summaryrefslogtreecommitdiff
path: root/534/CH6/EX6.6/6_6_Molar_flux_Plate.sce
diff options
context:
space:
mode:
Diffstat (limited to '534/CH6/EX6.6/6_6_Molar_flux_Plate.sce')
-rw-r--r--534/CH6/EX6.6/6_6_Molar_flux_Plate.sce36
1 files changed, 36 insertions, 0 deletions
diff --git a/534/CH6/EX6.6/6_6_Molar_flux_Plate.sce b/534/CH6/EX6.6/6_6_Molar_flux_Plate.sce
new file mode 100644
index 000000000..8557b8d8f
--- /dev/null
+++ b/534/CH6/EX6.6/6_6_Molar_flux_Plate.sce
@@ -0,0 +1,36 @@
+clear;
+clc;
+printf('FUNDAMENTALS OF HEAT AND MASS TRANSFER \n Incropera / Dewitt / Bergman / Lavine \n EXAMPLE 6.6 Page 379 \n'); //Example 6.6
+// Water vapor conc and flux associated with the same location on larger surface of the same shape
+
+//Operating Conditions
+v = 100; //[m/s] Velocity of air
+Tsurr = 20+273; //[K] Surrounding Air Temperature
+L1 = 1; //[m] solid length
+Ts = 80+273; //[K] Surface Temp
+qx = 10000; //[W/m^2] heat flux at a point x
+Txy = 60+273; //[K] Temp in boundary layer above the point
+
+//Table A.4 Air Properties at T = 323K
+v = 18.2*10^-6; //[m^2/s] Viscosity
+k = 28*10^-3; //[W/m.K] Conductivity
+Pr = 0.7; //Prandttl Number
+//Table A.6 Saturated Water Vapor at T = 323K
+pasat = 0.082; //[kg/m^3]
+Ma = 18; //[kg/kmol] Molecular mass of water vapor
+//Table A.8 Water Vapor-air at T = 323K
+Dab = .26*10^-4; //[m^2/s]
+
+//Case 1
+Casurr = 0;
+Cas = pasat/Ma; //[kmol/m^3] Molar conc of saturated water vapor at surface
+Caxy = Cas + (Casurr - Cas)*(Txy - Ts)/(Tsurr - Ts);
+
+//Case 2
+L2 = 2;
+hm = L1/L2*Dab/k*qx/(Ts-Tsurr);
+Na = hm * (Cas - Casurr);
+
+
+printf("\n (a) Water vapor Concentration above the point = %.4f Kmol/m^3 \n (b) Molar flux to a larger surface = %.2e Kmol/s.m^2", Caxy,Na);
+//END \ No newline at end of file