Difference between revisions of "Brushed DC Motor Theory"

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[[Category:Motors]]
[[Category:Motors]]


'''How does a motor work?'''
===How does a motor work?===


Let's consider a permanent magnet brushed motor. The piece connected to the ground is called the <I>stator</I> and the piece
Let's consider a permanent magnet brushed motor. The piece connected to the ground is called the <I>stator</I> and the piece
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|[[image:torque2.jpg|300px]]
|[[image:torque2.jpg|300px]]
|}
|}

===Equations===


So, the torque is proportional to the current through the windings,
So, the torque is proportional to the current through the windings,


<math>\Tau = k I</math>,
<math>\tau = k I</math>,


where <math>\Tau</math> is the torque, <math>I</math> is the current, and <math>k</math> is a constant. The wire coils have both a resistance, <math>R</math>, and an inductance, <math>L</math>. When the motor is turning, the current is switching, causing a
where <math>\tau</math> is the torque, <math>I</math> is the current, and <math>k</math> is a constant. The wire coils have both a resistance, <math>R</math>, and an inductance, <math>L</math>. When the motor is turning, the current is switching, causing a
voltage,
voltage,


<math>V = L \frac{dI}{dt}</math>
<math>V = L \begin{matrix}\frac{dI}{dt}\end{matrix}</math>


This voltage is known as the back-emf(electromotive force), <math>\epsilon</math>. If the angular velocuty of the motor is <math>\omega</math>, then
This voltage is known as the back-emf(electromotive force), <math>\epsilon</math>. If the angular velocuty of the motor is <math>\omega</math>, then
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where
where


<math>I = \frac{\Tau}{R}</math>
<math>I = \frac{\tau}{R}</math>


which implies
which implies


<math>(V-k\omega) = \frac{\Tau}{k}R</math>.
<math>(V-k\omega) = \frac{\tau}{k}R</math>.


The maximum or stall torque is the torque at which <math>\omega = 0</math> or
The maximum or stall torque is the torque at which <math>\omega = 0</math> or


<math>\Tau = \frac{kV}{R}</math>,
<math>\tau_{stall} = \frac{kV}{R}</math>,


and the stall or starting current,
and the stall or starting current,


<math>I = \frac{V}{R}</math>
<math>I_{start} = \frac{V}{R}</math>


The no load speed,
The no load speed,


<math>\omega = \frac{V}{k}</math>,
<math>\omega_{no-load} = \frac{V}{k}</math>,


is the maximum speed the motor can run. Given a constant voltage, the motor will settle at a constant speed, just like a terminal velocity. If we plot w = V/k - (<I>T</I>/k^2)R, we can get the speed-torque
is the maximum speed the motor can run. Given a constant voltage, the motor will settle at a constant speed, just like a terminal velocity. If we plot
curve:</P>


<math>\omega = \begin{matrix}\frac{V}{k}\end{matrix} - \begin{matrix}\frac{\tau}{k^2}\end{matrix}R</math>,
<P><IMG SRC="graph.jpg" WIDTH=320 HEIGHT=230 X-CLARIS-USEIMAGEWIDTH X-CLARIS-USEIMAGEHEIGHT ALIGN=bottom></P>


we can get the speed-torque curve:
<P>

[[image:graph.jpg|320px]]


<HR>
<HR>


===Units===
</P>


Here are the different units for the torque, current and voltage
<P><B>Units </B></P>


{|
<P>Here are the different units for the torque, current and
|+
voltage</P>
| Torque || <math>\tau</math> || Nm (=kgm/s^2*m), kgfm(=9.8 times Nm), gfcm, mNm, etc

|+
<P>Torque: oz.in., Nm (=kgm/s^2*m), kgfm(=9.8 times Nm), gfcm, mNm,
| Current || <math>I</math> || Amperes(Amps), mA
etc.</P>
|+

| Voltage || <math>V</math> || Volts
<P>Current: Amperes(Amps), mA</P>
|+

| Mechanical Power || <math>\tau\omega</math> || 1 Nm/sec = 1 watt
<P>Voltage: Volts</P>
|+

| Electrical Power || <math>VI</math> || 1 volt*amp = 1 watt
<P>mechanical power = T*w(Nm/sec) = 1 watt</P>
|}

<P>electrical power = VI = 1 volt * amp = 1watt</P>

Revision as of 13:30, 9 June 2006


How does a motor work?

Let's consider a permanent magnet brushed motor. The piece connected to the ground is called the stator and the piece connected to the output shaft is called the rotor. The inputs of the motor are connected to 2 wires and by applying a voltage across them, the motor turns.

The torque of a motor is generated by a current carrying conductor in a magnetic field. The right hand rule states that if you point your right hand fingers along the direction of current, , and curl them towards the direction of the magnetic flux, , the direction of force is along the thumb.

580px

Now, imagine a loop of wire with some resistance is inserted between the two permanent magnets. The following diagrams show how the motor turns:

File:Motor2.jpg
Diagram showing how the motor works
Relationship between the Torque and the angle the loop made with the magnet

You might be able to notice that the direction of rotation is changing every half cycle. To keep it rotating in the same direction, we have to switch the current direction. The process of switching current is called commutation. To switch the direction of curent, we have to use brushes and commutators. Commutation can also be done electronically (Brushless motors) and a brushless motor usually has a longer life. The following diagram shows how brushes and commutators work.

550px

We could also have several commutators and loops. The total torque generated is the sum of all the torques from each of the loops added.

File:Brush.jpg
Motor with several commutators and loops
Torque1.jpg Torque2.jpg

Equations

So, the torque is proportional to the current through the windings,

,

where is the torque, is the current, and is a constant. The wire coils have both a resistance, , and an inductance, . When the motor is turning, the current is switching, causing a voltage,

This voltage is known as the back-emf(electromotive force), . If the angular velocuty of the motor is , then

,

like a generator. This voltage, , is working against the voltage we apply across the terminals, and so,

,

where

which implies

.

The maximum or stall torque is the torque at which or

,

and the stall or starting current,

The no load speed,

,

is the maximum speed the motor can run. Given a constant voltage, the motor will settle at a constant speed, just like a terminal velocity. If we plot

,

we can get the speed-torque curve:

Graph.jpg


Units

Here are the different units for the torque, current and voltage

Torque Nm (=kgm/s^2*m), kgfm(=9.8 times Nm), gfcm, mNm, etc
Current Amperes(Amps), mA
Voltage Volts
Mechanical Power 1 Nm/sec = 1 watt
Electrical Power 1 volt*amp = 1 watt