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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 /497/CH12/EX12.4/Chap12_Ex4.sce | |
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diff --git a/497/CH12/EX12.4/Chap12_Ex4.sce b/497/CH12/EX12.4/Chap12_Ex4.sce new file mode 100755 index 000000000..77c4e6ec6 --- /dev/null +++ b/497/CH12/EX12.4/Chap12_Ex4.sce @@ -0,0 +1,31 @@ +//Kunii D., Levenspiel O., 1991. Fluidization Engineering(II Edition). Butterworth-Heinemann, MA, pp 491
+
+//Chapter-12, Example 4, Page 305
+//Title: Reaction in the Slow Bubble Regime
+//==========================================================================================================
+
+clear
+clc
+
+//INPUT
+uo=0.25;//Superficial gas velocity in m/s
+db=0.025;//Equilibrium bubble size in m
+Kr=1.5;//rate constant in m^3 gas/m^3 cat s
+umf=0.21;//Velocity at minimum fluidization condition in m/s
+Lm=0.8;//Length of the bed in m
+ephsilonm=0.42;//Void fraction of fixed bed
+g=9.81;//Acceleration due to gravity in square m/s^2
+
+//CALCULATION
+ubr=0.711*(g*db)^0.5;//Rise velocity of bubble from Eqn.(6.7)
+ub=uo-umf+ubr;//Velocity of bubbles in bubbling beds in Eqn.(6.8)
+delta=(uo-umf)/(ub+2*umf);//Fraction of bed in bubbles from Eqn.(55) since ub/umf<<1
+XA=1-exp(-Kr*Lm*((1-ephsilonm)/uo)*(umf/uo)*(1-delta));//Conversion from Eqn.(57)
+Krtou=Kr*Lm*(1-ephsilonm)/uo;//Dimensionless reaction rate group from Eqn.(5)
+
+
+//OUTPUT
+mprintf('\nComparing the values of 1-XA = %f and Krtou = %f with Fig.(6), we can conlcude that this operating condition is shown as point B in Fig.(3)',1-XA,Krtou);
+printf('\nLine 3 gives the locus of conversions for different values of the reaction rate group for this fluidized contacting');
+
+//====================================END OF PROGRAM ======================================================
\ No newline at end of file |