Electrical Machines and Drives

Chapter 10
Electric Drive Mechanics and System Design

Bachelor Program in Mechatronics Engineering
Electrical Machines and Drives   •   Bachelor

Electric Drive Mechanics and System Design

Introduction

An electric drive is an electromechanical system that converts electrical energy into controlled mechanical motion. A complete drive includes a motor, power converter, controller, sensors, mechanical transmission, load, protection, and auxiliary equipment. Motor selection based only on rated power is inadequate: the motor must also satisfy starting torque, acceleration time, speed range, braking requirements, thermal duty, overload capability, and mechanical-interface constraints.

The central design task is to match the motor–converter combination to the load over the complete operating cycle. This requires a mechanical model linking torque, speed, inertia, friction, disturbances, and transmitted power. The same model supports commissioning, fault diagnosis, energy estimation, and safety analysis.

Learning objectives

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

  1. Construct torque–speed and power–speed models for common loads.
  2. Calculate equivalent inertia, acceleration torque, and acceleration time.
  3. Analyse motoring, generating, braking, and four-quadrant operation.
  4. Select mechanical transmissions and account for their efficiency and inertia.
  5. Apply RMS torque and thermal-duty methods to preliminary motor sizing.
  6. Select converters, sensors, brakes, and auxiliaries as parts of an integrated drive.
  7. Evaluate a drive design against performance, safety, and maintainability requirements.

1. Mechanical model of an electric drive

For rotational motion, Newton’s law gives the net torque required to change speed:

J\frac{d\omega}{dt}=Tm-TL-Tf-Td

Here, J is total rotational inertia in kg·m², ω is angular speed in rad/s, Tm is motor torque in N·m, TL is useful load torque, Tf is friction torque, and Td represents other opposing or disturbance torques. The equation assumes a rigid single-shaft model and uses positive torque in the selected direction of rotation.

The acceleration torque is therefore

Tacc=J\frac{d\omega}{dt}=Tm-Tres

where Tres=TL+Tf+Td. Acceleration occurs only when motor torque exceeds resisting torque. At steady speed, dω/dt=0, so motor torque equals the total resisting torque.

Mechanical power is

Pm=Tmω

with Pm in watts, torque in N·m, and speed in rad/s. If speed is given in revolutions per minute,

ω=\frac{2πn}{60}

where n is speed in r/min. The product of N·m and rad/s has units of watts because the radian is dimensionless.

Torque–speed characteristics of loads

Load torque commonly follows one of four models:

Load typeTypical relationExamples
Constant torqueTL≈constantconveyors, hoists, positive-displacement pumps
Fan or pumpTL∝ω2fans, centrifugal pumps
Constant powerTL=PL/ωmachine tools, traction over a speed range
Coulomb/friction dominatedapproximately constant opposing torquesliding mechanisms, heavily loaded gearboxes

For a fan or centrifugal pump, affinity laws approximately give Q∝ω, H∝ω2, and P∝ω3, where Q is flow, H is pressure or head, and P is power. These relations apply when geometry and fluid conditions remain comparable; they are not universal laws for every pump system.

The intersection of the motor torque–speed curve and the load torque–speed curve determines the operating point. A stable operating point generally requires that a small increase in speed produce a reduction in accelerating torque, so that the system returns toward equilibrium.

2. Inertia and mechanical transmission

The total inertia referred to the motor shaft includes the motor rotor, couplings, gears, drums, rollers, and reflected translational mass. For a translational mass m connected to a shaft through a wheel of radius r,

Jref=mr2

This follows from equating translational kinetic energy, (1/2)mv2, to rotational kinetic energy, (1/2)Jω2, with v=rω.

For an ideal gear pair with motor speed ωm, load speed ωL, and ratio i=ωm/ωL, load inertia referred to the motor is

JL,ref=\frac{JL}{i2}

where JL is load-side inertia. The corresponding load torque referred to the motor is approximately TL,ref=TL/(ηg i), where ηg is gearbox efficiency. The inertia-reflection relation assumes a rigid transmission and the stated speed-ratio convention; backlash, compliance, and shaft torsion require a multi-mass model.

For a belt, chain, or gear system, efficiency must be included separately in power and torque calculations. A transmission does not eliminate energy loss: approximately,

PL=ηgPm

in motoring operation. During regenerative power flow, efficiency and loss directions may differ and must be checked using the manufacturer’s data.

Acceleration time

If accelerating torque is constant,

tacc=\frac{J(ω2-ω1)}{Tm-Tres}

This is a useful preliminary equation. If torque varies with speed, the more general expression is

tacc=\intω1ω2\frac{J\,dω}{Tm(ω)-Tres(ω)}

The denominator must remain positive throughout the interval. Near a speed where motor and load torque become equal, acceleration time becomes very large, indicating that the selected drive may not reach the target speed.

Worked example: acceleration of a conveyor

A conveyor has total motor-referred inertia of 0.80 kg·m². Its motor supplies 42 N·m while the opposing torque is 12 N·m. It accelerates from 0 to 1,500 r/min. The net accelerating torque is 30 N·m. First convert speed:

ω2=2π(1500)/60=157.1 rad/s.

Thus,

tacc=0.80×157.1/30=4.19 s.

The result assumes constant torque and neglects changes in friction and converter current limits. If a four-second acceleration is required, this motor–drive pair is marginal and should be evaluated with tolerances, not merely nominal values.

3. Four-quadrant operation and braking

A speed–torque plane is divided into four quadrants. Let positive speed denote forward rotation and positive torque denote torque in the forward direction.

  • Quadrant I: positive speed and positive torque—forward motoring.
  • Quadrant II: positive speed and negative torque—forward regenerative braking.
  • Quadrant III: negative speed and negative torque—reverse motoring.
  • Quadrant IV: negative speed and positive torque—reverse regenerative braking.

Motoring converts electrical energy to mechanical energy. Regeneration converts mechanical energy back through the motor and converter into electrical energy. Regenerated energy may be returned to the supply, stored in a battery or capacitor, or dissipated in a braking resistor. A standard diode-front-end inverter usually cannot return energy to an AC supply without an active front end or another regenerative arrangement.

Braking methods

Regenerative braking provides controlled negative torque and can recover energy. It requires a converter capable of accepting reverse power and a destination for that power.

Dynamic braking directs DC-link or motor energy to a resistor. It is robust but converts energy into heat. The resistor must satisfy both peak-power and thermal-energy ratings.

DC-injection braking applies a stationary magnetic field to an AC motor after the rotating field is removed. It is useful for stopping but normally does not provide efficient energy recovery and can overheat the motor if applied excessively.

Mechanical braking uses a friction brake. It is essential for holding a suspended load, emergency stopping, or safely maintaining position when electrical torque cannot be guaranteed. A friction brake should not be treated as a routine substitute for controlled electrical braking unless the duty and wear are explicitly designed.

The kinetic energy available at speed ω is

Ek=\frac{1}{2}Jω2

If a brake must stop the system from ω1 to ω2, the change in kinetic energy is

∆Ek=\frac{1}{2}J(ω12-ω22)

Additional energy may come from a descending load or process force. Braking-resistor sizing must consider peak instantaneous power, allowable voltage, pulse duration, repetition rate, and cooling.

Safety implications

A drive that can regenerate must control DC-link overvoltage, overspeed, and loss of braking capability. Hoists and vertical axes require a spring-applied, electrically released brake or an equivalent safety architecture in many applications. Emergency-stop design must follow applicable machinery and electrical-safety standards, risk assessment, and the required stop category; software-only stopping is not automatically a safe torque-off function.

4. Speed ranges and motor operating regions

A motor’s operating envelope usually contains a constant-torque region and, above base speed, a constant-power region. In the constant-torque region, flux and current can generally be maintained so that torque is available over the lower speed range. Above base speed, voltage becomes limiting; field weakening reduces available torque approximately in inverse proportion to speed, while power remains approximately constant:

T≈\frac{P}{ω}

This approximation applies only within the motor’s field-weakening capability and thermal limits. It must not be extended to zero speed, where the equation would imply infinite torque.

The required operating envelope should be plotted against the motor’s permissible torque–speed curve. Important boundaries include rated continuous torque, short-time overload torque, maximum speed, voltage limit, current limit, commutation or inverter limit, and thermal limit. The converter must also support the required current, voltage, switching frequency, braking path, and control mode.

5. Thermal limits and duty cycles

Electrical losses heat the motor and converter. Motor copper loss is approximately proportional to current squared, while iron, mechanical, and stray-load losses vary with speed, voltage, and frequency. A thermal model may be expressed as

Cth\frac{dθ}{dt}=Ploss-\frac{θ-θa}{Rth}

where Cth is thermal capacitance in J/K, θ is motor temperature, θa is ambient temperature, Rth is thermal resistance in K/W, and Ploss is heat generation in watts. The model assumes lumped temperature and approximately constant parameters.

At steady state,

θ-θa=PlossRth

For repeated operation, an initial screening method is equivalent RMS torque:

Trms=\sqrt{\frac{\sumk=1NTk2tk}{\sumk=1Ntk}}

This method is appropriate when motor losses are reasonably represented by torque-squared dependence and speed-related losses are not dominant. For a drive with substantial speed variation, regenerative operation, or intermittent cooling, a thermal model is more reliable.

The selected motor should satisfy both:

  1. peak torque and current during acceleration, disturbances, and braking; and
  2. continuous or RMS thermal capability over the complete duty cycle.

A motor can meet the average power requirement and still fail because of repeated starts, insufficient cooling at low speed, high ambient temperature, blocked ventilation, or excessive overload duration.

Duty-cycle categories

A continuous-duty load may operate at constant load until thermal equilibrium. An intermittent-periodic load alternates load and rest periods. A short-time duty operates for a limited time followed by sufficient cooling. Variable-load duty requires evaluation of each segment, including acceleration and braking. Standard motor duty classifications should be consulted when specifying the motor, but the actual process cycle remains the decisive input.

6. Integrated drive-system design

A sound design begins with a requirements table rather than a catalogue search. The table should include:

RequirementDesign question
MotionWhat speed, position, direction, and accuracy are required?
LoadWhat is the torque–speed curve, inertia, friction, and disturbance torque?
DynamicsWhat acceleration, deceleration, settling time, and overshoot are acceptable?
DutyWhat is the complete cycle, including idle and braking intervals?
EnvironmentWhat are ambient temperature, dust, moisture, altitude, vibration, and enclosure needs?
SafetyIs holding, safe stop, overspeed protection, or redundant feedback required?
InterfaceWhat voltage, communication, shaft, mounting, and maintenance provisions exist?

Motor and converter selection

The motor must provide the required continuous torque at the operating speed and sufficient peak torque for transient conditions. The converter must be selected for motor current, voltage, overload duration, switching and cooling conditions, control method, and regenerative energy. Converter ratings may be derated by ambient temperature, altitude, carrier frequency, enclosure, and installation arrangement.

For a three-phase motor, a preliminary electrical input estimate is

Pin≈\frac{Pout}{ηmηc}

where ηm and ηc are motor and converter efficiencies. This is an estimate, not a substitute for manufacturer efficiency maps. Apparent power, power factor, harmonic current, and supply protection must also be checked.

Feedback and sensors

Speed feedback may use an encoder, resolver, Hall sensor, or sensorless estimator. Position accuracy, low-speed torque, disturbance rejection, and safety integrity often determine the choice. An encoder must be matched to shaft speed, resolution, electrical interface, cable length, vibration, and contamination. Torque may be measured directly with a torque transducer or estimated from current and motor parameters; estimation is convenient but sensitive to parameter variation and sensor offset.

Limit switches, proximity sensors, temperature sensors, DC-link measurement, brake-status switches, and safe-torque-off inputs are often necessary auxiliaries. Sensor placement should measure the variable that matters: a motor-side encoder cannot detect all backlash or belt slip at the load.

Mechanical and structural design

Shafts, keys, couplings, gear teeth, belts, and bearings must withstand steady torque, peak torque, shock loads, and reversing fatigue. Coupling misalignment and torsional resonance can create oscillation even when the static torque calculation is satisfactory. Flexible couplings reduce alignment sensitivity but may introduce compliance. Backlash affects positioning and can amplify impact during reversals.

7. Worked design example: indexing conveyor

Consider an illustrative indexing conveyor with a 0.20 m radius drive pulley. The transported mass and equivalent belt mass total 120 kg. The pulley and transmission inertia referred to the pulley is 0.60 kg·m². The conveyor must accelerate from rest to 1.2 m/s in 0.8 s. Constant resisting force is 180 N. A gearbox has ratio i=10 and efficiency ηg=0.92. The motor is connected to the gearbox input.

Step 1: Pulley speed

ωL=v/r=1.2/0.20=6.0 rad/s.

The motor speed is ωm=iωL=60 rad/s, or approximately 573 r/min.

Step 2: Equivalent inertia at the pulley

The translational mass reflected to the pulley is

Jtrans=mr2=120(0.20)2=4.80 kg·m2.

Thus total pulley-side inertia is JL=4.80+0.60=5.40 kg·m². Referred to the motor,

Jref=5.40/102=0.054 kg·m².

Step 3: Acceleration torque

The pulley angular acceleration is αL=6.0/0.8=7.5 rad/s2. The pulley-side acceleration torque is JLαL=5.40×7.5=40.5 N·m. Resisting torque at the pulley is Tres,L=Fr=180×0.20=36 N·m. Therefore required pulley torque is 76.5 N·m.

The corresponding motor torque, including gearbox efficiency, is

Tm=76.5/(0.92×10)=8.32 N·m.

The motor must provide at least 8.32 N·m during acceleration, with engineering margin for uncertainty, starting friction, and control response. At constant speed, the motor torque falls to

Tm,steady=36/(0.92×10)=3.91 N·m.

The steady mechanical output at the motor shaft at 60 rad/s is approximately P=3.91×60=235 W. The acceleration condition, not the steady power alone, is likely to govern peak torque. A complete selection would additionally evaluate cycle repetition, motor cooling, gearbox service factor, brake requirements, and the converter’s overload rating.

8. Case study: vertical packaging axis

Background

An illustrative packaging machine raises a 35 kg carriage through 0.45 m, positions it, and returns it. The axis operates 20 cycles per minute. A servo motor and belt transmission are considered.

Problem

The design team initially proposes a motor selected from average mechanical power. During testing, the axis stalls near the upper position and the motor overheats during repeated cycling.

Analysis

Average power hides two critical effects. First, the gravitational torque is present throughout lifting and must be included in the motor-side torque. Second, repeated acceleration and deceleration produce peak current and RMS heating. Belt compliance also causes position error when the carriage reverses.

The design review constructs a complete cycle with position, speed, acceleration, gravity, friction, and transmission efficiency. Motor-side inertia is calculated from the carriage mass and pulley radius. The required peak torque is compared with the servo’s short-time torque curve, while RMS torque is compared with the continuous thermal rating. Downward motion is analysed as regeneration rather than assumed to be a zero-power return stroke.

Approach and solution

The revised design uses a larger servo, a regenerative-capable drive, a spring-applied holding brake, an encoder on the motor, and a load-side home and limit-sensor arrangement. The controller applies an S-curve speed profile to reduce jerk and belt excitation. A braking resistor is retained as a controlled fallback for energy that cannot be returned to the DC bus.

Outcome

The revised system meets the cycle time without thermal overload, maintains position after power removal through the brake, and prevents the DC bus from exceeding its voltage limit during descent. Commissioning includes verification of brake timing, encoder direction, limit-switch operation, safe torque off, and abnormal-load stopping.

Learning points

Average power is not sufficient for cyclic motion. Vertical loads require explicit gravity and holding analysis. Regenerative energy must have a controlled destination. Feedback location and mechanical compliance influence actual positioning performance. Safety functions must be tested as system functions, not assumed from individual component labels.

9. Challenges, limitations, and best practices

The rigid single-inertia model is valuable for first design but can fail when shafts, belts, or couplings are flexible. A two-mass model may be required for torsional resonance and vibration-control design. Manufacturer torque curves may assume specific voltage, cooling, duty, and ambient conditions. Catalogue ratings should therefore be interpreted with their test conditions.

Common design errors include ignoring reflected inertia, using rated motor power instead of torque at the required speed, neglecting braking energy, treating a gearbox as lossless, omitting low-speed cooling derating, and selecting an encoder without considering load-side backlash. Another error is assuming that a software stop is equivalent to a safety-rated stop.

Best practice is to:

  • define the complete motion and duty cycle;
  • calculate both peak and thermal requirements;
  • include tolerances, friction variation, and worst-case load;
  • verify four-quadrant energy flow and DC-link management;
  • check mechanical resonance, backlash, and shaft strength;
  • specify sensors and auxiliaries as functional parts of the drive;
  • validate the design by simulation, calculation, and controlled testing;
  • document assumptions, parameter limits, protective functions, and maintenance procedures.

Digital models and AI-based monitoring can assist with load identification, bearing-fault detection, and remaining-useful-life estimation. They do not remove the need for physical limits, validated sensors, deterministic protection, or engineering accountability. A learned model should never be the sole barrier against overspeed, crushing, suspended-load drop, or electrical shock.

Chapter Summary

Electric-drive design is a system problem involving motor torque, load torque, inertia, speed, transmission, converter limits, thermal duty, sensors, braking, and safety. Newton’s rotational equation determines acceleration, while torque–speed intersection determines operating points. Translational masses and load inertias can be referred to the motor shaft using speed-ratio relationships, but compliance and backlash may require multi-mass models.

Four-quadrant operation distinguishes forward and reverse motoring from regenerative braking. Braking energy must be returned, stored, or dissipated, and vertical axes generally require an independent holding function. Motor selection must satisfy peak torque, continuous or RMS thermal demand, speed range, and environmental derating. Converter, feedback, brake, and protection choices must be made together with the mechanical design. The most reliable workflow begins with the complete duty cycle and ends with documented verification of performance and safety.

Key Terms

Torque: Rotational force, measured in N·m.

Angular speed: Rotational speed in rad/s.

Inertia: Resistance to change in rotational speed, measured in kg·m².

Acceleration torque: Net torque available to change speed.

Load torque: Torque demanded by the driven mechanism.

Reflected inertia: Load inertia expressed at another shaft through a transmission.

Gear ratio: Ratio relating motor speed to load speed.

Transmission efficiency: Ratio of useful transmitted power to input power.

Constant-torque load: Load whose required torque is approximately independent of speed.

Constant-power region: Speed range in which torque decreases approximately inversely with speed.

Regenerative braking: Braking in which mechanical energy is converted to electrical energy.

Dynamic braking: Dissipation of braking energy in a resistor.

Four-quadrant operation: Operation allowing both directions of speed and torque.

Duty cycle: Time sequence of load, speed, acceleration, and rest conditions.

RMS torque: Thermal-equivalent torque calculated over a duty cycle.

Thermal resistance: Temperature rise per unit heat flow, in K/W.

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

Safe torque off: Safety function that prevents torque production when correctly implemented.

Backlash: Mechanical clearance that causes lost motion during reversal.

Review Questions

Short Answer Questions

  1. State the rotational equation governing acceleration in an electric drive.
  2. Why is motor rated power alone insufficient for motor selection?
  3. Define regenerative braking and identify one requirement for its use.
  4. What is meant by reflected inertia?
  5. State the two principal thermal requirements checked during drive sizing.

Long Answer Questions

  1. Explain the four quadrants of the torque–speed plane and relate each quadrant to energy conversion.
  2. Derive the reflected translational inertia relation using kinetic energy.
  3. Compare regenerative, dynamic, DC-injection, and mechanical braking.
  4. Explain how a complete duty cycle is used to assess motor thermal capability.
  5. Discuss why a flexible transmission may require a multi-mass mechanical model.

Analytical / Application Questions

  1. A motor accelerates a load with known total inertia from one speed to another while motor and resisting torques vary with speed. Formulate the integral required to determine acceleration time and state the condition for successful acceleration.
  2. Design a preliminary braking strategy for a vertical axis that must stop repeatedly and hold its load after power loss. Identify energy, control, mechanical, and safety issues.
  3. For a conveyor with a gearbox, calculate motor-side peak torque and steady torque from given mass, pulley radius, acceleration time, resistance, gear ratio, and efficiency. Explain which result governs peak converter current and which governs continuous thermal loading.

Multiple Choice Questions with Answers

Question 1

For a rigid rotational drive, what condition produces acceleration?

A. Motor torque is less than resisting torque

B. Motor torque equals zero

C. Motor torque exceeds resisting torque

D. Speed is independent of torque

Correct Answer: C. Motor torque exceeds resisting torque

Question 2

A 100 kg translational mass connected to a shaft by a 0.10 m radius pulley has what reflected inertia at the pulley shaft?

A. 0.1 kg·m²

B. 1.0 kg·m²

C. 10 kg·m²

D. 100 kg·m²

Correct Answer: B. 1.0 kg·m²

Question 3

Which quadrant represents positive speed and negative torque?

A. Forward motoring

B. Forward regenerative braking

C. Reverse motoring

D. Reverse regenerative braking

Correct Answer: B. Forward regenerative braking

Question 4

What is the main purpose of a braking resistor?

A. To increase motor flux

B. To dissipate braking energy as heat

C. To reduce gearbox backlash

D. To measure shaft position

Correct Answer: B. To dissipate braking energy as heat

Question 5

For a fan under comparable operating conditions, load torque is approximately proportional to:

A. ω⁻¹

B. ω

C. ω²

D. ω³

Correct Answer: C. ω²

Question 6

A motor runs at 1,200 r/min. Its angular speed is approximately:

A. 20 rad/s

B. 62.8 rad/s

C. 120 rad/s

D. 7,200 rad/s

Correct Answer: B. 62.8 rad/s

Question 7

Which quantity is most directly associated with repeated thermal loading over a duty cycle?

A. Peak position

B. RMS torque

C. Gear ratio only

D. Encoder resolution only

Correct Answer: B. RMS torque

Question 8

Above base speed in a typical field-weakening region, motor torque generally:

A. Increases in direct proportion to speed

B. Remains infinite

C. Decreases approximately inversely with speed

D. Becomes independent of power

Correct Answer: C. Decreases approximately inversely with speed

Question 9

Why is a mechanical brake often required on a vertical axis?

A. To improve encoder resolution

B. To hold the load when electrical torque is unavailable

C. To eliminate all motor losses

D. To increase supply frequency

Correct Answer: B. To hold the load when electrical torque is unavailable

Question 10

If a gearbox speed ratio is defined as motor speed divided by load speed, load inertia referred to the motor is:

A. J_L i²

B. J_L/i²

C. J_L/i

D. J_L+ i²

Correct Answer: B. J_L/i²

Electrical Machines and Drives
Chapter 10 of 15