From 7f60ea012dd2524dae921a2a35adbf7ef21f2bb6 Mon Sep 17 00:00:00 2001 From: prashantsinalkar Date: Tue, 10 Oct 2017 12:27:19 +0530 Subject: initial commit / add all books --- 534/CH12/EX12.9/12_9_Brick_Wall.sce | 35 +++++++++++++++++++++++++++++++++++ 1 file changed, 35 insertions(+) create mode 100644 534/CH12/EX12.9/12_9_Brick_Wall.sce (limited to '534/CH12/EX12.9/12_9_Brick_Wall.sce') diff --git a/534/CH12/EX12.9/12_9_Brick_Wall.sce b/534/CH12/EX12.9/12_9_Brick_Wall.sce new file mode 100644 index 000000000..55c598a70 --- /dev/null +++ b/534/CH12/EX12.9/12_9_Brick_Wall.sce @@ -0,0 +1,35 @@ +clear; +clc; +printf('FUNDAMENTALS OF HEAT AND MASS TRANSFER \n Incropera / Dewitt / Bergman / Lavine \n EXAMPLE 12.9 Page 766 \n')// Example 12.9 + +// Total hemispherical emissivity of fire brick wall +// Total emissive power of brick wall +// Absorptivity of the wall to irradiation from coals + +Ts = 500 ;//[K] temperature of brick surface +Tc = 2000 ;//[K] Temperature of coal exposed +stfncnstt = 5.67*10^-8; //[W/m^2.K^4] Stefan-Boltzmann constant +// From the given graph of emissivities +e1 = .1; //between wavelength 0 micro-m- 1.5 micro-m +e2 = .5; //between wavelength 1.5 micro-m- 10 micro-m +e3 = .8; //greater than wavelength 10 micro-m + +//From Table 12.1 +//For wl1 = 1.5 micro-m and T = 500 K, At wl1*T = 750 micro-m.K +F0wl1 = 0; +//For wl2 = 10 micro-m and T = 500 K, At wl2*T = 5000 micro-m.K +F0wl2 = .634; +//From equation 12.36 +e = e1*F0wl1 + e2*F0wl2 + e3*(1-F0wl1-F0wl2); + +//Equation 12.26 and 12.35 +E = e*stfncnstt*Ts^4; + +//From Table 12.1 +//For wl1 = 1.5 micro-m and T = 2000 K, At wl1*T = 3000 micro-m.K +F0wl1c = 0.273; +//For wl2 = 10 micro-m and T = 2000 K, At wl2*T = 20000 micro-m.K +F0wl2c = .986; +ac = e1*F0wl1c + e2*[F0wl2c-F0wl1c] + e3*(1-F0wl2c); + +printf('\n Total hemispherical emissivity of fire brick wall = %.3f \n Total emissive power of brick wall = %i W/m^2.\n Absorptivity of the wall to irradiation from coals = %.3f',e,E,ac); \ No newline at end of file -- cgit