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-Sample Notebook - Heat and Mass Transfer by R.K. Rajput : Chapter 1 - Basic Concepts
-author: Umang Agarwal
-
-
-# Example 1.1 Page 16-17
-
-L=.045; #[m] - Thickness of conducting wall
-delT = 350 - 50; #[C] - Temperature Difference across the Wall
-k=370; #[W/m.C] - Thermal Conductivity of Wall Material
-#calculations
-#Using Fourier's Law eq 1.1
-q = k*delT/(L*10**6); #[MW/m^2] - Heat Flux
-#results
-print '%s %.2f %s' %("\n \n Rate of Heat Transfer per unit area =",q," W");
-#END
-
-# Example 1.2 Page 17
-
-L = .15; #[m] - Thickness of conducting wall
-delT = 150 - 45; #[C] - Temperature Difference across the Wall
-A = 4.5; #[m^2] - Wall Area
-k=9.35; #[W/m.C] - Thermal Conductivity of Wall Material
-#calculations
-#Using Fourier's Law eq 1.1
-Q = k*A*delT/L; #[W] - Heat Transfer
-#Temperature gradient using Fourier's Law
-TG = - Q/(k*A); #[C/m] - Temperature Gradient
-#results
-print '%s %.2f %s' %("\n \n Rate of Heat Transfer per unit area =",Q," W");
-print '%s %.2f %s' %("\n \n The Temperature Gradient in the flow direction =",TG," C/m");
-#END
-
-# Example 1.3 Page 17-18
-
-x = .0825; #[m] - Thickness of side wall of the conducting oven
-delT = 175 - 75; #[C] - Temperature Difference across the Wall
-k=0.044; #[W/m.C] - Thermal Conductivity of Wall Insulation
-Q = 40.5; #[W] - Energy dissipitated by the electric coil withn the oven
-#calculations
-#Using Fourier's Law eq 1.1
-A = (Q*x)/(k*delT); #[m^2] - Area of wall
-#results
-print '%s %.2f %s' %("\n \n Area of the wall =",A," m^2");
-#END
-
-# Example 1.4 Page 18-19
-
-delT = 300-20; #[C] - Temperature Difference across the Wall
-h = 20; #[W/m^2.C] - Convective Heat Transfer Coefficient
-A = 1*1.5; #[m^2] - Wall Area
-#calculations
-#Using Newton's Law of cooling eq 1.6
-Q = h*A*delT; #[W] - Heat Transfer
-#results
-print '%s %.2f %s' %("\n \n Rate of Heat Transfer =",Q," W");
-#END
-
-# Example 1.5 Page 19
-
-L=.15; #[m] - Length of conducting wire
-d = 0.0015; #[m] - Diameter of conducting wire
-A = 22*d*L/7; #[m^2] - Surface Area exposed to Convection
-delT = 120 - 100; #[C] - Temperature Difference across the Wire
-h = 4500; #[W/m^2.C] - Convective Heat Transfer Coefficient
-print 'Electric Power to be supplied = Convective Heat loss';
-#calculations
-#Using Newton's Law of cooling eq 1.6
-Q = h*A*delT; #[W] - Heat Transfer
-Q = round(Q,1);
-#results
-print '%s %.2f %s' %("\n \n Rate of Heat Transfer =",Q," W");
-#END
-
-# Example 1.6 Page 20-21
-
-T1 = 300 + 273; #[K] - Temperature of 1st surface
-T2 = 40 + 273; #[K] - Temperature of 2nd surface
-A = 1.5; #[m^2] - Surface Area
-F = 0.52; #[dimensionless] - The value of Factor due geometric location and emissivity
-sigma = 5.67*(10**-8) #(W/(m^2 * K^4)) - Stephen - Boltzmann Constant
-#calculations
-#Using Stephen-Boltzmann Law eq 1.9
-Q = F*sigma*A*(T1**4 - T2**4) #[W] - Heat Transfer
-#Equivalent Thermal Resistance using eq 1.10
-Rth = (T1-T2)/Q; #[C/W] - Equivalent Thermal Resistance
-#Equivalent convectoin coefficient using h*A*(T1-T2) = Q
-h = Q/(A*(T1-T2)); #[W/(m^2*C)] - Equivalent Convection Coefficient
-#results
-print '%s %.2f %s' %("\n \n Rate of Heat Transfer =",Q," W");
-print '%s %.2f %s' %("\n The equivalent thermal resistance =",Rth," C/W");
-print '%s %.2f %s' %("\n The equivalent convection coefficient =",h," W/(m^2 * C)");
-#END
-
-# Example 1.7 Page 21-22
-
-L = 0.025; #[m] - Thickness of plate
-A = 0.6*0.9; #[m^2] - Area of plate
-Ts = 310; #[C] - Surface Temperature of plate
-Tf = 15; #[C] - Temperature of fluid(air)
-h = 22; #[W/m^2.C] - Convective Heat Transfer Coefficient
-Qr = 250; #[W] - Heat lost from the plate due to radiation
-k = 45; #[W/m.C] - Thermal Conductivity of Plate
-#calculations
-# In this problem, heat conducted by the plate is removed by a combination of convection and radiation
-# Heat conducted through the plate = Convection Heat losses + Radiation Losses
-# If Ti is the internal plate temperature, then heat conducted = k*A*(Ts-Ti)/L
-Qc = h*A*(Ts-Tf); #[W] - Convection Heat Loss
-Ti = Ts + L*(Qc + Qr)/(A*k); #[C] - Inside plate Temperature
-#results
-print '%s %.2f %s' %("\n \n Rate of Heat Transfer =",Ti," C");
-#END
-
-# Example 1.8 Page 22
-
-Ts = 250; #[C] - Surface Temperature
-Tsurr = 110; #[C] - Temperature of surroundings
-h = 75; #[W/m^2.C] - Convective Heat Transfer Coefficient
-F = 1; #[dimensionless] - The value of Factor due geometric location and emissivity
-sigma = 5.67*(10**-8) #(W/(m^2 * K^4)) - Stephen - Boltzmann Constant
-k = 10; #[W/m.C] - Thermal Conductivity of Solid
-#calculations
-# Heat conducted through the plate = Convection Heat losses + Radiation Losses
-qr = F*sigma*((Ts+273)**4-(Tsurr+273)**4) #[W/m^2] - #[W] - Heat lost per unit area from the plate due to radiation
-qc = h*(Ts-Tsurr); #[W/m^2] - Convection Heat Loss per unit area
-TG = -(qc+qr)/k; #[C/m] - Temperature Gradient
-#results
-print '%s %.2f %s' %("\n \n The temperature Gradient =",TG," C/m");
-#END
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