %1 := C = 1.500000000 A, 0 %2 := C = 1.500000000 B, 0 %3 := K = 2.630000000 R2 Page 23
- Page 1 and 2: Maple Solutions to the Chemical Eng
- Page 3 and 4: The Van der Waals Equation of State
- Page 5 and 6: dimensionless form (in terms of the
- Page 7 and 8: lprint(`Reduced pressure is `, Pr);
- Page 9 and 10: Steady State Material Balances on a
- Page 11 and 12: set of independent equations for th
- Page 13 and 14: x = .54 , x = .35 , F x = F x + F x
- Page 15 and 16: and a cubic is > p(3); a + a T + a
- Page 17 and 18: -40 1000. 100. 10. -20 1. 20 40 60
- Page 19 and 20: -40 1000. 100. 10. -20 1. 20 40 60
- Page 21: ( Z, R1 ) = 0 ( D, R3) = 0 ( C, R2
- Page 25 and 26: Terminal Velocity of Falling Partic
- Page 27 and 28: Make a list of tank numbers > Units
- Page 29 and 30: Diffusion and Reaction in a One Dim
- Page 31 and 32: IC := {C[A](0)=0.2,y(0)=y0}; Alleqn
- Page 33 and 34: Kvalues := [seq(RAOULT(i),i=compid)
- Page 35 and 36: ead `c:/maple/numerics/newton.mpl`:
- Page 37 and 38: 108 106 104 102 100 98 96 0.4 0.5 0
- Page 39 and 40: ∂ 1 α( 1 + εX) T y = − ∂W 2
- Page 41 and 42: ∂ A ∂ DAEqns X = − = ∂W F
- Page 43 and 44: 0 -0.2 -0.4 -0.6 -0.8 5 W 10 15 20
- Page 45 and 46: deproc := proc(n,t,y,dy) local q,qs
- Page 47 and 48: params := { V = , , , , , , , } 400