Sensors and Actuators

Chapter 8
Electrical Actuators and Drive Systems

Bachelor Program in Mechatronics Engineering
Sensors and Actuators   •   Bachelor

Electrical Actuators and Drive Systems

Introduction

Electrical actuators convert electrical energy into controlled mechanical motion. They are central to mechatronic systems because a controller cannot directly move a valve, wheel, robot joint, conveyor, or positioning stage; it must command an actuator through an appropriate power-electronic drive. The actuator, drive, mechanical load, sensors, and control algorithm therefore form an integrated electromechanical system.

This chapter examines the operating principles, models, selection criteria, control methods, and limitations of DC motors, AC motors, stepper motors, servo motors, brushless motors, linear motors, solenoids, relays, and electromagnetic brakes. Particular attention is given to torque–speed behavior, commutation, drive circuits, efficiency, thermal constraints, and application-level design.

Learning Objectives

By the end of this chapter, the reader should be able to:

  1. Explain how electrical energy is converted into force and torque.
  2. Model the electrical, mechanical, and thermal behavior of motor-driven systems.
  3. Compare DC, induction, synchronous, brushless, stepper, servo, and linear actuators.
  4. Select a motor and drive using torque, speed, duty cycle, accuracy, and environmental requirements.
  5. Explain commutation, PWM, inverter operation, feedback, and regenerative braking.
  6. Identify thermal, electromagnetic, safety, and reliability constraints.
  7. Analyze an actuator application and justify an engineering solution.

1. Electromechanical Energy Conversion

A motor produces torque when current-carrying conductors experience force in a magnetic field. For a rotary actuator, mechanical output power is

Pm = Tω

where Pm is mechanical power in watts, T is shaft torque in newton-metres, and ω is angular velocity in radians per second. Since radians are dimensionless, the unit is equivalent to watts.

For translational motion,

Pm = Fv

where F is force in newtons and v is linear velocity in metres per second.

In an ideal motor, electrical input power equals mechanical output power. Real motors have copper, iron, friction, windage, switching, brush, and bearing losses. Thus,

η = Pout / Pin

where η is efficiency. The equation applies to steady operation when input and output powers are measured at the same operating point.

A useful motor model separates electrical and mechanical dynamics. For a separately excited or permanent-magnet DC motor,

va = Raia + La(dia/dt) + ea
ea = keω
Te = ktia

Here va is armature voltage, ia is armature current, Ra is armature resistance, La is armature inductance, ea is back electromotive force, ke is the back-emf constant, kt is the torque constant, and Te is electromagnetic torque. In SI units, ke and kt have numerically equal values when the motor constants are expressed consistently.

The mechanical equation is

J(dω/dt) = Te - TL - Bω - Tf

where J is combined rotor and load inertia, TL is load torque, Bω represents viscous friction, and Tf represents approximately constant friction torque. The equation assumes a rigid shaft and lumped mechanical parameters.

At steady speed, acceleration is zero, so electromagnetic torque balances load and friction torque. At standstill, back emf is zero; consequently, an uncontrolled motor may draw a very large current limited mainly by winding resistance and drive current limits.

2. Torque–Speed Characteristics

Motor selection requires more than rated power. The complete operating point is defined by torque, speed, acceleration, duty cycle, and direction. A motor's torque–speed curve must be compared with the load torque–speed requirement.

For a permanent-magnet DC motor supplied by constant voltage and neglecting inductive transients,

ω ≈ (va - Raia)/ke

Since T = ktia, speed decreases approximately linearly as torque increases. The no-load speed occurs near ia = 0, while the stall torque occurs at ω = 0. This model is most useful below the base speed, where the drive can apply approximately rated voltage.

A variable-speed drive commonly operates in two regions:

  • Constant-torque region: Voltage is increased with speed so that magnetic flux remains approximately constant. Current and torque can be maintained up to the base speed.
  • Constant-power region: Above base speed, voltage is limited. Field weakening reduces flux, allowing speed to rise while available torque decreases approximately inversely with speed.

The load must also be classified. Constant-torque loads include conveyors and positive-displacement pumps. Variable-torque loads, such as centrifugal fans and pumps, approximately follow TL ∝ ω2 and power approximately follows P ∝ ω3. Constant-power loads include some winding, machine-tool, and traction applications.

Acceleration torque is

Tacc = J(dω/dt)

For a required speed change over time ∆t, assuming constant acceleration,

Tacc = J(ω2 - ω1)/∆t

The drive must provide load torque plus acceleration torque, with allowance for friction and transient overload.

3. DC Motors and Their Drives

3.1 Brushed DC motors

A brushed DC motor uses a commutator and carbon or metal-graphite brushes to reverse armature current as the rotor turns. Permanent-magnet DC motors are compact and efficient at low and medium power. Separately excited and wound-field motors provide field control and are used where wide speed ranges or high power are required.

Advantages include simple voltage-based speed control, high starting torque, and straightforward modeling. Limitations include brush wear, electrical arcing, acoustic noise, electromagnetic interference, and limited operation in explosive or contaminated environments.

3.2 DC motor drives

A DC drive may use a transistor chopper or an H-bridge. Pulse-width modulation (PWM) controls the average voltage by rapidly switching the supply. If the switching period is Ts and the switch is on for Ton, duty ratio is

D = Ton/Ts

For an ideal one-quadrant buck drive in continuous current operation,

Va,avg ≈ DVdc

where Vdc is the DC-link voltage. An H-bridge permits forward and reverse voltage and, with suitable switching, motoring and regenerative braking in four quadrants.

The bridge requires dead time to prevent simultaneous conduction of high-side and low-side switches, known as shoot-through. Current sensors, gate drivers, freewheeling paths, overcurrent protection, and undervoltage lockout are essential practical features.

4. AC Motors and Inverter Drives

4.1 Induction motors

In a three-phase induction motor, the stator produces a rotating magnetic field. Its synchronous speed is

ns = 120f/p

where ns is synchronous speed in revolutions per minute, f is supply frequency in hertz, and p is the number of poles. Rotor speed is slightly lower in motoring operation. Slip is

s = (ns - nr)/ns

where nr is rotor speed. Slip is dimensionless and is positive for motoring operation. Rotor current and torque depend strongly on slip, rotor resistance, frequency, and applied voltage.

Induction motors are rugged, inexpensive, and suitable for pumps, fans, compressors, conveyors, and industrial machinery. Their disadvantages include magnetizing current, lower low-speed torque unless controlled by an inverter, and slip-related losses.

4.2 Synchronous and permanent-magnet AC motors

A synchronous motor rotates at synchronous speed under steady-state conditions. Permanent-magnet synchronous motors (PMSMs) use rotor magnets rather than induced rotor currents. They offer high efficiency and power density but require an inverter and rotor-position information or estimation.

4.3 Variable-frequency drives

A variable-frequency drive (VFD) commonly contains a rectifier, DC link, and three-phase inverter. The inverter synthesizes variable-frequency, variable-amplitude voltages using PWM. For induction motors, scalar V/f control provides basic speed control, while field-oriented control independently regulates flux-producing and torque-producing current components. Direct-torque control regulates torque and flux more directly but can produce greater switching variation depending on implementation.

At low frequency, stator resistance causes voltage drop; therefore, voltage boost or current control may be needed to maintain flux. At excessive frequency, voltage limitation produces field weakening and reduced torque capability.

5. Brushless DC and Servo Motors

A brushless DC (BLDC) motor replaces the mechanical commutator with electronic switching. Permanent magnets are mounted on the rotor, while stator windings are energized in a controlled sequence. Hall sensors, encoders, resolvers, or sensorless estimators determine rotor position.

BLDC motors commonly use trapezoidal back emf and six-step commutation. PMSMs generally use sinusoidal back emf and sinusoidal or vector current control. The distinction is based primarily on back-emf shape and control strategy, although terminology varies across industry.

Electronic commutation must be synchronized with rotor position. Incorrect phase timing produces torque ripple, reduced efficiency, acoustic noise, and possible reverse torque. Sensorless control estimates position from back emf or observer models, but it is less reliable at zero and very low speed because back emf is small.

A servo system is not a motor type alone; it is a closed-loop motion system. It normally includes a motor, drive, position or velocity sensor, controller, mechanical transmission, and tuning parameters. A cascaded servo controller often contains:

  1. An inner current or torque loop.
  2. A middle velocity loop.
  3. An outer position loop.

The inner loop is fastest because electrical current responds more rapidly than mechanical speed, and speed responds more rapidly than position. Feedback improves accuracy and disturbance rejection but adds cost, sensor failure modes, bandwidth limitations, and tuning requirements.

6. Stepper Motors

A stepper motor moves in discrete angular increments. A two-phase hybrid stepper commonly has a toothed rotor with permanent magnetization and a toothed stator. The step angle for an ideal motor is determined by the stator and rotor tooth geometry; practical specifications are normally provided by the manufacturer.

Full-step, half-step, and microstepping drives control phase currents in different sequences. Microstepping produces smoother motion and lower audible noise, but it does not guarantee proportional absolute positioning under changing load because torque margin and detent effects remain.

Stepper motors can operate open loop, avoiding an encoder, but they may lose synchronism if commanded acceleration or load torque exceeds available pull-in or pull-out torque. Their holding current produces heat even when the shaft is stationary. A closed-loop stepper adds position feedback and can detect or correct position error.

Stepper selection must consider:

  • Required acceleration and inertia matching.
  • Pull-in and pull-out torque at the operating speed.
  • Driver current and supply voltage.
  • Resonance and vibration.
  • Holding temperature and duty cycle.
  • Whether missed steps are tolerable.

7. Linear Motors and Solenoids

A linear motor is conceptually a rotary motor unrolled into a straight path. Permanent-magnet synchronous linear motors provide direct thrust without ballscrews or belts. They offer high acceleration, low mechanical backlash, and precise positioning, but require accurate feedback, careful cable management, and attention to cogging, bearing loads, and heat removal.

A linear motor's force is commonly related to q-axis current through a force constant, in the same conceptual manner that rotary torque is related to current. The manufacturer’s force constant must be used with its specified current definition and cooling conditions.

A solenoid produces linear motion by drawing a ferromagnetic plunger into a region of lower magnetic reluctance. Its force is strongly position-dependent and generally falls as the air gap increases. Solenoids are suitable for latching, valve actuation, locking, and short-stroke mechanisms. They are poor choices for long travel or precise continuous positioning unless combined with feedback and specialized magnetic design.

A solenoid coil has resistance and inductance. The current transient is approximately

i(t) = (V/R)(1 - e-tR/L)

for a constant applied voltage, initially zero current, and constant parameters. Here R is coil resistance, L is inductance, and τe = L/R is the electrical time constant. The model neglects magnetic saturation and back emf. When a coil is switched off, stored magnetic energy can create a high voltage; a diode, TVS suppressor, or appropriately rated switching network is required.

8. Relays and Electromagnetic Brakes

An electromagnetic relay uses a coil to move an armature and change electrical contacts. Relays provide galvanic isolation and can switch loads, but contacts have finite current, voltage, inrush, arc, and life ratings. Contact bounce can generate unwanted transitions, so debouncing or suitable control logic may be required.

Solid-state relays avoid mechanical contact wear but introduce leakage current, voltage drop, heat, and sometimes limited switching speed. Relay selection must consider load type: resistive, inductive, capacitive, lamp, or motor loads can have very different inrush and interruption behavior.

Electromagnetic brakes create holding or stopping torque through magnetic attraction, friction surfaces, or eddy-current effects. Spring-applied, electrically released brakes are often selected for fail-safe holding: loss of power causes braking. Brake torque, release time, stopping energy, thermal capacity, wear, and emergency-stop requirements must be evaluated. A brake is not automatically a substitute for a safety-rated stopping system; risk assessment and applicable machinery standards remain necessary.

9. Power Electronics and Control Functions

The drive is the energy interface between the controller and actuator. Common switching devices include MOSFETs for lower-voltage, high-frequency applications; IGBTs for medium- and high-power inverter applications; and emerging wide-bandgap devices such as silicon-carbide MOSFETs and gallium-nitride devices for high-frequency, efficient conversion.

Important drive functions include:

  • Current regulation and torque limitation.
  • PWM generation and dead-time control.
  • Position and speed feedback processing.
  • Soft start and controlled stopping.
  • Overcurrent, overvoltage, undervoltage, and overtemperature protection.
  • Electromagnetic compatibility filtering.
  • Regenerative-energy management.

During regeneration, mechanical energy flows back into the electrical bus. The energy may be returned to the supply, stored in a battery or capacitor, or dissipated in a braking resistor. If the DC-link voltage rises beyond its safe limit, the drive must manage the energy or trip safely.

10. Thermal Limits and Efficiency

Motor ratings are thermal ratings as much as electromagnetic ratings. Copper loss is approximately

PCu = I2R

where I is RMS winding current and R is winding resistance at the relevant temperature. Iron, mechanical, inverter, and stray-load losses must also be considered.

A simplified steady-state thermal model is

∆T = PlossR_θ

where ∆T is temperature rise and R_θ is thermal resistance in kelvins per watt. This model assumes steady state and a linear thermal path. For transient duty, a first-order thermal model may be used:

T(t) = Tambient + PlossR_θ(1 - e-t/τth)

where τth is the thermal time constant. Real motors have multiple thermal masses, nonuniform temperature, temperature-dependent resistance, and cooling that varies with speed.

Continuous torque must be based on RMS-equivalent heating over the duty cycle. For discrete intervals with approximately constant torque-related current,

IRMS = √[(Σ Ik2tk)/(Σtk)]

where Ik is current during interval k and tk is its duration. This equation estimates copper heating when resistance and cooling are approximately constant.

11. Worked Example: Selecting a Conveyor Motor

A conveyor requires a steady belt force of 180 N at 0.8 m/s. The drive pulley radius is 0.10 m and total mechanical efficiency from motor shaft to belt is 88%. The motor must accelerate the reflected load with an additional shaft torque of 4 N·m. Select a preliminary motor rating.

The belt-side power is

Pbelt = Fv = 180 × 0.8 = 144 W

Pulley torque is

Tpulley = Fr = 180 × 0.10 = 18 N·m

The required steady motor torque, excluding acceleration torque, is

Tsteady = 18/0.88 ≈ 20.45 N·m

The motor shaft speed is

ω = v/r = 0.8/0.10 = 8 rad/s

Thus the steady motor mechanical power is

Pmotor,steady = Tsteadyω ≈ 20.45 × 8 = 163.6 W

Including acceleration torque,

Tpeak ≈ 20.45 + 4 = 24.45 N·m

A suitable motor must therefore provide approximately 20.5 N·m continuously at 8 rad/s and at least 24.5 N·m during acceleration. A design margin is required for starting friction, belt tension variation, voltage reduction, temperature, and manufacturing tolerances. The numerical result is not a complete selection: gearbox ratio, motor speed, duty cycle, inertia, brake requirements, and drive current rating must also be checked.

12. Applied Case: Robotic Joint Actuator

Background

Consider an illustrative robotic arm joint requiring accurate positioning, frequent reversals, and low backlash. The joint experiences gravity torque, acceleration torque, and external disturbance torque. It operates for repeated cycles and must hold position during power loss.

Problem

A simple open-loop stepper could provide adequate nominal holding torque, but its risk of lost steps during rapid reversal is unacceptable. The joint also requires controlled deceleration and a fail-safe holding function.

Analysis and approach

A permanent-magnet synchronous or BLDC servo motor with an absolute encoder is selected. A reduction gearbox increases output torque while reducing motor-side torque demand. The drive uses a current loop for torque control, a velocity loop, and an outer position loop. Gravity compensation reduces steady-state current, while acceleration feedforward improves tracking.

The selection process includes:

  1. Calculate maximum output torque from gravity, acceleration, friction, and disturbance.
  2. Reflect load inertia through the gearbox to the motor shaft.
  3. Verify continuous and peak motor torque against the duty cycle.
  4. Confirm encoder resolution and communication integrity.
  5. Check gearbox backlash, stiffness, efficiency, and thermal limits.
  6. Provide a spring-applied electromagnetic brake if the joint must hold safely without power.
  7. Verify emergency-stop behavior and stored regenerative energy.

Outcome

The closed-loop servo provides accurate position control and detects following error. The brake provides static holding but is not used for routine servo stopping because repeated friction-brake operation would cause wear. The drive limits current, monitors temperature, and decelerates within the available DC-bus capacity.

Learning points

The case illustrates that actuator selection is a system decision. Peak torque alone is insufficient; feedback, gearbox behavior, thermal duty, regeneration, safety, and failure response are equally important.

13. Selection Framework and Best Practices

A disciplined selection sequence is:

  1. Define motion: travel, speed, acceleration, precision, reversals, and load profile.
  2. Determine force or torque at the load and reflect it through transmissions.
  3. Calculate continuous, peak, and RMS requirements.
  4. Select actuator technology according to precision, cost, environment, and duty cycle.
  5. Match the drive voltage, current, switching frequency, feedback, and communications.
  6. Check thermal performance at the worst credible ambient condition.
  7. Assess braking, regeneration, emergency stopping, and mechanical restraint.
  8. Validate electromagnetic compatibility, noise, grounding, and cable shielding.
  9. Test stall, overload, sensor failure, loss of communication, and power interruption.
  10. Document assumptions, ratings, maintenance intervals, and replacement procedures.

Common errors include selecting by wattage alone, ignoring startup torque, confusing peak and continuous ratings, neglecting motor inertia, operating a stepper near its pull-out limit, and installing a brake without calculating stopping energy.

14. Challenges, Safety, and Contemporary Developments

Electrical actuators can create crushing, entanglement, impact, thermal, electrical, and fire hazards. A safe design uses guarded motion, current and torque limits, safe stopping functions, appropriate isolation, protective earthing, and risk assessment. Standards for machinery safety, functional safety, EMC, and electrical equipment should be identified for the application and jurisdiction.

Modern systems increasingly use integrated motor drives, networked servo amplifiers, condition monitoring, and model-based diagnostics. Edge computation can estimate bearing wear, load anomalies, or thermal aging from current, vibration, and temperature data. Machine-learning tools can assist anomaly detection, but they do not replace calibrated protection circuits, deterministic interlocks, or safety-rated controls. Cybersecurity is relevant when drives are connected to industrial networks: authentication, segmentation, secure updates, and controlled access reduce the risk of unauthorized motion.

Chapter Summary

Electrical actuators convert electrical energy into controlled force or torque, while drives regulate voltage, current, commutation, speed, position, and braking. DC motors offer simple control but require brushes; induction motors are rugged and economical; PMSM and BLDC motors provide high efficiency and power density with electronic commutation; stepper motors provide discrete motion but may lose synchronism; linear motors provide direct thrust; solenoids provide short-stroke force; relays switch electrical circuits; and electromagnetic brakes provide controlled or fail-safe stopping and holding.

Motor behavior is governed by electrical and mechanical equations, torque–speed limits, load characteristics, and thermal constraints. PWM, inverters, H-bridges, feedback sensors, current loops, and regenerative-energy management are fundamental drive technologies. Reliable selection requires analysis of continuous and peak torque, acceleration, duty cycle, inertia, efficiency, cooling, safety, EMC, and failure behavior rather than reliance on nominal power alone.

Key Terms

Actuator: Device that converts energy into controlled physical motion.

Back emf: Voltage generated by a motor’s motion that opposes the applied voltage.

BLDC motor: Permanent-magnet motor using electronic rather than mechanical commutation.

Commutation: Switching current among motor phases to maintain useful torque.

Duty cycle: Time pattern describing actuator operation and rest intervals.

Electromagnetic brake: Brake producing mechanical restraint through electromagnetic action.

Field weakening: Reduction of magnetic flux to permit operation above base speed.

H-bridge: Four-switch circuit that applies reversible voltage to a load.

Induction motor: AC motor whose rotor current is induced by the stator field.

Linear motor: Motor producing direct translational force.

PWM: Pulse-width modulation used to control average voltage or current.

Regeneration: Conversion of mechanical energy back into electrical energy.

Servo system: Closed-loop motion system using feedback for controlled position, speed, or torque.

Slip: Relative difference between synchronous speed and induction-motor rotor speed.

Solenoid: Electromagnetic actuator producing linear plunger motion.

Stepper motor: Motor that advances through discrete commanded angular steps.

Thermal resistance: Temperature rise per unit dissipated power.

Torque constant: Proportionality constant relating motor current to electromagnetic torque.

Variable-frequency drive: Power converter controlling AC motor voltage and frequency.

Review Questions

Short Answer Questions

  1. Why does a motor draw high current at startup?
  2. Define slip in an induction motor.
  3. What is the purpose of PWM in a motor drive?
  4. Why can an open-loop stepper motor lose position?
  5. What is regenerative braking?

Long Answer Questions

  1. Explain the electrical and mechanical equations of a permanent-magnet DC motor and state their assumptions.
  2. Compare brushed DC, BLDC, PMSM, induction, and stepper motors for industrial applications.
  3. Explain the operation of a variable-frequency drive and the role of the rectifier, DC link, and inverter.
  4. Discuss continuous torque, peak torque, RMS current, and thermal limits in actuator selection.
  5. Explain the architecture and advantages of a cascaded servo-control system.

Analytical / Application Questions

  1. A motor drives a constant-torque load through a gearbox. Develop a method for calculating motor torque during steady operation and acceleration, including gearbox efficiency.
  2. Design a preliminary actuator and drive specification for a robotic joint requiring frequent reversals, position feedback, emergency stopping, and power-loss holding.
  3. Compare a stepper motor and a closed-loop servo for a positioning axis. Justify the choice using accuracy, speed, torque margin, thermal behavior, cost, and safety.

Multiple Choice Questions with Answers

Question 1

Which equation represents the mechanical power of a rotary motor?

A. Pm = Tω

B. Pm = T/ω

C. Pm = ω/T

D. Pm = R/I

Correct Answer: A. Pm = Tω

Question 2

In an ideal PWM buck drive operating in continuous current mode, the average output voltage is approximately:

A. Vdc/D

B. DVdc

C. D2Vdc

D. Zero for all duty ratios

Correct Answer: B. DVdc

Question 3

What distinguishes a brushless DC motor from a brushed DC motor?

A. It cannot produce torque at zero speed

B. It uses electronic instead of mechanical commutation

C. It requires an AC transformer at its shaft

D. It has no magnetic field

Correct Answer: B. It uses electronic instead of mechanical commutation

Question 4

For a three-phase induction motor, synchronous speed depends directly on:

A. Frequency and inversely on pole number

B. Rotor resistance only

C. Bearing friction only

D. Armature inductance only

Correct Answer: A. Frequency and inversely on pole number

Question 5

A major risk of operating an open-loop stepper motor beyond its pull-out capability is:

A. Automatic increase in position accuracy

B. Loss of synchronism and missed steps

C. Zero winding temperature

D. Conversion into an induction motor

Correct Answer: B. Loss of synchronism and missed steps

Question 6

A motor produces 10 N·m torque at 20 rad/s. Its mechanical output power is:

A. 0.5 W

B. 2 W

C. 200 W

D. 2,000 W

Correct Answer: C. 200 W

Question 7

Which device is most directly suited to short-stroke electromagnetic linear actuation?

A. Solenoid

B. Induction motor rotor

C. Flywheel

D. Braking resistor

Correct Answer: A. Solenoid

Question 8

Copper winding loss is approximately proportional to:

A. I/R

B. I2R

C. R/I2

D. 1/(IR)

Correct Answer: B. I2R

Question 9

The main purpose of dead time in an inverter half-bridge is to:

A. Increase shoot-through current

B. Prevent simultaneous conduction of opposing switches

C. Eliminate all electromagnetic interference

D. Remove the need for gate drivers

Correct Answer: B. Prevent simultaneous conduction of opposing switches

Question 10

A servo system is best defined as:

A. Any motor operated without feedback

B. A closed-loop system controlling motion using feedback

C. A relay with a mechanical latch

D. A motor that operates only at synchronous speed

Correct Answer: B. A closed-loop system controlling motion using feedback

Sensors and Actuators
Chapter 8 of 14