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Diffstat (limited to '1938/CH6/EX6.18')
-rwxr-xr-x | 1938/CH6/EX6.18/6_18.jpg | bin | 0 -> 1647073 bytes | |||
-rwxr-xr-x | 1938/CH6/EX6.18/6_18.sce | 23 |
2 files changed, 23 insertions, 0 deletions
diff --git a/1938/CH6/EX6.18/6_18.jpg b/1938/CH6/EX6.18/6_18.jpg Binary files differnew file mode 100755 index 000000000..8ff024583 --- /dev/null +++ b/1938/CH6/EX6.18/6_18.jpg diff --git a/1938/CH6/EX6.18/6_18.sce b/1938/CH6/EX6.18/6_18.sce new file mode 100755 index 000000000..ca1a30f4f --- /dev/null +++ b/1938/CH6/EX6.18/6_18.sce @@ -0,0 +1,23 @@ +clc,clear
+printf('Example 6.18\n\n')
+//note that a new function p2z has been defined below for direct representation of complex numbers in polar form
+function [FUN] = p2z(RRRR,Theeeta)
+ FUN = RRRR.*exp(%i*%pi*Theeeta/180.);
+endfunction
+
+load_total=1600*10^3
+pf=1/sqrt(2) //lag
+V_L=6600
+I_L=p2z(load_total/(sqrt(3)*V_L*pf),-1*acosd(pf))
+I_1=p2z(90,-1*acosd(0.8))
+I_2=I_L-I_1
+phi=abs(phasemag(I_2))
+I_a=abs(I_2)
+R_a=1.05,X_s=5 //resistance and synchronous reactance per phase
+V_ph=V_L/sqrt(3)
+E_ph=sqrt( (V_ph*cos(phi)+I_a*R_a )^2 + ( V_ph*sin(phi)+I_a*X_s )^2 )
+E_line=sqrt(3)*E_ph
+
+printf('Excitation of second alternator is %.2f V ',E_line)
+printf('\n The corresponding field current from the graph is about 310 A\n\n')
+printf('Note: The answer obtained will differ from textbook answer because of higher degree \nof accuracy while storing I_2 and the improper rounding off of I_2 in the textbook')
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