Electrical Drives & Control

Chapter 5
DC Motor Drives and Control

Bachelors Program in Electrical Engineering
Electrical Drives & Control   •   Bachelor

DC Motor Drives and Control

Introduction

A DC motor drive combines a DC motor, a power converter, control circuitry, sensors, protection, and a mechanical load. Its principal advantages are simple torque production, wide speed range, rapid dynamic response, and straightforward four-quadrant operation. Although variable-frequency AC drives dominate many modern installations, DC drives remain important in laboratories, legacy industrial systems, traction equipment, hoists, rolling mills, test benches, and applications requiring high starting torque.

The essential control variables are armature voltage, armature current, and field flux. Armature voltage primarily controls speed below base speed, while field weakening extends speed above base speed. Armature current is proportional to torque, so current regulation provides direct control of acceleration and load response.

Learning Objectives

After studying this chapter, the student should be able to:

  1. Model separately excited, shunt, series, and permanent-magnet DC motors.
  2. Relate voltage, current, flux, torque, speed, and mechanical load.
  3. Explain armature-voltage control, field control, and field weakening.
  4. Analyze rectifier-fed and chopper-fed DC drives.
  5. Design basic current and speed-control loops.
  6. Explain plugging, regenerative braking, dynamic braking, and four-quadrant operation.
  7. Select an appropriate motor-drive arrangement for an industrial application.

1. DC Motor Fundamentals

In a conventional DC motor, armature conductors carrying current interact with the magnetic field to produce electromagnetic torque. Rotation generates a counter-emf, which opposes the applied armature voltage.

For a separately excited or shunt motor, neglecting brush drop initially:

Va = Ea + Ia Ra + La (dIa/dt)

where Va is armature voltage (V), Ea is back emf (V), Ia is armature current (A), Ra is armature resistance (Ω), and La is armature inductance (H). In steady state, the inductive term is zero:

Va = Ea + Ia Ra

The electromechanical relationships are

Ea = ke Φ ωm
Te = kt Φ Ia

Here, Φ is flux per pole (Wb), ωm is mechanical angular speed (rad/s), Te is electromagnetic torque (N·m), and ke and kt are machine constants. In SI units, with consistent definitions of flux and current, the numerical values of the torque and emf constants are equal: ke = kt = k.

The mechanical equation is

J (dωm/dt) = Te - TL - Bωm

where J is combined inertia (kg·m²), TL is load torque (N·m), and B is viscous-friction coefficient (N·m·s/rad). Coulomb friction and disturbances can be added when required.

Combining the steady-state equations gives

ωm = (Va - Ia Ra)/(k Φ)

This equation applies when the motor is not saturated, flux is approximately constant, and brush voltage and nonlinear losses are neglected. It demonstrates that speed falls as load current increases because of the armature-resistance drop.

The converted mechanical power is

Pconv = Ea Ia = Te ωm

and copper loss in the armature is Pcu,a = Ia2 Ra. The motor input power is Pin = Va Ia for a DC armature supply.

Torque–Speed Characteristic

At constant flux and fixed armature voltage, substituting Ia = Te/(kΦ) into the speed equation gives

ωm = Va/(kΦ) - (Ra/(k²Φ²)) Te

Thus, the torque–speed characteristic is approximately a straight line. A larger armature resistance produces greater speed droop. Electronic feedback can compensate for this droop and maintain nearly constant speed.

2. Types of DC Motors Used in Drives

Separately Excited Motor

The field winding is supplied from an independent source. Therefore, armature voltage and field current can be controlled independently. This arrangement provides excellent control flexibility and is the standard analytical model for modern DC drives.

Shunt Motor

The field winding is connected in parallel with the armature supply. If the supply voltage is constant, field flux is nearly constant. A shunt motor has moderate starting torque and good speed regulation.

Series Motor

The field winding is in series with the armature, so the field current is approximately the armature current. Before magnetic saturation, Φ ≈ kf Ia, and therefore

Te = kt kf Ia²

After saturation, flux is nearly constant and torque becomes approximately proportional to current. A series motor has very high starting torque, but it must never be operated unloaded because its speed can rise dangerously.

Permanent-Magnet DC Motor

Permanent magnets provide the field flux, eliminating field copper loss and the field converter. For a fixed magnet flux,

Va = k Φm ωm + Ia Ra + La(dIa/dt)

The PM motor is compact and efficient, but excessive armature current or temperature can demagnetize the magnets. Above-base-speed operation is possible only if the machine has suitable flux-weakening capability, often through controlled negative d-axis current in brushless equivalents; a conventional brushed PM motor generally has limited weakening capability.

Motor typeMain advantagePrincipal limitationTypical use
Separately excitedIndependent flux and speed controlRequires field supplyIndustrial test drives, rolling mills
ShuntGood steady-state speed regulationModerate starting torqueConstant-speed machinery
SeriesVery high starting torqueUnsafe at no loadTraction, cranes, hoists
Permanent magnetCompact and efficientMagnet heating/demagnetizationSmall drives, servomechanisms

3. Operating Regions and Control Methods

Constant-Torque Region: Armature-Voltage Control

With rated field flux, the motor operates below base speed by varying Va. Since Te = kΦIa, rated torque can be produced at rated current over much of this range. The converter must be capable of supplying the required armature current.

The base speed is reached when the armature voltage approaches its rated maximum while the field remains at rated flux:

ωbase ≈ (Va,rated - Ia,ratedRa)/(kΦrated)

Constant-Power Region: Field Weakening

Above base speed, armature voltage cannot be increased further. Speed is increased by reducing field flux. At approximately constant armature voltage,

ωm ≈ (Va - IaRa)/(kΦ)

so decreasing Φ increases speed. However, for a given current limit, torque decreases:

Te = kΦIa

If current remains at its rated limit, output power P = Teωm is approximately constant because torque decreases as speed increases. Field weakening is limited by commutation, mechanical overspeed, field-current minimum, and allowable armature voltage.

A drive must include an overspeed limit and field-loss protection. Loss of field in a separately excited motor can cause rapid acceleration, especially when the load torque is small.

4. Power Converters for DC Drives

Controlled Rectifier Drives

A phase-controlled rectifier converts AC supply voltage to controllable average DC voltage. For a fully controlled single-phase bridge with continuous current, the ideal average output is

Vd = (2Vm/π) cos α

where Vm is the AC source peak voltage and α is firing angle. The equation assumes an ideal bridge, continuous current, negligible source impedance, and no commutation overlap. In practice, source inductance, device drops, harmonics, and discontinuous current reduce the actual voltage.

For a three-phase fully controlled bridge,

Vd = (3√3 VLL/π) cos α

where VLL is the RMS line-to-line source voltage. For 0° ≤ α < 90°, the average voltage is positive and rectifying operation is obtained. For firing angles above 90°, average voltage can become negative; with a suitable DC current path and an active source, regenerative inversion is possible.

A dual converter uses two fully controlled bridges connected antiparallel on the DC side. It permits positive and negative average armature voltage and therefore enables reversible motoring and regenerative braking. Circulating-current dual converters require reactors and circulating-current control; non-circulating designs transfer control between bridges and avoid continuous circulating current.

Chopper Drives

A DC chopper applies a sequence of source-voltage pulses to the armature. In continuous-current operation, the average armature voltage of a step-down chopper is approximately

Va = D Vs

where D is duty ratio, the fraction of each switching period for which the switch is on, and Vs is source voltage. This ideal relationship assumes sufficiently smooth current, negligible semiconductor voltage drop, and a suitable freewheeling path.

Choppers provide high efficiency, fast response, regenerative capability, and reduced low-frequency supply harmonics. Their disadvantages include switching electromagnetic interference, ripple current, acoustic effects, and the need for careful grounding and filtering.

5. Current and Speed Control

Because torque is proportional to armature current, the inner current loop is normally faster than the outer speed loop.

A typical cascade structure is:

reference speed → speed controller → current limit → current controller → converter → motor → mechanical load

A tachogenerator, encoder, or observer supplies speed feedback. A current sensor supplies armature-current feedback. The current controller protects the motor and converter while producing rapid torque response. The speed controller commands torque-producing current and should include current limiting and anti-windup.

For a PI current controller,

uc(t) = Kp,iei(t) + Ki,i∫ei(t)dt

where ei = Ia^* - Ia is current error, Kp,i is proportional gain, and Ki,i is integral gain. The controller output uc is converted into firing angle or duty ratio. Practical implementations impose voltage saturation, current limits, measurement filtering, and anti-windup.

A speed PI controller has the analogous form

u_ω(t) = Kp,ωe_ω(t) + Ki,ω∫e_ω(t)dt

where e_ω = ω^* - ωm. The speed-loop bandwidth is normally substantially lower than the current-loop bandwidth so that the inner loop appears fast to the outer loop.

Dynamic Response

The electrical time constant of the armature, ignoring converter dynamics, is

τa = La/Ra

and the mechanical time constant depends on inertia, torque sensitivity, and operating point. Large inertia produces slower acceleration. A drive controller should be tuned with the actual motor, load, sensor, converter delay, and current limits rather than using nominal motor data alone.

6. Braking and Four-Quadrant Operation

The signs of speed and torque define four operating quadrants.

QuadrantSpeedTorqueOperation
I++Forward motoring
II+−Forward regenerative braking
III−−Reverse motoring
IV−+Reverse regenerative braking

Regenerative Braking

During regeneration, electromagnetic torque opposes rotation and mechanical energy is converted to electrical energy. The converter must return energy to the AC source or to a storage system. Regeneration is efficient but requires a reversible converter, an active front end, or a supply capable of absorbing power.

Dynamic Braking

The armature is disconnected from the supply and connected to a braking resistor. The rotating motor acts as a generator, with energy dissipated as heat. Dynamic braking is simple and reliable but does not return energy to the source. Braking torque decreases as speed falls.

Plugging

Plugging reverses the applied armature voltage or field polarity while the motor is rotating. The resulting torque opposes motion strongly, but armature current can become excessive. A current-limiting resistor or controlled converter is essential, and the supply must be disconnected at zero speed to prevent reverse acceleration.

Four-Quadrant Converter Requirements

A four-quadrant drive must control both the sign of armature voltage and the sign of armature current. The field is normally kept unidirectional; reversing armature voltage reverses torque and speed after deceleration. Interlocks, dead time, current sensing, and controlled transitions are required to prevent short circuits and torque shocks.

7. Worked Example: Separately Excited Motor

A separately excited motor has Va = 240 V, Ra = 0.50 Ω, kΦ = 1.20 V·s/rad, and a load requiring TL = 36 N·m. Friction is neglected. Find the steady-state armature current and speed.

At steady state, motor torque equals load torque:

Ia = TL/(kΦ) = 36/1.20 = 30 A

The back emf is

Ea = Va - IaRa = 240 - (30)(0.50) = 225 V

Therefore,

ωm = Ea/(kΦ) = 225/1.20 = 187.5 rad/s

In revolutions per minute,

n = (60ωm)/(2π) ≈ 1790 rpm

The converted power is

Pconv = TLωm = (36)(187.5) = 6750 W

The armature copper loss is Ia2Ra = (30)2(0.50) = 450 W. The calculation illustrates why current is the direct torque-control variable and why speed decreases under load because of the armature voltage drop.

8. Applied Case: Reversible Hoist Drive

Background

Consider an illustrative 15-kW separately excited DC motor driving a warehouse hoist. The hoist must lift and lower loads, hold position briefly, and stop rapidly. The load can drive the motor during lowering.

Problem

A one-quadrant armature converter can lift the load but cannot safely return energy during lowering. Uncontrolled lowering could cause overspeed, and plugging could produce excessive current.

Analysis

Lifting requires positive speed and positive torque. During controlled lowering, the motor may rotate forward while electromagnetic torque is negative, placing the system in the regenerative-braking quadrant. The drive therefore needs a reversible armature converter, a field-loss relay, an encoder, a current sensor, a mechanical brake, and an emergency braking path.

Approach and Solution

A four-quadrant dual converter is selected. The inner current loop limits armature current to the motor’s permissible value. The outer speed loop commands negative torque during lowering. A field-current monitor inhibits armature operation if the field falls below its safe threshold. A mechanical brake engages when the drive is disabled or when the hoist is stationary. The controller uses a ramped speed reference to avoid load shock and includes overspeed and overcurrent trips.

Outcome

The arrangement provides smooth lifting, controlled regenerative lowering, rapid but limited braking, and safe shutdown. Energy returned during lowering may be absorbed by the supply, a regenerative front end, or a braking resistor if regeneration is unavailable.

Learning Points

The correct converter is determined by required power flow, not merely by motor rating. Hoists require attention to field loss, holding brakes, load-driven regeneration, current limits, and fail-safe behavior. Electrical control does not replace a mechanical brake where a falling load presents a hazard.

9. Design and Practical Considerations

Motor and converter ratings must account for continuous current, overload duration, duty cycle, acceleration time, thermal limits, ambient temperature, and altitude. A converter rated only for average current may fail under repeated acceleration or plugging.

Feedback sensors should be selected for the required bandwidth, resolution, isolation, and environmental conditions. Current sensors need adequate peak range and electrical isolation. Encoder wiring should be shielded and routed away from high dv/dt switching conductors.

Protection should include semiconductor fuses, overcurrent detection, overvoltage protection, field-loss detection, overspeed detection, thermal protection, emergency stop, and appropriate braking resistors. The design must comply with applicable electrical-safety, electromagnetic-compatibility, machinery, and workplace regulations.

Common engineering errors include operating a series motor without load, weakening the field without checking overspeed, tuning the speed loop faster than the current loop, ignoring converter dead time, omitting anti-windup, and assuming that a motor can absorb regenerative energy indefinitely.

10. Contemporary Developments

Modern DC drives increasingly use digital signal processors, isolated gate drivers, high-resolution encoders, and networked diagnostics. Digital control permits adaptive current limiting, condition monitoring, parameter identification, and coordinated multi-axis operation. Data analytics can identify brush wear, commutator sparking, bearing deterioration, and abnormal current signatures. Artificial intelligence may assist predictive maintenance, but safety-critical trips should remain deterministic, validated, and independent of an opaque prediction model.

The long-term trend is replacement of brushed DC systems by induction, permanent-magnet synchronous, and switched-reluctance drives. Nevertheless, the DC motor equations remain foundational because they clearly expose the relationships among flux, current, torque, voltage, and speed that also appear in field-oriented AC-drive control.

Chapter Summary

A DC drive controls motor torque primarily through armature current and controls speed through armature voltage and field flux. The fundamental equations are Va = Ea + IaRa, Ea = kΦωm, and Te = kΦIa. Separately excited motors provide independent field and armature control; shunt motors offer good speed regulation; series motors provide very high starting torque but must not run unloaded; and permanent-magnet motors are compact and efficient but have limited field control.

Armature-voltage control produces the constant-torque region below base speed. Field weakening produces the approximately constant-power region above base speed, subject to overspeed, commutation, thermal, and demagnetization limits. Controlled rectifiers and choppers supply variable armature voltage. Cascade current–speed control gives fast torque response and regulated speed. Dynamic braking dissipates energy, regenerative braking returns energy, and plugging provides rapid braking but demands current limiting. Four-quadrant operation requires control of both voltage and current polarity and careful protection.

Key Terms

Armature voltage: Voltage applied to the motor armature.

Back emf: Generated emf opposing the applied armature voltage.

Base speed: Highest speed at rated flux and maximum permitted armature voltage.

Braking resistor: Resistor that dissipates regenerated electrical energy.

Chopper: High-frequency switch-mode DC–DC converter.

Commutation: Reversal of armature-coil current as coils pass the neutral plane.

Current loop: Fast feedback loop regulating armature current.

Dynamic braking: Braking in which generated energy is dissipated in a resistor.

Field weakening: Reduction of field flux to increase speed above base speed.

Four-quadrant drive: Drive capable of motoring and braking in both rotational directions.

Plugging: Braking by applying torque opposite to the direction of rotation through supply reversal.

Regenerative braking: Braking that returns mechanical energy to an electrical source or storage system.

Separately excited motor: Motor with an independently supplied field winding.

Series motor: Motor whose field winding carries armature current.

Shunt motor: Motor with field winding connected in parallel with the armature supply.

Speed loop: Outer feedback loop regulating motor speed.

Torque constant: Proportionality constant relating torque, flux, and armature current.

Duty ratio: Fraction of a switching period during which a chopper is on.

Review Questions

Short Answer Questions

  1. State the steady-state armature voltage equation of a separately excited DC motor.
  2. Why is armature current a suitable torque-control variable?
  3. What is meant by field weakening?
  4. Distinguish dynamic braking from regenerative braking.
  5. Why must a series motor not be operated without mechanical load?

Long Answer Questions

  1. Derive the steady-state torque–speed characteristic of a separately excited DC motor.
  2. Explain constant-torque and constant-power operation, including their practical limits.
  3. Describe the structure and purpose of cascade current and speed control.
  4. Compare controlled rectifier and chopper-fed DC drives.
  5. Explain the operation and protection requirements of a four-quadrant drive.

Analytical / Application Questions

  1. A motor has Va = 220 V, Ra = 0.4 Ω, kΦ = 1.1 V·s/rad, and load torque 33 N·m. Calculate armature current, back emf, and speed while neglecting friction.
  2. Design a control and protection arrangement for a hoist that must regenerate energy during lowering and hold its load when stopped.
  3. A drive reaches its maximum armature voltage at base speed but must operate at 1.5 times base speed. Explain how field weakening can achieve this and identify two safety limitations.

Multiple Choice Questions with Answers

Question 1

For a separately excited DC motor at steady state, which equation is correct when brush drop is neglected?

A. V_a = E_a + I_aR_a

B. V_a = E_a − I_aR_a

C. E_a = V_a + I_aR_a

D. V_a = I_a/R_a

Correct Answer: A. V_a = E_a + I_aR_a

Question 2

If field flux and armature current are constant, electromagnetic torque is

A. Inversely proportional to speed

B. Proportional to flux and armature current

C. Proportional only to armature voltage

D. Independent of armature current

Correct Answer: B. Proportional to flux and armature current

Question 3

Which control method normally provides operation below base speed in the constant-torque region?

A. Armature-voltage control at rated flux

B. Field weakening only

C. Mechanical overspeed control

D. Opening the armature circuit

Correct Answer: A. Armature-voltage control at rated flux

Question 4

For an ideal step-down chopper, the average armature voltage is

A. V_s/D

B. D/V_s

C. D V_s

D. V_s − D

Correct Answer: C. D V_s

Question 5

A series DC motor must not be operated without load primarily because

A. Its field flux becomes zero at all speeds

B. Its speed can rise to a dangerous value

C. Its armature resistance becomes infinite

D. It cannot produce starting torque

Correct Answer: B. Its speed can rise to a dangerous value

Question 6

In a cascade-controlled DC drive, the current loop is normally

A. Slower than the speed loop

B. Faster than the speed loop

C. Removed during acceleration

D. Used only during braking

Correct Answer: B. Faster than the speed loop

Question 7

Regenerative braking occurs when

A. Mechanical energy is converted to electrical energy and returned or absorbed electrically

B. All energy is dissipated in a mechanical brake

C. The field is permanently disconnected

D. The armature current is always zero

Correct Answer: A. Mechanical energy is converted to electrical energy and returned or absorbed electrically

Question 8

Forward regenerative braking corresponds to which signs of speed and torque?

A. Positive speed and positive torque

B. Positive speed and negative torque

C. Negative speed and negative torque

D. Negative speed and positive torque

Correct Answer: B. Positive speed and negative torque

Question 9

In the worked example, with TL = 36 N·m and kΦ = 1.20, the armature current is

A. 15 A

B. 24 A

C. 30 A

D. 43.2 A

Correct Answer: C. 30 A

Question 10

The principal purpose of field-loss protection in a separately excited motor is to prevent

A. Low armature resistance

B. Excessive speed caused by loss of torque-producing flux

C. Normal regenerative operation

D. Commutator voltage reversal

Correct Answer: B. Excessive speed caused by loss of torque-producing flux

Electrical Drives & Control
Chapter 5 of 14