Continuous and discontinuous modes of series excited DC motors

In summary, the speed-torque characteristics of a DC motor change as the angle of rotation α changes.
  • #1
Fatima Hasan
319
14
Homework Statement
Attached below.
Relevant Equations
-
Here's my attempt:
Matlab:
clc;
clear all;
Ra=1.8;
La=150*10^(-3);
Ls=150*10^(-3);
Rs=1.8;
Rt=Rs+Ra;
ws=100*pi;
c=1.25;
vrms=240;
vm=240*sqrt(2);
f=50;
T=1:0.5:50;

for a=0:pi/9:pi/3
vt=(2*vm*cos(a))/pi

wc=((ws*(Ls+La)/tan(a))-Rs-Ra)/c;
x=[wc; a+pi];
Tc=c*(2*vm*cos(a)/(pi*(c*wc+Ra+Rs)))^2;

for i=1:length(T)
    if T(i)>Tc % Continuous Mode
        w(i)=vt/(c*sqrt(T(i)))-Rt/c;
        
else %Discontinuous Mode
for j=1:100
g1=sin(x(1)-x(2))-sin(a-x(2))*exp(-(x(1)-a)/(tan(x(2))));
%Ia=sqrt(T)=sqrt(vt/(c*sqrt(T(i)))-Rt/c);
g2=vm*(cos(a)-cos(x(1)))*tan(x(2))-pi*ws*(Ls+La)*sqrt(vt/(c*sqrt(T(i)))-Rt/c);
G=[g1; g2];
J11=cos(x(1)-x(2))+sin((a-x(2))/(tan(x(2))))*exp(-(x(1)-a)/(tan(x(2))))
J12=-cos(x(1)-x(2))+cos(a-x(2))*exp(-(x(1)-a)/tan(x(2)))-sin(a-x(2))*exp(-(x(1)-a)/tan(x(2)))*(x(1)-a)/(sin(x(2))^2)
J21=vm*sin(x(1))*tan(x(2))
J22=vm*(cos(a)-cos(x(1)))/(cos(x(2)))^2
J=[J11 J12; J21 J22];
x=x-inv(J)*G
end
w(i)=x(1);
end
end
n=w*60/(2*pi);
plot(T,n)
end
 legend('a=0 deg','a=20 deg','a=40 deg','a=60 deg')
 title('Speed-Torque Characteristics')
 xlabel('Torque (N.m)')
 ylabel('Speed (rpm)')

I got a wrong result, I attached it below.
Could someone let me know where is my mistake please?
 

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  • #2
I don't know how MATLAB works.

I can do the calculation using Visual Basic [or even Microsoft Excel]

It is hard to guess what the symbol meanings are.

In my opinion vt it has to be average Vo(t). In this case vt=Vm*[1+cos(α)].

According to my calculation for α=0 rpm=311.9 and torque=3.6 Nm; for α=30 rpm=180 and torque=9.28Nm; α=60 rpm=69.6 and torque=38.2 Nm

If α<=60o[1.045 rad] the non-conduction time it is α /(2.π.50)=0.0033 sec.

[if T=(0.3/3.6)=0.0833 sec] Ia=1.9.e^(-t/T)=1.8262 A
 
  • #3
Sorry.Correction: vt=Vm*[1+cos(α)]/π
 
  • #4
If I remember correctly, the calculation formulas for DC motors are as follows:
 

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FAQ: Continuous and discontinuous modes of series excited DC motors

What is the difference between continuous and discontinuous modes of series excited DC motors?

The main difference between these two modes is the way in which the motor is controlled. In continuous mode, the motor is constantly supplied with current, while in discontinuous mode, the current is only supplied for a portion of the motor's rotation.

What are the advantages of using continuous mode in a series excited DC motor?

Continuous mode allows for a more stable and smoother operation of the motor. It also provides better control over the speed and torque of the motor, making it suitable for applications that require precise control.

In what situations would discontinuous mode be more suitable for a series excited DC motor?

Discontinuous mode is often used in applications where the motor needs to operate at varying speeds or where energy efficiency is a priority. It can also be used in situations where the motor needs to be stopped and started frequently.

How does the control of a series excited DC motor differ in continuous and discontinuous modes?

In continuous mode, the motor is controlled using a variable resistance in the circuit, while in discontinuous mode, the control is achieved by switching the current on and off at specific intervals using a switching device.

Can a series excited DC motor be operated in both continuous and discontinuous modes?

Yes, a series excited DC motor can be designed to operate in both continuous and discontinuous modes. This allows for greater flexibility in its use and allows the motor to be adapted to different applications.

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