# Brushed DC Motor Theory

m (Reverted edits by 134.157.250.5 (Talk); changed back to last version by 213.42.21.80) |
m (Reverted edits by Stephens (Talk); changed back to last version by 134.157.250.5) |

## Revision as of 13:12, 29 November 2006

## Contents |

## 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*.

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## 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 wire instead of a single electron, 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 fingers along the direction of current, *I*, and curl them towards the direction of the magnetic flux, *B*, the direction of force is along the thumb. See the picture below.

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 with forces as shown.

This coil is attached to the rotor and rotates. As it does so, the magnitude and direction of the force on the wires remains 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.

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 alway greater than zero, but is not constant. This variation is called *torque ripple*.

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.

## Equations

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

The wire coils have both a resistance, *R*, and an inductance, *L*. When the motor is turning, the current is switching, causing a voltage,

This voltage is called the *back-emf* (**e**lectro**m**otive **f**orce). The motor constants relate various quantities in a motor. They are a property of the design and material of each individual motor. The speed constant relates the back-emf to the output speed of the shaft,

where *n* is the rotation in **revolutions-per-minute** (rpm). The torque constant relates the input current (in the windings) to the torque of the output,

These two constants are actually the same number with different units. The relationship between the two is

Now look at the electrical side. If we sum the voltages, we get

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 *n* = 0 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*

## Reading Datasheets

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.

**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.

## References

- Carl R. Nave, "DC Motors," http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/motdc.html
- Maxon Motor Guide (pdf)