Electrical Power System

Chapter 4
Fault Analysis and Grounding

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Electrical Power System   •   Post Graduate

4. Fault Analysis and Grounding

Introduction and Context

Electrical power systems are designed to operate close to balanced, steady-state conditions. Generation, transmission, and distribution equipment are selected for normal voltage, current, frequency, and thermal loading. A fault abruptly changes these conditions. Conductors may short together, a conductor may contact earth, or insulation failure may create a high-impedance path. The resulting current can be several times the rated current of the equipment and can produce severe thermal, mechanical, dielectric, and safety consequences.

Fault analysis therefore serves two related purposes. First, it determines currents and voltages during abnormal conditions so that circuit breakers, busbars, cables, transformers, generators, and current transformers can be correctly rated. Second, it provides the electrical quantities needed to design protection systems that detect and isolate faults selectively and rapidly. Grounding is inseparable from this task because the method by which system neutrals are connected to earth strongly influences fault current, overvoltages, protection sensitivity, and public safety.

Balanced three-phase faults can be studied using ordinary single-phase equivalents. Unbalanced faults cannot generally be treated in this way. Symmetrical components transform an unbalanced set of phasors into positive-, negative-, and zero-sequence sets, allowing the system to be represented by sequence networks. This chapter develops that method, applies it to common fault types, and examines the engineering decisions associated with neutral grounding.

Learning Objectives

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

1. Distinguish symmetrical and unsymmetrical faults and identify their electrical consequences.

2. Explain the physical meaning of positive-, negative-, and zero-sequence components.

3. Construct and interconnect sequence networks for common fault conditions.

4. Calculate fault currents and voltages for three-phase, line-to-line, single-line-to-ground, and double-line-to-ground faults.

5. Determine short-circuit duties and relate them to equipment interrupting and withstand ratings.

6. Compare solid, resistance, reactance, resonant, and isolated-neutral grounding.

7. Evaluate grounding choices in relation to protection, overvoltage, continuity, and safety.

8. Recognize practical modelling assumptions, common errors, and emerging computational practices.

The Physical Nature of Power-System Faults

A fault is an abnormal electrical connection between conductors or between a conductor and earth. Faults may be permanent, such as a failed cable termination, or transient, such as a flashover caused by lightning or contamination. They may be bolted, with negligible impedance, or arcing and high impedance, in which case the actual current is lower than the prospective bolted-fault current.

The principal fault categories are:

  • Three-phase fault: all three phase conductors are involved, with or without earth. It is balanced and usually produces the highest current.
  • Line-to-line fault: two phase conductors are connected without earth.
  • Single-line-to-ground fault: one phase is connected to earth. It is the most frequent fault in many systems.
  • Double-line-to-ground fault: two phases are connected to earth, directly or through an impedance.

Fault current is not constant. Immediately after a fault, synchronous machines contribute a subtransient current governed by their subtransient reactances. This current decays through transient and synchronous stages. In addition, an ac component may be accompanied by a decaying dc offset determined by the point on the voltage wave at which the fault occurs and by the system X/R ratio. Consequently, a breaker must withstand both the symmetrical rms current and the asymmetrical peak and rms currents associated with dc offset.

A useful first approximation for a three-phase fault at a bus is

\[

I_f=\frac{V_{LL}}{\sqrt{3}Z_{th}},

\]

where \(V_{LL}\) is the prefault line-to-line voltage and \(Z_{th}\) is the Thevenin impedance seen from the fault location. In per-unit form, if the prefault voltage is approximately 1.0 per unit,

\[

I_f=\frac{1}{Z_{th,pu}}.

\]

This approximation is appropriate for many planning and rating studies, but detailed protection studies must represent machine models, transformers, lines, grounding impedances, fault resistance, and time-dependent reactances.

Symmetrical Components: Transforming the Problem

An unbalanced set of three phasors can be resolved into three balanced sets. For phase quantities \(I_a,I_b,I_c\),

\[

\begin{bmatrix}I_a\\I_b\\I_c\end{bmatrix}=

\begin{bmatrix}1&1&1\\1&a^2&a\\1&a&a^2\end{bmatrix}

\begin{bmatrix}I_0\\I_1\\I_2\end{bmatrix},

\qquad a=1\angle120^\circ.

\]

The inverse transformation is

\[

\begin{bmatrix}I_0\\I_1\\I_2\end{bmatrix}=\frac{1}{3}

\begin{bmatrix}1&1&1\\1&a&a^2\\1&a^2&a\end{bmatrix}

\begin{bmatrix}I_a\\I_b\\I_c\end{bmatrix}.

\]

The three components have distinct physical meanings:

  • Positive sequence consists of three equal phasors, displaced by 120 degrees, with the normal phase sequence a-b-c. It represents the balanced operating field and is the sequence primarily associated with normal power transfer.
  • Negative sequence has equal magnitudes and reverse phase sequence a-c-b. Negative-sequence currents induce double-frequency currents in rotating-machine rotors and can cause rapid rotor heating.
  • Zero sequence consists of three equal phasors in phase. It can flow only when a return path exists through neutrals, earth, cable sheaths, transformer windings, or grounded structural paths.

The sequence impedances \(Z_1,Z_2,Z_0\) are the impedances experienced by positive-, negative-, and zero-sequence currents. For static balanced components such as lines and transformers, \(Z_1\) and \(Z_2\) are often similar, although machine negative-sequence impedance is distinct. Zero-sequence impedance is strongly dependent on winding connection, core construction, grounding, earth-return geometry, and metallic paths.

The sequence-network approach replaces an unbalanced three-phase circuit with three single-phase networks. Positive-sequence sources are normally present because generators produce positive-sequence voltage. Negative- and zero-sequence networks are usually source-free and contain only impedances, except where special converter or control behaviour is explicitly modelled.

Sequence Networks of System Components

For a synchronous generator, the positive-sequence network contains the internal emf behind the appropriate subtransient, transient, or synchronous reactance. The negative-sequence network contains the generator negative-sequence impedance, and the zero-sequence network depends on the stator winding connection and neutral grounding impedance. If a generator neutral impedance is \(Z_n\), its contribution in the zero-sequence network is conventionally represented as \(3Z_n\), because the neutral current is \(3I_0\).

For a transformer, positive- and negative-sequence currents see impedances close to the transformer leakage impedance. Zero-sequence current depends on winding connections. A grounded wye winding provides a zero-sequence path; an ungrounded wye winding blocks it. A delta winding permits circulating zero-sequence current within the delta but does not pass zero-sequence line current through to the other side. Thus, transformer vector group and grounding must be represented explicitly in fault studies.

For overhead lines and cables, positive- and negative-sequence impedances are usually similar. Zero-sequence impedance is generally higher because the return path includes earth, shield wires, cable sheaths, or parallel metallic conductors. Mutual coupling between circuits can also affect zero-sequence quantities and earth-fault relay performance.

In per-unit analysis, all impedances should be converted to a common MVA and voltage base. For a change of base,

\[

Z_{pu,new}=Z_{pu,old}\left(\frac{S_{base,new}}{S_{base,old}}\right)

\left(\frac{V_{base,old}}{V_{base,new}}\right)^2.

\]

Consistent base selection is one of the simplest ways to reduce calculation errors in interconnected systems.

Fault Conditions and Sequence-Network Interconnections

Three-Phase Fault

For a balanced fault, only the positive-sequence network is involved. If the prefault positive-sequence voltage at the fault is \(E\),

\[

I_1=\frac{E}{Z_1+Z_f},\qquad I_2=0,\qquad I_0=0,

\]

where \(Z_f\) is the fault impedance in the equivalent positive-sequence circuit. For a bolted fault, \(Z_f=0\). The phase currents are equal in magnitude and separated by 120 degrees. Although this fault is less frequent than earth faults, it often determines the maximum breaker interrupting duty.

Line-to-Line Fault

Consider a fault between phases b and c through impedance \(Z_f\), with no earth connection. At the fault, \(I_a=0\) and \(I_b=-I_c\). These conditions imply

\[

I_0=0,\qquad I_1=-I_2.

\]

The positive- and negative-sequence networks are connected in series, and

\[

I_1=\frac{E}{Z_1+Z_2+Z_f'},

\]

where the exact form of \(Z_f'\) depends on the phase-domain definition of fault impedance. For a bolted line-to-line fault, the commonly used phase-current magnitude is

\[

|I_{LL}|=\frac{\sqrt{3}|E|}{|Z_1+Z_2|}.

\]

Zero sequence is absent because no current returns through earth or a neutral path.

Single-Line-to-Ground Fault

For an a-phase-to-ground fault through impedance \(Z_f\), the three sequence currents are equal:

\[

I_0=I_1=I_2.

\]

The three sequence networks are therefore connected in series. The fault current is

\[

I_a=3I_0=\frac{3E}{Z_1+Z_2+Z_0+3Z_f}.

\]

This equation shows directly why neutral grounding and zero-sequence impedance are decisive. A solidly grounded system may produce a large earth-fault current, whereas a resistance-grounded system deliberately limits it. The phase currents in the unfaulted phases are zero at the ideal fault point, but their voltages and currents elsewhere in the network need not be zero.

Double-Line-to-Ground Fault

For a b-c-ground fault, the phase-a current at the fault is zero, while phases b and c carry currents whose sum returns through ground. All three sequence networks participate, but their interconnection differs from the series arrangement of the single-line-to-ground fault. In a standard derivation, the positive-sequence network is in series with the parallel combination of the negative- and zero-sequence networks, modified by the fault impedance. For a bolted fault, a convenient form is

\[

I_1=\frac{E}{Z_1+\frac{Z_2Z_0}{Z_2+Z_0}},

\]

with \(I_2\) and \(I_0\) obtained from the parallel-network voltage and the phase currents reconstructed using the symmetrical-component transformation. Because the result depends strongly on \(Z_0\), the double-line-to-ground current may be greater or less than the line-to-line current and is not safely estimated by a universal rule.

The sequence method is most reliable when the fault boundary conditions are written first. A common error is to memorize network diagrams without checking which phase currents are constrained to zero, equal, or opposite values.

Short-Circuit Duties and Equipment Ratings

Fault calculations support several distinct equipment decisions. The interrupting rating of a circuit breaker is the rms symmetrical current it can interrupt under specified voltage, power factor, and operating conditions. The momentary or close-and-latch rating relates to the peak electromagnetic force and the ability to close onto a fault. The short-time withstand rating specifies the current that equipment can carry for a stated duration without unacceptable thermal or mechanical damage. These ratings must not be confused.

The asymmetrical current can be represented approximately by

\[

i(t)=\sqrt{2}I_{sym}\sin(\omega t+\alpha-\phi)+I_{dc,0}e^{-t/\tau},

\]

where the time constant \(\tau=L/R\) reflects the system X/R ratio. High X/R systems have slowly decaying dc components and therefore larger first-cycle asymmetry. Breaker selection must use the applicable standard procedures rather than only the symmetrical rms fault current.

Fault level is often expressed in short-circuit MVA:

\[

S_{sc}=\sqrt{3}V_{LL}I_{sc},

\]

or, in per unit, approximately \(S_{sc,pu}=1/Z_{th,pu}\) on the selected base. A high fault level means a stiff network and demands higher equipment ratings. A low fault level may reduce equipment duty but create voltage depression and protection-coordination challenges.

Fault studies should consider maximum and minimum system configurations. Maximum generation and parallel lines generally produce the highest fault current. Minimum generation, open tie lines, and inverter-limited sources may produce the lowest current and are critical for relay sensitivity. Motor contributions, transformer tap positions, network topology, and future expansion should be included where material.

Neutral Grounding as an Engineering Choice

Grounding is the intentional connection of a system neutral, equipment frame, or other conductive part to earth or to a grounding network. System grounding controls the relationship between circuit conductors and earth; equipment grounding bonds exposed conductive parts so that a fault produces a safe protective response. These functions are related but should not be confused.

Solid Grounding

In solid grounding, the neutral is connected to earth with negligible intentional impedance. Single-line-to-ground faults can be large, allowing fast operation of overcurrent and differential protection. The disadvantages are high thermal and mechanical stress, greater touch and step potentials near the fault, and possible damage at the fault point. Solid grounding is common in many high-voltage and effectively grounded transmission and distribution systems where rapid fault clearing is essential.

Resistance Grounding

A neutral grounding resistor limits earth-fault current. Low-resistance grounding permits a substantial current, often sufficient for selective relaying, while high-resistance grounding limits current to a small value and may permit continued operation for a single ground fault under controlled conditions. The resistor must be rated for the fault current and clearing duration, and the system must include ground-fault detection. High-resistance grounding is particularly useful for industrial systems where continuity is important, but it does not eliminate arc-flash or touch-voltage hazards.

Reactance Grounding

A reactor in the neutral limits ground-fault current. It can be economical at high power levels, but the inductive nature of the path may produce transient overvoltages and resonance concerns. Its suitability depends on system capacitance, protection requirements, and transient performance.

Resonant or Petersen-Coil Grounding

A reactor tuned approximately to compensate the system's capacitive earth-fault current can reduce the residual current at a single-line-to-ground fault. This may allow arc extinction in overhead networks. Detuning, changing network topology, and protection discrimination must be carefully managed. Resonant grounding is a system-level control problem rather than merely a choice of a neutral resistor.

Isolated or Ungrounded Systems

An isolated neutral does not intentionally connect the system to earth. A first earth fault may produce limited current, but the healthy phases can experience elevated phase-to-earth voltages, especially during intermittent arcing faults. Insulation stress and transient overvoltage can be severe. Such systems require insulation monitoring and disciplined fault-location procedures; they should not be interpreted as inherently safe.

Grounding design must balance fault-current magnitude, transient overvoltage, relay sensitivity, continuity of service, equipment damage, arc-flash energy, electromagnetic interference, and personnel exposure. There is no universally optimum grounding method.

Safety, Protection, and Professional Practice

The primary safety principle is rapid removal of dangerous fault energy while maintaining a low-impedance, reliable path for protective current. Protective bonding, grounding-electrode systems, equipotential bonding, touch- and step-voltage control, and periodic testing are essential. A grounding conductor should not be sized solely by normal load current; it must withstand the prospective fault current for the clearing time and satisfy the governing standard.

Protection engineers must distinguish system ground current from current through a particular relay. Transformer connections, CT saturation, cable sheath currents, parallel grounding paths, and mutual coupling can cause these quantities to differ. CT saturation during high-current faults may delay or distort differential and overcurrent protection. Relay settings should therefore be verified using realistic fault simulations rather than nominal equations alone.

Digital relays now calculate symmetrical components directly and can apply directional earth-fault, negative-sequence, distance, differential, and adaptive protection functions. Phasor measurement units and synchronized measurements support system-wide disturbance analysis. Electromagnetic-transient programs can represent inverter controls, frequency dependence, travelling waves, and arc models more accurately than classical short-circuit programs. Nevertheless, software does not replace engineering judgement: model validation, base consistency, data quality, and sensitivity studies remain essential.

Inverter-based resources introduce additional complexity. Their fault current may be limited in magnitude, controlled by converter software, and dependent on voltage, current limits, control mode, and grid strength. The classical assumption that every generator behaves as a voltage source behind a fixed reactance may therefore be inappropriate. Protection and grounding studies for converter-rich systems should use manufacturer-validated models and examine both grid-following and grid-forming behaviour where relevant.

Illustrative Applied Case: Ground-Fault Study at an Industrial Bus

Background

Consider an illustrative 11-kV industrial bus supplied by a utility transformer and two induction-motor groups. The plant initially uses a solidly grounded transformer neutral. The utility requests that the plant limit earth-fault damage and reduce arc-flash exposure while preserving dependable fault detection.

Situation and Analysis

A preliminary study represents the utility and transformer by a positive-sequence Thevenin impedance of 0.12 per unit, with \(Z_2\approx0.12\) per unit and zero-sequence impedance of 0.36 per unit. For a bolted single-line-to-ground fault with solid grounding and a prefault voltage of 1.0 per unit,

\[

I_{LG,pu}=\frac{3}{0.12+0.12+0.36}=5.0\;pu.

\]

The high current produces substantial thermal and arc energy. A line-to-line fault, using the same positive- and negative-sequence impedances, would have a phase-current magnitude proportional to \(\sqrt{3}/(0.12+0.12)\), demonstrating that the fault type producing the greatest phase current need not be the most severe for every equipment or protection measure.

The plant evaluates a high-resistance neutral grounding system. In the zero-sequence network, the resistor contributes \(3Z_n\). If its value is selected so that the total single-line-to-ground current is limited to approximately 10 A on the actual system base, the resistor must be rated for the full current and specified duration. A ground-fault relay and insulation-monitoring scheme are added, and the plant establishes a controlled procedure for locating the first fault.

Approach and Solution

The engineering team compares three alternatives: retain solid grounding, install low-resistance grounding, or install high-resistance grounding. Low-resistance grounding provides stronger relay current and faster selective tripping but leaves higher arc energy. High-resistance grounding minimizes damage and may permit controlled continuity, but it requires reliable monitoring and a clear policy for clearing the first fault. The selected solution includes a grounding resistor, a neutral grounding transformer where necessary, a resistor temperature monitor, sensitive ground-fault protection, bonded equipment frames, and verification of touch voltages.

Outcome

The revised design reduces prospective earth-fault current and improves the probability that a fault will be detected before extensive equipment damage occurs. It does not remove the need for arc-flash boundaries, personal protective equipment, maintenance, or prompt fault clearance. The study also identifies that motor contributions must be included in breaker momentary-duty checks even though they decay rapidly.

Learning Points

The case illustrates that grounding is a coordinated design decision. Reducing fault current can improve equipment survival but may make relay operation more difficult. Protection, resistor duty, insulation monitoring, equipment bonding, and operating procedures must be designed as one system.

Common Errors, Limitations, and Governance Considerations

Frequent analytical errors include using line-to-line voltage where phase voltage is required, omitting the factor of three in neutral impedance, assuming \(Z_0=Z_1\), ignoring transformer winding connections, mixing per-unit bases, and applying a three-phase-fault formula to an earth fault. Another error is using the maximum fault current for all purposes. Minimum fault current is often more important for relay sensitivity, while maximum asymmetrical current governs mechanical duty.

The classical method assumes a prefault balanced system, linear impedances, a specified fault type, and adequate network data. It may not represent arc resistance, saturation, frequency-dependent line behaviour, converter controls, or evolving faults. Results should therefore be accompanied by assumptions, source data, fault resistance scenarios, and uncertainty or sensitivity ranges.

Grounding and protection decisions are subject to electrical-safety legislation, installation codes, utility requirements, and applicable equipment standards. Professional responsibility includes documenting assumptions, using certified equipment, maintaining test records, protecting workers from foreseeable arc-flash and touch-voltage hazards, and ensuring that changes in network topology trigger a review of protection settings. Cost reduction must never be achieved by weakening protective bonding or omitting fault-detection functions.

Best-Practice Workflow for Fault Studies

A defensible study normally follows this sequence:

1. Define the study purpose, voltage levels, operating cases, fault types, fault impedance range, and required outputs.

2. Assemble and verify the single-line diagram, equipment ratings, transformer connections, cable data, generator and motor models, grounding arrangements, and protection settings.

3. Select consistent MVA and voltage bases and convert all impedances.

4. Build positive-, negative-, and zero-sequence networks, checking the physical paths for zero-sequence current.

5. Calculate maximum and minimum fault currents, including relevant source and motor contributions.

6. Convert results to breaker interrupting, close-and-latch, short-time, busbar, cable, transformer, and arc-flash duties.

7. Test relay sensitivity, selectivity, CT performance, and clearing times.

8. Perform sensitivity studies for topology, generation dispatch, fault resistance, grounding impedance, and model uncertainty.

9. Compare calculated duties with equipment ratings and document required modifications.

10. Validate the model through commissioning tests, disturbance records, and periodic review after system changes.

Chapter Summary

Fault analysis determines the currents, voltages, equipment duties, and protection requirements created by abnormal connections in a power system. Three-phase faults are balanced and use only the positive-sequence network, whereas unsymmetrical faults require positive-, negative-, and zero-sequence networks. Symmetrical components transform unbalanced phase quantities into three balanced sets and provide a systematic method for calculating line-to-line, single-line-to-ground, and double-line-to-ground faults.

Zero-sequence behaviour is controlled by transformer connections, generator neutrals, line and cable return paths, and grounding impedances. In a single-line-to-ground fault, the sequence networks are in series and the fault current includes the factor of three associated with neutral current. Short-circuit studies must distinguish symmetrical interrupting current from asymmetrical peak, close-and-latch, and short-time withstand duties.

Grounding is a design compromise among fault-current limitation, protection sensitivity, transient overvoltage, service continuity, equipment damage, arc energy, and personnel safety. Solid, resistance, reactance, resonant, and isolated-neutral systems each have appropriate applications and risks. Modern digital relays and advanced simulation tools improve analysis, but accurate data, validated models, standards compliance, and professional judgement remain fundamental.

Key Terms

Symmetrical fault: A fault producing equal three-phase currents displaced by 120 degrees.

Unsymmetrical fault: A fault whose three phase currents or voltages are unequal or not normally displaced.

Positive sequence: Balanced phasors with the normal phase sequence and forward rotating field.

Negative sequence: Balanced phasors with reverse phase sequence.

Zero sequence: Three equal, in-phase phasors.

Sequence impedance: Impedance presented to a specified sequence current.

Thevenin impedance: Equivalent impedance seen from the fault location toward the source network.

Bolted fault: An ideal fault with negligible fault impedance.

Fault resistance: Resistance associated with an arc, contact, or other fault path.

Short-circuit MVA: Apparent power associated with a specified short-circuit current and voltage.

Interrupting rating: Maximum specified current a breaker can interrupt safely.

Short-time withstand rating: Current an apparatus can carry for a specified short duration.

Asymmetrical current: Fault current containing ac and decaying dc components.

Solid grounding: Neutral grounding through negligible intentional impedance.

Resistance grounding: Neutral grounding through a resistor selected to limit earth-fault current.

Reactance grounding: Neutral grounding through an intentional reactor.

Resonant grounding: Grounding using a tuned reactor to compensate capacitive earth current.

Touch voltage: Voltage between an accessible object and a person’s point of contact with earth.

Zero-sequence path: The complete conductive route required for zero-sequence current.

Per-unit system: A normalized representation of electrical quantities on selected common bases.

Review Questions

Short Answer Questions

1. Why is the zero-sequence impedance of a transformer dependent on its winding connections?

2. State the physical meaning of positive-, negative-, and zero-sequence currents.

3. Why does a single-line-to-ground fault current contain a factor of three?

4. Distinguish interrupting rating from short-time withstand rating.

5. Identify two reasons for studying minimum as well as maximum fault current.

Long Answer Questions

1. Explain the symmetrical-component transformation and derive the sequence conditions for a single-line-to-ground fault.

2. Describe the sequence networks of a synchronous generator, transformer, and transmission line.

3. Compare solid, resistance, reactance, resonant, and isolated-neutral grounding with respect to protection, safety, and continuity.

4. Explain how dc offset and system X/R ratio affect circuit-breaker duty.

5. Develop a complete workflow for an industrial short-circuit and grounding study.

Analytical / Application Questions

1. A bus has \(Z_1=0.20\) pu, \(Z_2=0.20\) pu, and \(Z_0=0.50\) pu, with a prefault voltage of 1.0 pu. Calculate the bolted single-line-to-ground current in per unit and explain how adding a neutral impedance changes the result.

2. A transformer has a grounded-wye primary and delta secondary. Determine whether zero-sequence line current can pass from the primary to the secondary, and explain the implications for an earth-fault study.

3. An industrial plant proposes high-resistance grounding to reduce arc energy. Evaluate the protection, monitoring, operating, and safety measures that must accompany the proposal.

22. Multiple Choice Questions with Answers

Question 1

Which sequence components are present in an ideal three-phase balanced fault?

A. Positive sequence only

B. Negative sequence only

C. Zero sequence only

D. All three sequences in equal magnitude

Correct Answer: A. Positive sequence only

Question 2

For a single-line-to-ground fault, what is the relationship among the three sequence currents at the fault?

A. I1 = -I2 and I0 = 0

B. I0 = I1 = I2

C. I1 = I2 = 0

D. I0 = -I1 = -I2

Correct Answer: B. I0 = I1 = I2

Question 3

Why is a neutral impedance represented as 3Zn in the zero-sequence network?

A. Three neutral conductors are always used

B. Zero-sequence voltage is three times phase voltage

C. Neutral current equals 3I0

D. The transformer ratio triples the impedance

Correct Answer: C. Neutral current equals 3I0

Question 4

Which transformer connection generally blocks zero-sequence line current from passing through to the other side?

A. Grounded-wye to grounded-wye

B. Grounded-wye to delta

C. Ungrounded-wye to grounded-wye

D. Delta to delta with a grounded neutral

Correct Answer: B. Grounded-wye to delta

Question 5

A high system X/R ratio mainly causes which short-circuit effect?

A. Faster decay of the dc component

B. A larger and more persistent dc offset

C. Elimination of negative-sequence current

D. Reduction of the symmetrical rms current to zero

Correct Answer: B. A larger and more persistent dc offset

Question 6

If the Thevenin impedance at a bus is 0.25 pu and prefault voltage is 1.0 pu, the approximate three-phase fault current is:

A. 0.25 pu

B. 1.25 pu

C. 4.0 pu

D. 25 pu

Correct Answer: C. 4.0 pu

Question 7

Which grounding method intentionally uses a tuned reactor to compensate capacitive earth-fault current?

A. Solid grounding

B. Resistance grounding

C. Reactance grounding

D. Resonant grounding

Correct Answer: D. Resonant grounding

Question 8

Why can an isolated-neutral system experience serious insulation stress during an earth fault?

A. It always produces the maximum fault current

B. Healthy-phase voltages to earth may rise substantially

C. It eliminates all transient overvoltages

D. It forces positive-sequence current through the neutral

Correct Answer: B. Healthy-phase voltages to earth may rise substantially

Question 9

Which study case is especially important for checking relay sensitivity?

A. Maximum generation and all lines in service only

B. Minimum fault current and high fault resistance

C. Three-phase bolted fault only

D. Maximum motor contribution only

Correct Answer: B. Minimum fault current and high fault resistance

Question 10

In a single-line-to-ground fault, increasing the zero-sequence impedance while other quantities remain fixed will generally:

A. Increase the ground-fault current

B. Leave the ground-fault current unchanged

C. Decrease the ground-fault current

D. Convert the fault into a line-to-line fault

Correct Answer: C. Decrease the ground-fault current

Electrical Power System
Chapter 4 of 15