Difference between revisions of "Brushed DC Motor Theory"

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where <math>\tau<\math> is the torque produced by the motor and <math>\omega<\math> is its angular velocity.
where <math>\tau\,<\math> is the torque produced by the motor and <math>\omega<\math> is its angular velocity.


The wire coils have both a resistance, <math>R</math>, and an inductance, <math>L</math>. If we define <math>v_m</math> to be the voltage across the
The wire coils have both a resistance, <math>R</math>, and an inductance, <math>L</math>. If we define <math>v_m</math> to be the voltage across the

Revision as of 17:05, 2 January 2007


Introduction

The specific type of motor we are addressing is the permanent magnet brushed DC motor (PMDC). These motors have two terminals. Applying a voltage across the terminals results in a proportional speed of the output shaft.

There are two pieces to the motor: 1) stator and 2) rotor. The stator includes the housing, windings and brushes. The rotor consists of the output shaft, windings and commutators. The image below shows a cut-away view of a Maxon motor. Note this picture has a gearbox and encoder attached to the motor.

Motor cutaway.png

Motor Physics

The forces inside a motor that cause the rotor to rotate are called Lorentz Forces. If an electron is moving through an electric field, it experiences a force that is perpendicular to both the magnetic field and the direction it's moving. If we have a current passing through a wire in a magnetic field , the wire experiences a force equal to

You can easily find the direction of this force using the Right Hand Rule. The Right Hand Rule states that if you point your right hand's index finger along the direction of current, , and your middle finger in the direction of magnetic flux, , the direction of force is along the thumb. See the picture below.

Lorentz Force.png

Now, imagine this single wire is replaced with a loop of wire. Between the magnets' poles, this looks like two wires with current flowing in opposite directions. The forces on the wires cause the loop to rotate.

A coil consists of many such loops, and it is attached to the rotor and rotates. As it does so, the magnitude and direction of the forces on the wires remain approximately constant. However, the resultant torque varies with the angle. Look at the picture below. When the coil starts, there is maximum torque. As the coil moves, the moment arm is reduced and the torque decreases. Finally, when the coil is vertical (in the picture), there is no torque.

Rotating-coil.jpg


To keep a (almost) constant torque on the rotor, there are two things that happen. First, the current through the coil is reversed every half turn. So instead of an alternating torque like the one in the first figure below, the torque is always in the same direction. Also, additional coils can be used. When these coils are offset at different angles around the motor, the resultant torque becomes the sum of the colored torque curves in the figure below. The resultant torque is always greater than zero, but is not constant. This angle-dependent variation is called torque ripple.

Torque graphs.png

The process of switching current direction is called commutation. To switch the direction of curent, brushed DC motors use brushes and commutators. Commutation can also be done electronically (see Brushless DC Motors). The following diagram shows how brushes and commutators work.

Motor Commutators.jpg

Equations

Dc motor power.png

We start by writing the equation for conservation of energy in the motor. The power is input as electrical power, and the motor converts that to mechanical power, . However, some of the power is lost as heat, .


We can re-write this in terms of electrical and mechanical quantities as



where Failed to parse (unknown function "\math"): {\displaystyle \tau\,<\math> is the torque produced by the motor and <math>\omega<\math> is its angular velocity. The wire coils have both a resistance, <math>R} , and an inductance, . If we define to be the voltage across the terminals of the motor, then the motor's defining equation is

where is called the back-emf (electromotive force). The back-emf is proportional to the speed of the motor,

where is the rotation in revolutions-per-minute (rpm) and is called the speed constant, which depends on the motor design. The back-emf term indicates that any motor is also a generator: if we spin the motor shaft, we read a voltage at the motor terminals. This is how dams create hydroelectric power.

The torque generated by the motor is proportional to the current through the windings, where the constant of proportionality is called the torque constant or motor constant :

The torque constant has the same numerical value as the inverse of the speed constant when they are expressed in SI units, so there really is just one constant describing how our motor converts current to torque and angular velocity to voltage.


We are often interested in the steady-state operating characteristics of a motor, when the current is constant. The term becomes zero, and we get

which, using the relationships and , can be expressed equivalently as

We see that if we apply a constant voltage , the motor will spin at a speed such that . At this speed, the current is zero, so there is no more torque () to accelerate the motor to higher speeds. (Realistically, the motor is always applying some This back-emf voltage is working against the voltage we apply across the terminals. Using the constants from above, we get this equation,



The maximum torque, or stall torque, is the torque at which or



From this we can find the stall current, or starting current,



The no-load speed is the maximum speed the motor can turn. To find its value, we set the torque equal to zero and we get



This relationship means that, given a constant voltage, the motor will settle at a constant speed. This linear relationship produces the constant voltage speed-torque line


Datasheets and Speed-Torque Curves

The datasheet below is for the Maxon motor available in the Mechatronics Lab, which also has an integrated 6:1 gearhead and a 100 line encoder.

Maxon-characteristics-small.jpg

1. Nominal voltage: The recommended maximum voltage across the motor terminals, and the voltage for which the speed-torque curve (below) is plotted. The motor can be powered with less or more voltage, but higher voltage should be used with care, to prevent the motor coils from overheating due to ohmic (resistive) heating.

2. No load speed, : The speed of the motor powered by the nominal voltage when the motor provides zero torque.

3. No load current: The current required to spin the motor at the no load condition (i.e., the current needed to provide the torque necessary to overcome friction).

4. Nominal speed: The speed of the motor at the maximum continuous torque.

5. Nominal torque (max continuous torque): The maximum torque the motor can provide continuously.

6. Nominal current (max continuous current): The current that yields the maximum continuous torque. This maximum is determined by thermal characteristics of the motor. The power dissipated by the motor as heat is the product of the voltage across the motor and the current through it. Larger currents are acceptable intermittently, but larger continuous currents may cause the motor to overheat.

7. Stall torque, : The maximum torque achievable by the motor at the nominal voltage. This torque is achieved at zero velocity (stall).

8. Starting current, : The current through the motor at zero velocity, equal to the nominal voltage divided by the terminal resistance. Also called the stall current.

9. Max efficiency: The maximum efficiency of the motor in converting electrical power to mechanical power. This maximum efficiency typically occurs at high speed and low torque; the efficiency is zero at zero speed and zero torque.

10. Terminal resistance : The resistance of the motor windings.

11. Terminal inductance : The inductance of the motor windings.

12. Torque constant, : The constant of proportionality relating current to torque. In SI units (Newton-meters per amp), the torque constant is equivalent to the speed constant in SI units (radians per volt-second).

13. Speed constant, : The constant of proportionality relating speed to voltage. Equivalent to the torque constant when expressed in SI units.

14. Speed/torque gradient: A representation of the slope of the speed-torque curve (see graph below), approximately equal to the no load speed divided by the stall torque.

15. Mechanical time constant: The time it takes the unloaded motor to reach 63% of its no load speed under a constant voltage, starting from rest. Proportional to the inertia of the rotor and inversely proportional to the square of the the torque constant.

16. Rotor inertia: The inertia of the rotating element (the rotor) about the axis of rotation.

Much of the data sheet can be expressed in the speed-torque curve, plotted for the constant nominal voltage (below). The mechanical power output is the product of the torque and the speed, and is maximized at half the maximum speed and torque.

New-speed-torque-small.gif

Often you need higher torques but lower speeds in your application. In this case, you can add a gearbox to the motor, as discussed in Choosing a Motor and Gearing Combination.


References