Confused with back emf,

by Dash-IQ
Tags: confused
 P: 107 I need help in understanding back emf, I'm a bit confused here. Example(for understanding): Let's assume we have a 12 V DC motor, that draws 20Amps when it starts, as it reaches maximum speeds, current drops due to back emf, lets assume the resistance is 0.6 ohms, and b.emf = 10V. Vtot = 2V ,from ohms law I can find the current at maximum speed, it would now be I = V/R = 3.3Amps Now what about power? Initial power = 240W Power at max rpm = 6.6W? Will the motor be stable at 2V at maximum speeds? Or will it draw more voltage because of the b.emf and stay the same rate of power @ 240W with lower current? (here is where I'm struggling). If everything above correct?
 P: 1,084 A motor does not "draw" voltage. There is 12V across the motor at all times. The 0.6 ohms represents 6.6W lost as heat in the motor windings. The motor is drawing 3.3A @ 12V which is 39.6 watts. The difference 39.6-6.6 = 33Watts of power delivered to the load (ignoring other motor losses). When it starts @ 20 amps it is producing high torque and delivering a lot of power to accelerate the load. You can do the numbers.
P: 107
 Quote by meBigGuy The 0.6 ohms represents 6.6W lost as heat in the motor windings. The motor is drawing 3.3A @ 12V which is 39.6 watts. The difference 39.6-6.6 = 33Watts of power delivered to the load (ignoring other motor losses). When it starts @ 20 amps it is producing high torque and delivering a lot of power to accelerate the load. You can do the numbers.
I'm trying to understand the idea to relate the numbers and make sense out of them. How is it still running @ 12 V when there is - 10 V shouldn't be 2V?

HW Helper
Thanks
P: 5,335
Confused with back emf,

 Quote by Dash-IQ I'm trying to understand the idea to relate the numbers and make sense out of them. How is it still running @ 12 V when there is - 10 V shouldn't be 2V? Please explain.
What is the electrical model you are using to represent the DC motor? Attach a sketch of the model and describe the purpose of each element in the model.
Engineering
HW Helper
Thanks
P: 7,160
 Quote by meBigGuy When it starts @ 20 amps it is producing high torque and delivering a lot of power to accelerate the load. You can do the numbers.
That is a bit confusing. When the motor starts (at zero RPM) the mechanical power output is zero. It is producing a torque, of course, but the torque doesn't do any mechanical work, or produce any mechanical power, until the motor starts to turn.

At zero RPM, all the electrical power (I2R) is converted into heat in the windings.
 P: 107 The example I used is random from my head, I have no specific model to study in detail. I just wanted to understand back emf more.
 Sci Advisor PF Gold P: 3,665 You might study this thread. Another PF'er was similarly confused, but he 'got it' by end of second page. See if it helps. http://www.physicsforums.com/showthread.php?t=624785
PF Gold
P: 1,431
 Quote by Dash-IQ The example I used is random from my head, I have no specific model to study in detail. I just wanted to understand back emf more.
I find this almost impossible to describe without images.

In a simplified dc motor:

12 vdc
10 amps
We can see that we can't really solve the equation: F=ILB
F being the force on the wire in newtons
I being current in amps
L being length in meters, of the motor winding perpendicular to the flux field
B being the flux field strength in tesla
But one thing we can tell is that the motor is going to start rotating.

There is another equation: emf = vBL sin θ (ref)
which describes what happens when a conductor is pushed through a magnetic field.
emf being the voltage generated
v being the velocity of the conductor through the magnetic field
B & L were defined above
sin θ being the angle of motion of the conductor in relation to the magnetic field
Now in the illustration that Hyperphysics has graciously provided, the angle θ changes constantly. But in real world dc motors, there are multiple loops of wire in the rotor, keeping the angle at relatively close to 90°. So the equation reduces to: emf = vBL

If you were to make up some numbers to to fill in the missing variables, you can actually calculate how fast your motor will run under no load, ideal textbook conditions, which would be when your emf generated, equaled the voltage supplied.

If c-emf didn't exist, the implications of F=ILB, would be disastrous, for an unloaded motor.

For F=ma, and if the current didn't reduce because of the c-emf, the motor would accelerate, until it disintegrated.
 Sci Advisor PF Gold P: 3,665 Nice Job OM ! One can empirically arrive at these two formulas for a DC machine, it's just lumping the constants together: Counter EMF = K X (flux) X RPM, where [K X (flux)] is usually written K$\Phi$, giving Counter EMF = K$\Phi$RPM , $\Phi$ of course is flux, K encompasses pi and radius to get from RPM to velocity, and length L too. Drive the motor at some speed and measure the open circuit voltage it makes, you have K$\Phi$ Torque = same K$\Phi$ X Armature Current X 7.04 , gives foot-pounds As OM said - with no counter EMF , ie motor stalled, armature current goes sky high and torque is dramatic. Your automobile starter is a good example . It's a beautifully self regulating system. As RPM comes up so does counter-emf, reducing current. Continuing to raise RPM (by driving the motor with something), counter-emf overwhelms applied voltage so current reverses and you have a generator.
PF Gold
P: 1,431
 Quote by jim hardy Nice Job OM !
 As OM said - with no counter EMF , ie motor stalled
The OP may not know what "stalled" means, in the context of electric motors.
"Stalled", in this context, means the motor is not allowed to turn.
We referred to this as "locked rotor", back in my day.
 , armature current goes sky high and torque is dramatic.
Which is actually a good thing. If you don't lock the rotor, something will happen.
 Your automobile starter is a good example .
It's been awhile, but I believe that's an example of a series wound electric motor, which is another subject. Let's just leave that alone for a while.
 It's a beautifully self regulating system.
That, I cannot argue with.

On the submarine I sailed around on, they had what was called a "motor-generator".

 As RPM comes up so does counter-emf, reducing current. Continuing to raise RPM (by driving the motor with something), counter-emf overwhelms applied voltage so current reverses and you have a generator.
At idle, neither end of the machine drew much current. All thanks to "counter" or "back" emf.
P: 107
 Quote by OmCheeto I find this almost impossible to describe without images. In a simplified dc motor: and given your initial parameters:12 vdc 10 ampsWe can see that we can't really solve the equation: F=ILBF being the force on the wire in newtons I being current in amps L being length in meters, of the motor winding perpendicular to the flux field B being the flux field strength in tesla But one thing we can tell is that the motor is going to start rotating. There is another equation: emf = vBL sin θ (ref) which describes what happens when a conductor is pushed through a magnetic field. emf being the voltage generated v being the velocity of the conductor through the magnetic field B & L were defined above sin θ being the angle of motion of the conductor in relation to the magnetic fieldNow in the illustration that Hyperphysics has graciously provided, the angle θ changes constantly. But in real world dc motors, there are multiple loops of wire in the rotor, keeping the angle at relatively close to 90°. So the equation reduces to: emf = vBL If you were to make up some numbers to to fill in the missing variables, you can actually calculate how fast your motor will run under no load, ideal textbook conditions, which would be when your emf generated, equaled the voltage supplied. If c-emf didn't exist, the implications of F=ILB, would be disastrous, for an unloaded motor. For F=ma, and if the current didn't reduce because of the c-emf, the motor would accelerate, until it disintegrated.
 Quote by jim hardy Nice Job OM ! One can empirically arrive at these two formulas for a DC machine, it's just lumping the constants together: Counter EMF = K X (flux) X RPM, where [K X (flux)] is usually written K$\Phi$, giving Counter EMF = K$\Phi$RPM , $\Phi$ of course is flux, K encompasses pi and radius to get from RPM to velocity, and length L too. Drive the motor at some speed and measure the open circuit voltage it makes, you have K$\Phi$ Torque = same K$\Phi$ X Armature Current X 7.04 , gives foot-pounds As OM said - with no counter EMF , ie motor stalled, armature current goes sky high and torque is dramatic. Your automobile starter is a good example . It's a beautifully self regulating system. As RPM comes up so does counter-emf, reducing current. Continuing to raise RPM (by driving the motor with something), counter-emf overwhelms applied voltage so current reverses and you have a generator.
Both wonderful and useful answers thank you.

 Related Discussions Electrical Engineering 4 Introductory Physics Homework 4 Special & General Relativity 14 Academic Guidance 8 High Energy, Nuclear, Particle Physics 11