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 --- 3831/CH11/EX11.12/Ex11_12.sce | 21 +++++++++++++++++++++ 1 file changed, 21 insertions(+) create mode 100644 3831/CH11/EX11.12/Ex11_12.sce (limited to '3831/CH11/EX11.12/Ex11_12.sce') diff --git a/3831/CH11/EX11.12/Ex11_12.sce b/3831/CH11/EX11.12/Ex11_12.sce new file mode 100644 index 000000000..a3a969613 --- /dev/null +++ b/3831/CH11/EX11.12/Ex11_12.sce @@ -0,0 +1,21 @@ +// Example 11_12 +clc;funcprot(0); +// Given data +T=60.0;// °F +p_1=14.7;// psia +r_c=19.2:1;// Compression ratio + +// Solution +// From Table C.16a in Thermodynamic Tables to accompany Modern Engineering Thermodynamics,we find that, at 60.0°F = 520.R, +u_1=88.62;// Btu/lbm +p_r1=1.2147; +v_r1=158.58; +v_2byv_1=1/19.2; +v_r2=v_r1*v_2byv_1; +// Scanning down the v_r column in Table C.16a, we find that vr = 8.26 at about +T_2=1600-459.67;// °F +u_2=286.06;// Btu/lbm +p_r2=71.73; +p_2=p_1*(p_r2/p_r1);// psia +W_12bym=u_1-u_2;// Btu/lbm +printf("\nThe final temperature and pressure of the air at the end of the compression stroke,T_2=%4.0f°F and p_2=%3.1f psia. \nThe work required per lbm of air present,1W2/m=%3.2f Btu/lbm",T_2,p_2,W_12bym); -- cgit