Electrical Machines and Drives

Chapter 3
Transformers and Magnetic Devices

Bachelor Program in Mechatronics Engineering
Electrical Machines and Drives   •   Bachelor

Transformers and Magnetic Devices

Introduction and Context

Transformers are static electromagnetic devices that transfer electrical energy between circuits through mutual magnetic coupling. They change voltage and current levels, provide electrical isolation, match impedances, and enable efficient transmission and distribution of electric power. Although a transformer has no mechanical motion, its electromagnetic behavior is central to electrical drives, power converters, industrial automation, measurement systems, and renewable-energy installations.

A transformer operates with alternating current. A time-varying current in one winding establishes a changing magnetic flux in a ferromagnetic core; that flux links another winding and induces an electromotive force (emf). The ideal transformer is a useful conceptual model, but practical transformers exhibit winding resistance, leakage flux, core loss, magnetizing current, temperature rise, and waveform distortion. Engineering analysis therefore requires both ideal relationships and an equivalent circuit representing nonideal behavior.

Learning Objectives

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

  1. Explain transformer action using Faraday’s law and magnetic circuits.
  2. Derive and apply ideal-transformer voltage, current, and impedance relationships.
  3. Construct and interpret the practical equivalent circuit and phasor diagrams.
  4. Calculate voltage regulation, efficiency, losses, and approximate performance.
  5. Explain open-circuit and short-circuit tests and obtain circuit parameters from them.
  6. Analyze three-phase transformer connections, harmonics, and parallel operation.
  7. Compare two-winding transformers with autotransformers.
  8. Select and use instrument transformers safely and correctly.
  9. Evaluate transformer limitations, protection requirements, and modern applications.

1. Electromagnetic Basis of Transformer Operation

Faraday’s law states that an emf is induced when the flux linkage of a winding changes. For a winding with N turns and sinusoidal core flux of rms-related maximum value Φm and frequency f, the rms induced emf is

E = 4.44 f N Φm

Here, E is the rms induced emf in volts, f is frequency in hertz, N is the number of turns, and Φm is maximum flux in webers. The equation assumes sinusoidal flux and a sinusoidal steady state. The factor 4.44 results from integrating a sinusoidal flux waveform over a quarter cycle.

For a core of effective cross-sectional area Ac and maximum flux density Bm,

Φm = Bm Ac

Thus,

E = 4.44 f N Bm Ac

This equation shows why increasing frequency, turns, or core area increases induced emf for a specified flux density. Conversely, applying excessive voltage at low frequency can drive the core into saturation because approximately constant voltage-to-frequency ratio produces approximately constant flux:

V/f ≈ constant

The windings are usually designated primary and secondary according to the direction of energy transfer. The primary is connected to the source and the secondary to the load, although either winding may serve either role.

2. The Ideal Transformer

An ideal transformer is assumed to have:

  • zero winding resistance;
  • no leakage flux;
  • infinite core permeability, so magnetizing current is negligible;
  • no hysteresis or eddy-current loss; and
  • a perfectly coupled magnetic flux linking both windings.

Let the primary and secondary turns be N1 and N2. The turns ratio is

a = N1/N2

For an ideal transformer,

V1/V2 = N1/N2 = a

and, because input power equals output power,

I1/I2 = N2/N1 = 1/a

The signs depend on the selected dot convention and reference directions. In magnitude form, the high-voltage winding carries lower current for the same apparent power. The apparent power relationship is

S1 = S2

where S is apparent power in volt-amperes. For a balanced sinusoidal load,

S = V I

and real power is

P = V I cosθ

where θ is the phase angle between voltage and current.

Impedance Reflection

A load impedance connected to the secondary can be referred to the primary as

ZL' = a2 ZL

where ZL' is the equivalent primary-referred impedance and ZL is the actual secondary load impedance. Conversely, an impedance referred from primary to secondary is

Z' = Z/a2

This result is widely used in circuit analysis, power-system studies, and impedance matching.

Worked Example 1: Ideal Transformer

A transformer has 1000 primary turns and 100 secondary turns. The primary is supplied with 2300 V rms, and the secondary supplies a 10 Ω resistive load. Find the secondary voltage, secondary current, primary current, and input power.

The turns ratio is

a = 1000/100 = 10

Therefore,

V2 = V1/a = 2300/10 = 230 V

The secondary current is

I2 = V2/RL = 230/10 = 23 A

The ideal primary current is

I1 = I2/a = 23/10 = 2.3 A

The input power equals the output power:

P = V2 I2 = 230 × 23 = 5290 W

The transformer is therefore a step-down transformer with a 10:1 voltage ratio.

3. Practical Transformer Equivalent Circuit

A practical transformer differs from the ideal model in several ways.

Winding Resistance

Primary and secondary copper resistances, R1 and R2, cause copper losses:

Pcu = I12 R1 + I22 R2

This loss becomes heat and increases with the square of current.

Leakage Reactance

Not all flux produced by a winding links the other winding. Leakage flux produces leakage reactance, represented by X1 and X2. The series impedances are

Z1 = R1 + jX1

and

Z2 = R2 + jX2

where j = √(-1). Leakage reactance causes voltage drop and affects short-circuit current and transient performance.

Core-Loss and Magnetizing Branch

The exciting current has two components. The core-loss component supplies hysteresis and eddy-current losses; the magnetizing component establishes the core flux. These are represented by a shunt resistance Rc and magnetizing reactance Xm. The core loss is approximately

Pcore = V12/Rc

when the shunt branch is referred to the primary and the applied voltage is approximately constant. The magnetizing current is approximately

Im = V1/Xm

for a predominantly inductive magnetizing branch.

The exact equivalent circuit contains the primary series impedance, an exciting branch, an ideal transformer, and the secondary series impedance. For many calculations, all secondary quantities are referred to the primary. With turns ratio a,

R2' = a2 R2, X2' = a2 X2

The approximate series parameters are then

Req = R1 + R2'
Xeq = X1 + X2'

and

Zeq = Req + jXeq

These expressions assume that all quantities are referred to the primary. The same procedure can refer all quantities to the secondary.

4. Phasor Relationships and Voltage Regulation

Phasors represent sinusoidal quantities by magnitude and phase angle. For a lagging power-factor load, the load current lags the terminal voltage by θ. In the approximate equivalent circuit, the input voltage is approximately

V1' = V2 + I2(Req + jXeq)

when all quantities are referred to the same side. For a lagging load, the resistive drop I Req is in phase with current and the reactive drop j I Xeq leads current by 90°. For a leading load, the reactive drop can reduce the net voltage drop.

Voltage regulation measures the change in secondary voltage from no load to full load while the primary voltage remains constant:

VR = (Vno-load − Vfull-load)/Vfull-load × 100%

For a transformer with equivalent series resistance and reactance, approximate regulation is

VR ≈ (I2 Req cosθ ± I2 Xeq sinθ)/V2 × 100%

The plus sign applies to a lagging power factor and the minus sign to a leading power factor. The formula assumes small voltage drops and uses consistent quantities referred to the secondary. For a unity-power-factor load, the reactive term is zero. A leading power factor can produce negative regulation, meaning the loaded terminal voltage exceeds the no-load reference under the stated approximation.

5. Transformer Losses, Efficiency, and Loading

The principal losses are:

  1. Copper loss: proportional to current squared.
  2. Hysteresis loss: caused by repeated magnetization reversal.
  3. Eddy-current loss: caused by circulating currents in the core.
  4. Stray-load loss: caused by leakage flux inducing currents in structural parts.
  5. Dielectric loss: important in high-voltage insulation systems.

Transformer efficiency is

η = Pout/Pin × 100% = Pout/(Pout + Ploss) × 100%

For a load delivering apparent power SL at power factor cosθ,

Pout = SL cosθ

If the transformer operates at fraction x of rated current, copper loss is approximately x2 Pcu,rated, while core loss is approximately constant at fixed voltage and frequency. Therefore,

Ploss ≈ Pcore + x2 Pcu,rated

Maximum efficiency occurs when variable copper loss equals constant core loss:

Pcu = Pcore

This condition identifies the load for maximum efficiency, not necessarily the rated load. Distribution transformers are commonly designed for high efficiency at a fraction of full load because they remain energized continuously.

Worked Example 2: Efficiency and Maximum-Efficiency Loading

A transformer has a rated copper loss of 1600 W and a core loss of 400 W. At 75% load and 0.8 power factor, it supplies 100 kVA. Determine its efficiency and the load fraction for maximum efficiency.

Output power is

Pout = 100 × 0.8 = 80 kW

At x = 0.75, copper loss is

Pcu = 0.752 × 1600 = 900 W

Total loss is

Ploss = 400 + 900 = 1300 W

Thus,

η = 80,000/(80,000 + 1300) × 100% ≈ 98.40%

For maximum efficiency,

x2 × 1600 = 400

so

x = √(400/1600) = 0.5

Maximum efficiency occurs at 50% of rated load.

6. Transformer Tests

Testing determines equivalent-circuit parameters without loading the transformer at full rated power.

Open-Circuit Test

One winding is left open while rated voltage is applied to the other, usually the low-voltage winding. The measured quantities are voltage Voc, current Ioc, and power Poc. Since the current is small, series voltage drops and copper loss are usually negligible. Therefore,

Poc ≈ Pcore

The no-load power factor is

cosφoc = Poc/(Voc Ioc)

The shunt parameters referred to the test side are

Rc = Voc2/Poc
Iw = Poc/Voc
Im = √(Ioc2 − Iw2)
Xm = Voc/Im

Short-Circuit Test

One winding is short-circuited and a low voltage is applied to the other until rated current flows. The measured quantities are Vsc, Isc, and Psc. Because the applied voltage is small, core flux and core loss are negligible. Hence,

Psc ≈ Pcu,rated

The equivalent impedance is

Zeq = Vsc/Isc

The equivalent resistance is

Req = Psc/Isc2

and the equivalent reactance is

Xeq = √(Zeq2 − Req2)

The test results must be referred to the side on which the measurements were made. These tests are economical and safe when performed with appropriate protection, but they do not replace insulation, impulse, temperature-rise, or soundness tests required by applicable standards.

7. Three-Phase Transformers

Three-phase transformers may use one three-limb core or three separate single-phase units. Common connections are:

ConnectionPrincipal featuresTypical application
Y–YNeutral points available; third-harmonic issues may require a tertiary or grounded neutralBalanced systems and high-voltage applications
Δ–ΔProvides a path for triplen harmonics; can operate in open-delta at reduced capacityIndustrial loads
Y–ΔNeutral on the wye side; phase displacement between sidesTransmission and distribution
Δ–YNeutral available on wye side; common for distributionSupplying three-phase four-wire loads
ZigzagSpecial neutral and zero-sequence behaviorGrounding and harmonic reduction

For a balanced three-phase system,

S3φ = √3 VL IL

where VL and IL are line voltage and line current. The phase quantities depend on the connection. In a wye connection, VL = √3 V_φ and IL = I_φ. In a delta connection, VL = V_φ and IL = √3 I_φ.

A three-phase transformer connection introduces a phase displacement determined by winding connection and polarity. This displacement is essential when transformers are operated in parallel. Parallel transformers should have compatible voltage ratios, polarity, phase sequence, phase displacement, impedance, and per-unit characteristics. Otherwise, circulating currents or unequal load sharing can result.

8. Harmonics, Inrush, and Core Nonlinearity

The magnetizing characteristic of a ferromagnetic core is nonlinear. When the core approaches saturation, a small increase in magnetizing force produces a large increase in flux and current. Saturation can occur when the applied voltage-to-frequency ratio is excessive, when a dc component is present, or when residual flux combines unfavorably with switching conditions.

Transformer energization produces inrush current. This transient may be several times rated current and can operate protection incorrectly if relay settings do not distinguish inrush from an internal fault. Inrush contains substantial second-harmonic content in many conventional transformers, although modern transformer designs and power-electronic switching can alter this behavior.

Triplen harmonics—third, ninth, fifteenth, and so forth—are zero-sequence components in balanced three-phase systems. A delta winding provides a circulating path for these currents, preventing them from appearing freely in line currents. A grounded neutral or suitable tertiary winding can also provide a path for zero-sequence and harmonic components. Harmonic currents increase heating, acoustic noise, losses, and neutral-current stress. Transformer selection should therefore consider nonlinear loads such as rectifiers, variable-frequency drives, LED supplies, and data-center power systems.

9. Autotransformers

An autotransformer uses a single continuous winding with a portion common to both input and output. It transfers part of the power conductively and part inductively. For an ideal step-down autotransformer with input voltage VH and output voltage VL, the fraction of apparent power transferred inductively is approximately

(VH − VL)/VH

and the conductive portion is approximately

VL/VH

Compared with a two-winding transformer of the same physical size, an autotransformer can be smaller, lighter, cheaper, and more efficient for ratios near unity. Its disadvantages are the absence of complete electrical isolation and potentially higher fault current. It is used for motor starting, voltage adjustment, laboratory variable supplies, and interconnection of systems with similar voltages.

A Variac is a variable autotransformer. It must not be treated as an isolation transformer, and exposed output terminals require appropriate guarding and grounding.

10. Instrument Transformers

Instrument transformers reduce large currents or voltages to standardized values for meters, relays, and control systems while providing isolation.

Current Transformers

A current transformer (CT) is connected in series with the power circuit. Its secondary current is commonly 1 A or 5 A at rated primary current. The ideal relationship is

Np Ip ≈ Ns Is

The CT secondary must never be open-circuited while primary current flows. An open secondary can produce dangerously high voltage because the transformer attempts to maintain secondary ampere-turns and flux. CT accuracy is specified by ratio error, phase-angle error, and burden, where burden is the impedance connected to the secondary, often expressed in volt-amperes at rated current.

Potential and Voltage Transformers

A potential transformer (PT), or voltage transformer (VT), is connected across the system. It produces a lower, standardized secondary voltage. Its secondary must be protected against short circuits, and grounding practices must follow the system design and applicable standards. Capacitive voltage transformers are used at high transmission voltages and can also support communication functions.

Instrument transformers are measurement devices, not merely small power transformers. Saturation can distort relay inputs and cause protection errors during faults. Protection-class CTs are selected to remain sufficiently accurate at high fault currents, while metering-class CTs prioritize accuracy near normal operating current.

11. Applied Case: Transformer Selection for a Motor-Drive Facility

Background

This illustrative case concerns a manufacturing plant supplied at 11 kV. The plant includes induction motors driven by variable-frequency drives, welding equipment, and control systems requiring 400 V three-phase power. The existing 1 MVA transformer operates near full load and experiences overheating and nuisance protection trips.

Problem

Measurements show a peak demand of 1.05 MVA, a power factor of 0.82, and significant fifth- and seventh-harmonic currents. The plant also reports high neutral current in auxiliary low-voltage circuits. Simply installing a larger transformer without investigating waveform quality could shift, rather than solve, the problem.

Analysis

The existing transformer’s high loading increases copper loss approximately with the square of current. At 105% of its rating, the approximate copper-loss multiplier is

1.052 = 1.1025

or 110.25% of rated copper loss. Variable-frequency drives contribute harmonic current and additional stray and eddy-current heating. Welding loads create rapid changes in current and voltage. Protection trips may arise from genuine thermal overload, inrush misinterpretation, harmonic heating, or unsuitable relay coordination.

Approach and Solution

The engineering team performs synchronized measurements of rms current, demand, power factor, harmonic spectrum, temperature, and voltage distortion. It then:

  1. selects a transformer with adequate continuous and short-time capacity;
  2. specifies a low-voltage winding and grounding arrangement suitable for the plant distribution system;
  3. evaluates a K-rated or otherwise harmonic-capable transformer where justified by measured heating;
  4. provides line reactors or active harmonic filtering for selected drives;
  5. reviews neutral and bonding conductors;
  6. coordinates transformer protection with inrush characteristics and downstream faults; and
  7. verifies CT class, burden, and relay performance.

A 1.5 MVA transformer may provide operating margin, but its suitability depends on load growth, fault level, impedance, thermal performance, and utility requirements. Oversizing can increase no-load losses and fault current, so capacity alone is not a complete design criterion.

Outcome

After correcting harmonic sources and revising protection settings, transformer temperature remains within its specified limit, nuisance trips are reduced, and voltage regulation improves during motor-drive transients. The plant also adopts periodic power-quality monitoring rather than relying only on nameplate loading.

Learning Points

Transformer selection must consider apparent power, power factor, harmonics, duty cycle, grounding, fault current, ambient conditions, protection, and future expansion. A nameplate rating is necessary but not sufficient for a reliable installation.

12. Design, Safety, Standards, and Contemporary Practice

Transformers must be selected and operated according to applicable national and international standards, utility rules, and workplace-safety procedures. Important design considerations include insulation coordination, clearances, creepage distances, cooling method, altitude, ambient temperature, sound level, fire risk, oil containment, and environmental conditions.

Oil-filled transformers require attention to fire protection, leakage containment, oil quality, dissolved-gas analysis, and safe maintenance. Dry-type transformers reduce liquid-fire concerns but may require ventilation and careful control of dust and moisture. Protection commonly includes fuses or circuit breakers, overcurrent protection, differential protection, restricted earth-fault protection, temperature monitoring, pressure relief, and surge arresters, depending on rating and application.

Digital monitoring increasingly uses fiber-optic temperature sensors, online dissolved-gas analysis, partial-discharge monitoring, and asset-health models. Artificial intelligence can support anomaly detection and remaining-life estimation, but predictions require validated sensor data, engineering interpretation, cybersecurity controls, and human accountability. AI should not replace protective functions or inspection procedures without demonstrated safety compliance.

Best practice includes maintaining accurate nameplate and test records, verifying phase relationships before energization, tightening and thermographically inspecting connections, checking oil or insulation condition, controlling moisture, confirming tap-changer operation, and reviewing loading trends. Before energization, personnel must verify isolation, earthing, polarity, phasing, protection settings, and the absence of tools or personnel in hazardous zones.

Challenges and Limitations

The equivalent circuit is an approximation. Parameters vary with temperature, frequency, voltage, saturation, and load waveform. The assumption of constant core loss is most appropriate near rated voltage and frequency; it becomes inaccurate during overexcitation and transients. Leakage reactance is not always represented adequately by a single lumped value, especially in high-frequency or converter-fed applications. Harmonic analysis may require frequency-dependent winding and core models. Finally, measured efficiency and regulation depend on the exact test conditions, temperature, waveform, and power-factor definition.

Chapter Summary

A transformer transfers energy between electrical circuits through mutual induction. The ideal-transformer relationships connect turns ratio, voltage, current, power, and reflected impedance. Practical transformers require series resistance and leakage reactance to represent voltage drop and copper loss, together with a shunt core-loss resistance and magnetizing reactance.

Voltage regulation depends on equivalent resistance, leakage reactance, load current, and power factor. Efficiency is determined by output power and losses; maximum efficiency occurs when copper loss equals core loss. Open-circuit and short-circuit tests provide practical methods for finding equivalent-circuit parameters and rated losses.

Three-phase connections determine line-to-phase relationships, phase displacement, neutral availability, harmonic paths, and suitability for parallel operation. Saturation, inrush, and harmonics affect transformer heating, protection, and waveform quality. Autotransformers offer economical voltage conversion without isolation, while CTs and PTs enable safe measurement and protection but require correct burden, polarity, grounding, and operating procedures. Reliable transformer engineering combines electromagnetic analysis with thermal design, power-quality assessment, protection coordination, safety, and condition monitoring.

Key Terms

Transformer: Static device that transfers electrical energy by electromagnetic induction.

Mutual induction: Production of emf in one winding due to changing current or flux in another winding.

Turns ratio: Ratio of primary to secondary turns, a = N1/N2.

Magnetizing current: Current required to establish magnetic flux in the core.

Leakage flux: Flux linking one winding but not the other.

Leakage reactance: Reactance associated with leakage flux.

Core loss: Hysteresis and eddy-current loss in the magnetic core.

Copper loss: Resistive winding loss, proportional to current squared.

Equivalent circuit: Circuit model representing transformer nonidealities.

Impedance reflection: Conversion of an impedance from one winding side to the other by the square of the turns ratio.

Voltage regulation: Change in terminal voltage between no-load and load conditions.

Efficiency: Ratio of output power to input power.

Open-circuit test: Test used mainly to determine shunt-branch and core-loss parameters.

Short-circuit test: Test used mainly to determine series impedance and copper loss.

Inrush current: Temporary high current drawn when a transformer is energized.

Saturation: Nonlinear operating condition in which a small increase in magnetizing force causes a large current increase.

Autotransformer: Transformer using one tapped winding common to input and output.

Current transformer: Instrument transformer that produces a reduced current for measurement or protection.

Potential transformer: Instrument transformer that produces a reduced voltage for measurement or protection.

Burden: Impedance or apparent-power load connected to an instrument-transformer secondary.

Review Questions

Short Answer Questions

  1. State the assumptions of an ideal transformer.
  2. Why is a transformer core laminated?
  3. Define transformer voltage regulation.
  4. What information is obtained from the open-circuit test?
  5. Why must a current-transformer secondary not be left open-circuited?

Long Answer Questions

  1. Explain transformer operation from Faraday’s law and derive the rms emf equation for sinusoidal flux.
  2. Describe the exact and approximate equivalent circuits of a practical transformer.
  3. Explain the open-circuit and short-circuit tests, including the equations used to determine parameters.
  4. Compare Y–Y, Δ–Δ, Y–Δ, and Δ–Y three-phase transformer connections.
  5. Discuss transformer losses, efficiency, maximum-efficiency loading, and the effects of harmonics.

Analytical / Application Questions

  1. A 50 kVA transformer has core loss of 300 W and full-load copper loss of 900 W. Determine its efficiency at 80% load and 0.9 power factor, and find the load fraction for maximum efficiency.
  2. A transformer supplies a lagging-power-factor load. Explain how increasing leakage reactance affects voltage regulation, fault current, and motor-drive performance.
  3. A plant transformer overheats despite operating below its apparent-power rating. Propose a measurement and diagnostic plan that considers harmonics, ambient temperature, cooling, connections, protection, and load profile.

Multiple Choice Questions with Answers

Question 1

For an ideal transformer, if the primary-to-secondary turns ratio is 5:1 and the primary voltage is 1000 V, what is the secondary voltage?

A. 200 V

B. 500 V

C. 1000 V

D. 5000 V

Correct Answer: A. 200 V

Question 2

Which loss is approximately proportional to the square of winding current?

A. Hysteresis loss

B. Copper loss

C. Dielectric loss

D. No-load core loss

Correct Answer: B. Copper loss

Question 3

In an open-circuit transformer test, the measured power is approximately equal to which quantity?

A. Rated copper loss

B. Leakage-reactance loss

C. Core loss

D. Load power

Correct Answer: C. Core loss

Question 4

A transformer has rated copper loss of 1600 W and core loss of 400 W. At what fraction of rated load does maximum efficiency occur?

A. 25%

B. 40%

C. 50%

D. 75%

Correct Answer: C. 50%

Question 5

Which transformer connection commonly provides a neutral point on the wye side?

A. Δ–Δ

B. Y–Δ only

C. Δ–Y

D. Open-delta only

Correct Answer: C. Δ–Y

Question 6

What is the principal danger of opening a current-transformer secondary while primary current flows?

A. The primary voltage becomes zero

B. A dangerously high secondary voltage may develop

C. The core becomes perfectly lossless

D. The CT automatically becomes an autotransformer

Correct Answer: B. A dangerously high secondary voltage may develop

Question 7

For a balanced three-phase system, apparent power is given by which expression?

A. S = V_L I_L

B. S = 3V_L I_L

C. S = √3 V_L I_L

D. S = V_L/I_L

Correct Answer: C. S = √3 V_L I_L

Question 8

For a practical transformer referred to one side, the approximate series equivalent impedance consists of which components?

A. Only magnetizing reactance

B. Equivalent resistance and leakage reactance

C. Core-loss resistance in parallel with voltage

D. Only winding capacitance

Correct Answer: B. Equivalent resistance and leakage reactance

Question 9

Why can a delta winding be useful in a three-phase transformer with nonlinear loads?

A. It eliminates all copper loss

B. It provides a path for triplen-harmonic currents

C. It prevents any phase displacement

D. It guarantees unity power factor

Correct Answer: B. It provides a path for triplen-harmonic currents

Question 10

Which statement correctly distinguishes an autotransformer from a two-winding transformer?

A. An autotransformer always provides greater isolation

B. An autotransformer uses a common portion of one winding and does not provide complete electrical isolation

C. An autotransformer cannot change voltage

D. An autotransformer has no magnetic coupling

Correct Answer: B. An autotransformer uses a common portion of one winding and does not provide complete electrical isolation

Electrical Machines and Drives
Chapter 3 of 15