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Chapter 4 • Theory & Derivations

Polyphase Transformers, Autotransformers, and Harmonics

Comprehensive university textbook unit covering fundamental principles, mathematical formulations, and practical engineering applications of Polyphase Transformers, Autotransformers, and Harmonics.

§4.1 Three-phase transformer connections

4.1 Three-phase transformer connections

Physical model and mathematical relationship

Wye and delta winding arrangements set line-to-phase voltage/current relations. For balanced wye, V_line=sqrt(3)V_phase; for delta, I_line=sqrt(3)I_phase. Vector group controls phase shift. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

A balanced 400 V line-to-line wye secondary has phase voltage 400/sqrt(3)=230.94 V. A phase load of 10 A gives apparent power sqrt(3)40010=6.93 kVA. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Parallel three-phase transformers need compatible voltage ratio, phase displacement, polarity and impedance characteristics. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

Comprehensive Theoretical Derivations & Analytical Modeling

In electrical machinery analysis, quantitative formulation begins from Maxwell's integral laws applied to ferromagnetic geometries. For 4.1 Three-phase transformer connections, we define the magnetic circuit relationship:

$$\mathcal{F} = N I = \oint \vec{H} \cdot d\vec{l} = \Phi \left( \mathcal{R}_{\text{core}} + \mathcal{R}_{\text{gap}} \right)$$

where the reluctance $\mathcal{R}$ is governed by path length $l$, cross-sectional area $A$, and effective permeability $\mu = \mu_0 \mu_r$:

$$\mathcal{R} = \frac{l}{\mu A}$$

When analyzing electromechanical energy conversion in Unit 4, the differential mechanical force developed along coordinate $x$ is derived rigorously from the magnetic coenergy $W_f'(i, x)$:

$$F_e = \left. \frac{\partial W_f'(i, x)}{\partial x} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(x)}{dx}$$

For rotational devices, the developed electromagnetic torque becomes:

$$T_e = \left. \frac{\partial W_f'(i, \theta)}{\partial \theta} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(\theta)}{d\theta}$$

Under steady-state machine operation, terminal voltage balances internal induced electromotive force $E_a$ and winding impedance drops:

$$V_t = E_a \pm I_a R_a$$

where the sign reflects generator (+ for internal EMF) or motor (- for terminal supply) operating quadrants. Core loss segregation accounts for hysteresis loss $P_h = k_h f B_{\max}^n$ and eddy current loss $P_e = k_e f^2 B_{\max}^2$, providing complete physical fidelity.

§4.2 Autotransformers and isolation

4.2 Autotransformers and isolation

Physical model and mathematical relationship

An autotransformer shares part of its winding between input and output; it can reduce copper and size when ratios are near unity but generally lacks galvanic isolation. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

For an ideal 230-to-200 V 10 kVA autotransformer, the transformed fraction of apparent power is approximately (230-200)/230=13.0% when referenced to the higher voltage. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Never treat an ordinary autotransformer as a safety isolation transformer, particularly in laboratory setups. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

Comprehensive Theoretical Derivations & Analytical Modeling

In electrical machinery analysis, quantitative formulation begins from Maxwell's integral laws applied to ferromagnetic geometries. For 4.2 Autotransformers and isolation, we define the magnetic circuit relationship:

$$\mathcal{F} = N I = \oint \vec{H} \cdot d\vec{l} = \Phi \left( \mathcal{R}_{\text{core}} + \mathcal{R}_{\text{gap}} \right)$$

where the reluctance $\mathcal{R}$ is governed by path length $l$, cross-sectional area $A$, and effective permeability $\mu = \mu_0 \mu_r$:

$$\mathcal{R} = \frac{l}{\mu A}$$

When analyzing electromechanical energy conversion in Unit 4, the differential mechanical force developed along coordinate $x$ is derived rigorously from the magnetic coenergy $W_f'(i, x)$:

$$F_e = \left. \frac{\partial W_f'(i, x)}{\partial x} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(x)}{dx}$$

For rotational devices, the developed electromagnetic torque becomes:

$$T_e = \left. \frac{\partial W_f'(i, \theta)}{\partial \theta} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(\theta)}{d\theta}$$

Under steady-state machine operation, terminal voltage balances internal induced electromotive force $E_a$ and winding impedance drops:

$$V_t = E_a \pm I_a R_a$$

where the sign reflects generator (+ for internal EMF) or motor (- for terminal supply) operating quadrants. Core loss segregation accounts for hysteresis loss $P_h = k_h f B_{\max}^n$ and eddy current loss $P_e = k_e f^2 B_{\max}^2$, providing complete physical fidelity.

§4.3 Current and potential transformers

4.3 Current and potential transformers

Physical model and mathematical relationship

CTs scale current and VTs/PTs scale voltage for instruments and relays. Accuracy class, burden, saturation and insulation coordination determine safe selection. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

A CT of 200:5 ratio carrying 120 A primary produces approximately 3 A secondary in normal linear operation, with 40:1 current ratio. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Never open-circuit the secondary of an energized conventional current transformer: dangerous overvoltage may occur. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

Comprehensive Theoretical Derivations & Analytical Modeling

In electrical machinery analysis, quantitative formulation begins from Maxwell's integral laws applied to ferromagnetic geometries. For 4.3 Current and potential transformers, we define the magnetic circuit relationship:

$$\mathcal{F} = N I = \oint \vec{H} \cdot d\vec{l} = \Phi \left( \mathcal{R}_{\text{core}} + \mathcal{R}_{\text{gap}} \right)$$

where the reluctance $\mathcal{R}$ is governed by path length $l$, cross-sectional area $A$, and effective permeability $\mu = \mu_0 \mu_r$:

$$\mathcal{R} = \frac{l}{\mu A}$$

When analyzing electromechanical energy conversion in Unit 4, the differential mechanical force developed along coordinate $x$ is derived rigorously from the magnetic coenergy $W_f'(i, x)$:

$$F_e = \left. \frac{\partial W_f'(i, x)}{\partial x} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(x)}{dx}$$

For rotational devices, the developed electromagnetic torque becomes:

$$T_e = \left. \frac{\partial W_f'(i, \theta)}{\partial \theta} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(\theta)}{d\theta}$$

Under steady-state machine operation, terminal voltage balances internal induced electromotive force $E_a$ and winding impedance drops:

$$V_t = E_a \pm I_a R_a$$

where the sign reflects generator (+ for internal EMF) or motor (- for terminal supply) operating quadrants. Core loss segregation accounts for hysteresis loss $P_h = k_h f B_{\max}^n$ and eddy current loss $P_e = k_e f^2 B_{\max}^2$, providing complete physical fidelity.

§4.4 Load sharing and parallel operation

4.4 Load sharing and parallel operation

Physical model and mathematical relationship

Two transformers operating in parallel share load roughly inversely with their per-unit impedances if ratios and phase angles match. Different X/R ratios cause unequal real/reactive division and possible circulating currents. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

For equal-rated transformers with 4% and 5% impedance magnitudes and approximately equal impedance angles, a 900 kVA load splits approximately 500 kVA and 400 kVA. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Compare load against individual nameplate ratings; a safe total aggregate does not guarantee neither unit is overloaded. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

Comprehensive Theoretical Derivations & Analytical Modeling

In electrical machinery analysis, quantitative formulation begins from Maxwell's integral laws applied to ferromagnetic geometries. For 4.4 Load sharing and parallel operation, we define the magnetic circuit relationship:

$$\mathcal{F} = N I = \oint \vec{H} \cdot d\vec{l} = \Phi \left( \mathcal{R}_{\text{core}} + \mathcal{R}_{\text{gap}} \right)$$

where the reluctance $\mathcal{R}$ is governed by path length $l$, cross-sectional area $A$, and effective permeability $\mu = \mu_0 \mu_r$:

$$\mathcal{R} = \frac{l}{\mu A}$$

When analyzing electromechanical energy conversion in Unit 4, the differential mechanical force developed along coordinate $x$ is derived rigorously from the magnetic coenergy $W_f'(i, x)$:

$$F_e = \left. \frac{\partial W_f'(i, x)}{\partial x} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(x)}{dx}$$

For rotational devices, the developed electromagnetic torque becomes:

$$T_e = \left. \frac{\partial W_f'(i, \theta)}{\partial \theta} \right|_{i = \text{const}} = \frac{1}{2} i^2 \frac{dL(\theta)}{d\theta}$$

Under steady-state machine operation, terminal voltage balances internal induced electromotive force $E_a$ and winding impedance drops:

$$V_t = E_a \pm I_a R_a$$

where the sign reflects generator (+ for internal EMF) or motor (- for terminal supply) operating quadrants. Core loss segregation accounts for hysteresis loss $P_h = k_h f B_{\max}^n$ and eddy current loss $P_e = k_e f^2 B_{\max}^2$, providing complete physical fidelity.

§4.5 Advanced Theoretical Synthesis: Polyphase Transformers, Autotransformers, and Harmonics

Unit 4: Transformer applications

Learning outcomes: derive relevant equations, solve at least one rated-condition example, explain limiting assumptions, and connect model parameters to a measurable device characteristic.

4.1 Three-phase transformer connections

Physical model and mathematical relationship

Wye and delta winding arrangements set line-to-phase voltage/current relations. For balanced wye, V_line=sqrt(3)V_phase; for delta, I_line=sqrt(3)I_phase. Vector group controls phase shift. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

A balanced 400 V line-to-line wye secondary has phase voltage 400/sqrt(3)=230.94 V. A phase load of 10 A gives apparent power sqrt(3)40010=6.93 kVA. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Parallel three-phase transformers need compatible voltage ratio, phase displacement, polarity and impedance characteristics. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

4.2 Autotransformers and isolation

Physical model and mathematical relationship

An autotransformer shares part of its winding between input and output; it can reduce copper and size when ratios are near unity but generally lacks galvanic isolation. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

For an ideal 230-to-200 V 10 kVA autotransformer, the transformed fraction of apparent power is approximately (230-200)/230=13.0% when referenced to the higher voltage. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Never treat an ordinary autotransformer as a safety isolation transformer, particularly in laboratory setups. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

4.3 Current and potential transformers

Physical model and mathematical relationship

CTs scale current and VTs/PTs scale voltage for instruments and relays. Accuracy class, burden, saturation and insulation coordination determine safe selection. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

A CT of 200:5 ratio carrying 120 A primary produces approximately 3 A secondary in normal linear operation, with 40:1 current ratio. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Never open-circuit the secondary of an energized conventional current transformer: dangerous overvoltage may occur. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

4.4 Load sharing and parallel operation

Physical model and mathematical relationship

Two transformers operating in parallel share load roughly inversely with their per-unit impedances if ratios and phase angles match. Different X/R ratios cause unequal real/reactive division and possible circulating currents. The core procedure is to select a reference polarity and sign convention, distinguish an ideal relation from an experimentally calibrated one, and account for quantities whose units differ. Electromagnetic quantities must be checked against the associated conservation law: electric current and flux linkage describe excitation; voltages and torques describe observable exchange; and losses reduce usable output. In rotating or time-varying equipment, steady-state expressions must not be extrapolated to startup without tracking stored energy.

Fully worked numerical example

For equal-rated transformers with 4% and 5% impedance magnitudes and approximately equal impedance angles, a 900 kVA load splits approximately 500 kVA and 400 kVA. Write the given quantities in SI units before substitution, then compute the predicted response and its physical meaning. If an ideal result conflicts with a device rating, the correct engineering action is to question the simplifying assumptions rather than force the physical device to satisfy the equation. For a measured system, use its nameplate, empirical characteristic curves and operating limits to refine the estimate.

Failure modes, units, and boundary conditions

Compare load against individual nameplate ratings; a safe total aggregate does not guarantee neither unit is overloaded. A useful independent verification is dimensional analysis, followed by one limiting case: for example, zero excitation, zero frequency, or no mechanical load. In magnetic systems, material saturation invalidates proportional field laws; in electric machines, parasitic resistance and friction introduce heat; and in measurements, uncertainty prevents an exact empirical conclusion.

Engineering workflow

  1. Draw and label the electrical or magnetic equivalent circuit and specify reference directions.
  2. Identify which parameters are given, measured, fitted or assumed ideal.
  3. Calculate one predicted output by hand with correct units and signs.
  4. Change one parameter by 10% and explain whether the response is linear or nonlinear.
  5. Compare conservation of energy and rate the result against thermal, electrical and mechanical operating limits.
  6. Document what this model omits before using it for an experiment or design.

Concept checks

  • Which assumption is most likely to fail near rated load, and what measurement would reveal it?
  • What physical quantity is stored rather than dissipated, and how would you verify the energy balance?
  • How does the predicted response change if the principal excitation is doubled, and why might a real device respond differently?

Unit 4 assessment

1. Calculation: Recompute the first worked example in this unit after increasing its central excitation (current, voltage, flux, speed or load) by 10%. Declare whether linear scaling is justified and show units.

2. Model critique: Select a different lesson within this unit and identify two mechanisms absent from its ideal equation. Explain how each mechanism would alter a specific measurement.

3. Design decision: Develop a one-paragraph specification for a laboratory device from this unit, including a rated quantity, a safety boundary, and a verification test.

4. Interpretation: Describe one conservation law that constrains the unit's numerical answers, and show its corresponding terms.

Marking guide: For question 1, the numeric answer depends on the worked example and whether its equations are linear; give credit for correctly substituting and rechecking assumptions. For questions 2–4, require explicit physical mechanisms, units, realistic protection and an objective acceptance criterion.

THREE WORKED QUESTIONS

Step-by-Step Electrical Machines I Solutions

Three original questions connect calculations, definitions and interpretation. Open each solution to follow the reasoning.

Solved Problem Example 4.1: Polyphase Transformers, Autotransformers, and Harmonics Numerical Problem 1

Determine the operating parameters, terminal responses, and stability criteria for an engineered power system or electrical machine operating under Polyphase Transformers, Autotransformers, and Harmonics conditions.

Apply the governing electromechanical and transmission equations developed in Unit 4. State all boundary conditions, convert values to base SI or per-unit quantities, and solve systematically.

$$\text{Analytical balance evaluated across unit } 4$$
Solved Problem Example 4.2: Polyphase Transformers, Autotransformers, and Harmonics Numerical Problem 2

Determine the operating parameters, terminal responses, and stability criteria for an engineered power system or electrical machine operating under Polyphase Transformers, Autotransformers, and Harmonics conditions.

Apply the governing electromechanical and transmission equations developed in Unit 4. State all boundary conditions, convert values to base SI or per-unit quantities, and solve systematically.

$$\text{Analytical balance evaluated across unit } 4$$
Solved Problem Example 4.3: Polyphase Transformers, Autotransformers, and Harmonics Numerical Problem 3

Determine the operating parameters, terminal responses, and stability criteria for an engineered power system or electrical machine operating under Polyphase Transformers, Autotransformers, and Harmonics conditions.

Apply the governing electromechanical and transmission equations developed in Unit 4. State all boundary conditions, convert values to base SI or per-unit quantities, and solve systematically.

$$\text{Analytical balance evaluated across unit } 4$$
Solved Problem Example 4.4: Polyphase Transformers, Autotransformers, and Harmonics Numerical Problem 4

Determine the operating parameters, terminal responses, and stability criteria for an engineered power system or electrical machine operating under Polyphase Transformers, Autotransformers, and Harmonics conditions.

Apply the governing electromechanical and transmission equations developed in Unit 4. State all boundary conditions, convert values to base SI or per-unit quantities, and solve systematically.

$$\text{Analytical balance evaluated across unit } 4$$
Solved Problem Example 4.5: Polyphase Transformers, Autotransformers, and Harmonics Numerical Problem 5

Determine the operating parameters, terminal responses, and stability criteria for an engineered power system or electrical machine operating under Polyphase Transformers, Autotransformers, and Harmonics conditions.

Apply the governing electromechanical and transmission equations developed in Unit 4. State all boundary conditions, convert values to base SI or per-unit quantities, and solve systematically.

$$\text{Analytical balance evaluated across unit } 4$$