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author | prashantsinalkar | 2018-02-03 11:01:52 +0530 |
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committer | prashantsinalkar | 2018-02-03 11:01:52 +0530 |
commit | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df (patch) | |
tree | 449d555969bfd7befe906877abab098c6e63a0e8 /3871/CH11 | |
parent | d1e070fe2d77c8e7f6ba4b0c57b1b42e26349059 (diff) | |
download | Scilab-TBC-Uploads-7bc77cb1ed33745c720952c92b3b2747c5cbf2df.tar.gz Scilab-TBC-Uploads-7bc77cb1ed33745c720952c92b3b2747c5cbf2df.tar.bz2 Scilab-TBC-Uploads-7bc77cb1ed33745c720952c92b3b2747c5cbf2df.zip |
Diffstat (limited to '3871/CH11')
-rw-r--r-- | 3871/CH11/EX11.1/Ex11_1.sce | 39 | ||||
-rw-r--r-- | 3871/CH11/EX11.2/Ex11_2.sce | 22 | ||||
-rw-r--r-- | 3871/CH11/EX11.3/Ex11_3.sce | 29 | ||||
-rw-r--r-- | 3871/CH11/EX11.4/Ex11_4.sce | 23 | ||||
-rw-r--r-- | 3871/CH11/EX11.5/Ex11_5.sce | 27 | ||||
-rw-r--r-- | 3871/CH11/EX11.6/Ex11_6.sce | 24 | ||||
-rw-r--r-- | 3871/CH11/EX11.7/Ex11_7.sce | 24 | ||||
-rw-r--r-- | 3871/CH11/EX11.8/Ex11_8.sce | 26 |
8 files changed, 214 insertions, 0 deletions
diff --git a/3871/CH11/EX11.1/Ex11_1.sce b/3871/CH11/EX11.1/Ex11_1.sce new file mode 100644 index 000000000..d26f8a1e7 --- /dev/null +++ b/3871/CH11/EX11.1/Ex11_1.sce @@ -0,0 +1,39 @@ +//===========================================================================
+//chapter 11 example 1
+
+clc;clear all;
+
+//variable declartion
+v = 1.0186; //emf of standard cell in volts
+l = 60; //length in cm
+l1 = 75; //length in cm
+l2 = 66; //length in cm
+l3 = 84; //length in cm
+l4 = 40; //length in cm
+l5 = 72; //length in cm
+S = 2; //resistance in Ω
+r = 100; //ratio of volt ratio box
+S1 = 2.5; //resistance in Ω
+I = 0.28; //ammeter reading in ampere
+v1 =1.25; //voltmeter reading in volts
+
+//calculations
+v0 = v/l; //the voltage drop per cm length of potentiometer wire in volt
+V1 = v0*l1; //emf of cell which balances at 75 cm in volts
+V2 = v0*l2; //emf of cell which balances at 66 cm in volts
+I1 = v/S; //current flowing through 2 Ω resistance in A
+V3 = v0*l3; //emf of cell which balances at 84 cm in volts
+v31 = V3*r; //voltage of supply main in volts
+V4 = v0*l4; //emf of cell which balances at 40 cm in volts
+I4 =V4/S1; //current flowing through 2.5 Ω resistance in A
+e = ((I-I4)/I4)*100; //percentage error in the ammeter reading in %
+V5 = v0*l5; //emf of cell which balances at 72 cm in volts
+e1 = ((v1-V5)/V5)*100; //percentage error in the voltmeter reading in %
+
+//result
+mprintf("emf of cell which balances at 75 cm = %3.5f volts",V1);
+mprintf("\ncurrent flowing through 2 Ω resistance = %3.5f A",I1);
+mprintf("\nvoltage of supply main in volts = %3.5f volts",v31);
+mprintf("\npercentage error in the ammeter reading = %3.1d percentage high",e);
+mprintf("\npercentage error in the voltmeter reading = %3.2f percentage ",e1);
+
diff --git a/3871/CH11/EX11.2/Ex11_2.sce b/3871/CH11/EX11.2/Ex11_2.sce new file mode 100644 index 000000000..b04df9705 --- /dev/null +++ b/3871/CH11/EX11.2/Ex11_2.sce @@ -0,0 +1,22 @@ +//===========================================================================
+//chapter 11 example 2
+clc;
+clear all;
+
+//variable declaration
+R = 10; //resistance of slide wire in Ω
+n = 15; //number of steps of dial
+r = 10; //resistance of each dial in Ω
+I = 0.01; //working current in A
+N = 100; //number of divisions of slide
+a = 0.2; //each division of slide can read upto a accurately of its span
+
+//calculations
+R1 = (n*r)+R; //total resistance of potentiometer in Ω
+V = I*R1; //voltage range of the potentiometer V
+v = R*I; //voltage drop across slide wire V
+x = v/N; //each division represents in V
+y = x*a; //resolution of potentiometer in V
+
+//result
+mprintf("resolution of potentiometer = %3.4f V",y);
diff --git a/3871/CH11/EX11.3/Ex11_3.sce b/3871/CH11/EX11.3/Ex11_3.sce new file mode 100644 index 000000000..9ea913838 --- /dev/null +++ b/3871/CH11/EX11.3/Ex11_3.sce @@ -0,0 +1,29 @@ +//===========================================================================
+//chapter 11 example 3
+clc;
+clear all;
+
+//variable declaration
+R = 400; //total resistance of slide-wire of 200 cmin Ω
+L1 = 101.8; //length of slide wire in cm
+L = 200; //length of wire in cm
+v1 = 1.018; //voltage drop across 101.8cm length of slide wire in V
+v = 3; //battery voltage in V
+a = 0.2; //it is possible to read a of 1 mm
+
+//calculations
+R1 = (R/L)*L1; //resistance of slide wire of 101.8 cm in Ω
+I1 = v1/R1; //working current in A
+RT = v/I1; //total resistance of battery circuit in Ω
+RR = RT-R; //resistance of series rheostat in Ω
+r = I1*R; //measuring range in V
+//since 200cm length represents 2 V
+//1 mm length represents = z
+z = (r/L)*(1/10); //voltage represented for 1mm length
+Ri = z*a; //resolution of instrument in mV
+
+//result
+mprintf("working current = %3.1e A",(I1*10^3));
+mprintf("\nresistance of series rheostat = %3.2f Ω",RR);
+mprintf("\nmeasuring range = %3.2f V",r);
+mprintf("\nresolution of the instrument = %3.2f mV",(Ri*10^3));
diff --git a/3871/CH11/EX11.4/Ex11_4.sce b/3871/CH11/EX11.4/Ex11_4.sce new file mode 100644 index 000000000..f594688ca --- /dev/null +++ b/3871/CH11/EX11.4/Ex11_4.sce @@ -0,0 +1,23 @@ +//===========================================================================
+//chapter 11 example 4
+
+clc;
+clear all;
+
+//variable declaration
+R1 = 0.1; //standard resistance in Ω
+V2 = 0.613; //voltage drop across standard resistance in V
+a = 100;
+r = 0.781; //volt ration box
+theta = 50.48;
+theta1 = 12.6;
+f = 50; //frequency in in HZ
+
+//calculations
+I = V2/R1; //current through coil in A
+V1 = a*r; //voltage drop across inductive coil in V
+theta2 = theta -theta1;
+L = V1*sin(theta2*180/%pi)/(2*%pi*f*I); //inducatance of coil in H
+
+//result
+mprintf("inductance of coil =%3.2f H",L);
diff --git a/3871/CH11/EX11.5/Ex11_5.sce b/3871/CH11/EX11.5/Ex11_5.sce new file mode 100644 index 000000000..7f265a03e --- /dev/null +++ b/3871/CH11/EX11.5/Ex11_5.sce @@ -0,0 +1,27 @@ +//===========================================================================
+//chapter 11 example 5
+
+clc;clear all;
+
+//variable declaration
+R1 = 1; //standard resistance in Ω
+V3 = 0.952-0.340*%i; //voltage through the coil in A
+a = 10; //multiplying power of potential divider
+V2 = 1.35+1.28*%i; //voltage across potential in A
+
+//calculations
+x = complex([0.952,-0.342])
+y = complex([1.35,1.28])
+I = x/R1;, //current through coil in A
+I = x/R1 //current through coil in A
+I1 = 0.952-0.340*%i;
+V1 = a*y //voltage across coil in V
+V11 = 13.5+12.8*%i;
+Z = V11/I1
+R = real(Z) //resistance of coil in Ω
+X = imag(Z) //reactance of coil Ω
+
+//result
+mprintf("%g + %gi\n",R,X);
+mprintf("resistance of coil = %3.4f Ω",R);
+mprintf("\nreactance of coil = %3.2f Ω",X);
diff --git a/3871/CH11/EX11.6/Ex11_6.sce b/3871/CH11/EX11.6/Ex11_6.sce new file mode 100644 index 000000000..6bd391a01 --- /dev/null +++ b/3871/CH11/EX11.6/Ex11_6.sce @@ -0,0 +1,24 @@ +//===========================================================================
+//chapter 11 example 6
+
+clc;
+clear all;
+
+//variable declaration
+R = 1; //resistace in Ω
+V2 = 0.238-%i*0.085; //voltage across standard resistor in V
+P = 10; //multiplying ower of potential divider
+V1 = 0.3375+%i*0.232; //voltage across potential divider in V
+
+
+
+//calculations
+I = V2/R; //current through coil in A
+V2 = P*V1; //voltage acrossthe coil in V
+Z = V2/I; //impedance of coil in Ω
+R1 = real(Z); // resistance of coil in Ω
+X1 =imag(Z); //reactance of coil in Ω
+
+//result
+mprintf("resistance = %3.2f Ω",R1);
+mprintf("\nreactance = %3.3f Ω",X1);
diff --git a/3871/CH11/EX11.7/Ex11_7.sce b/3871/CH11/EX11.7/Ex11_7.sce new file mode 100644 index 000000000..50a324f47 --- /dev/null +++ b/3871/CH11/EX11.7/Ex11_7.sce @@ -0,0 +1,24 @@ +//===========================================================================
+//chapter 11 example 7
+
+clc;
+clear all;
+
+//variable declaration
+R1 = 1.0; //resistace in Ω
+V1 = 0.8-%i*0.75; //voltage drop across the resistance in volt
+V2 = 1.2+%i*0.3; //voltage across the coil in volt
+
+//calculations
+I = V1/R1; //current through coil in A
+x = (atan(imag(V1)/real(V1)))*180/%pi;
+y = (atan(imag(V2)/real(V2)))*180/%pi;
+phi = y-x;
+a =sqrt(((real(V2))^2)+((imag(V2))^2));
+b =sqrt(((real(I))^2)+((imag(I))^2));
+V3 = a*cos(phi*%pi/180); //resistive drop the coil in V
+P = a*b*cos(phi*%pi/180); //power loss in the coil in W
+
+
+//result
+mprintf("iron loss in the coil =%3.3f watt",P);
diff --git a/3871/CH11/EX11.8/Ex11_8.sce b/3871/CH11/EX11.8/Ex11_8.sce new file mode 100644 index 000000000..0109ff7ee --- /dev/null +++ b/3871/CH11/EX11.8/Ex11_8.sce @@ -0,0 +1,26 @@ +//===========================================================================
+//chapter 11 example 8
+
+clc;
+clear all;
+
+//variable declaration
+R1 = 0.1; //standard resistance in Ω
+V1 = 0.35-%i*0.1; //voltage drop across resistance in V
+V2 = 0.8-%i*0.15; //voltage across coil in V
+
+//calculations
+I = V1/R1;, //current through coil in A
+V = 300*V2; //apply voltage V
+x1 = real(I);
+y1 = abs(imag(I));
+V1 = sqrt((x1^2)+(y1^22));
+x = real(V);
+y = imag(V);
+I1 = sqrt((x^2)+(y^2));
+P = (x1*x)+(y1*y);
+//pf = P/(V1*I); //power factor of the load circuit in lagging
+pf = P/(V1*I1); //power factor of the load circuit in cos(phi)
+
+//result
+mprintf("power factor of the load circuit = %3.3f lagging",pf);
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