UNIT 5: HIGH VOLTAGE ENGINEERING - EXAM-FOCUSED NOTES
I. FUNDAMENTALS OF HIGH VOLTAGE TECHNOLOGY
Definition and Significance
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High Voltage (HV): Typically > 1 kV AC or 1.5 kV DC.
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Classification:
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HV: 1 kV – 36 kV (AC)
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EHV: 72.5 kV – 245 kV (AC)
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UHV: ≥ 800 kV (AC) / ≥ 600 kV (DC)
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Significance in Power Systems:
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Enables long-distance power transmission with reduced I²R losses (P = VI).
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Allows higher power transfer through a given conductor cross-section.
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Essential for substations, transformers, and switchgear insulation coordination.
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Applications
| Category | Applications |
|---|---|
| Power | Transmission lines, Substations, Power transformers, Circuit breakers, Instrument transformers, Insulators |
| Non-Power | X-ray tubes, Particle accelerators, Electrostatic precipitators (pollution control), Ozone generators, Food processing, Material surface treatment |
Need for HV Generation in Laboratories
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Insulation Testing: Type tests, routine tests, acceptance tests on equipment (cables, transformers, insulators).
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Research & Development: Studying breakdown mechanisms, new insulating materials.
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Calibration: Standardizing HV measuring instruments (sphere gaps, dividers).
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Simulating Overvoltages: Generating power frequency, switching impulse, and lightning impulse voltages to test equipment withstand capability.
[!TIP] Exam Focus: Be ready to list both power and non-power applications. Link HV generation directly to testing standards (IEC, IS).
II. BREAKDOWN MECHANISMS IN DIELECTRICS
Gaseous Dielectrics: Townsend's Theory
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Primary Ionization: Free electron (from natural radiation) gains energy from electric field, collides with neutral molecule → ionization (new electron + positive ion). Described by Townsend's first ionization coefficient (α): number of ionizing collisions per unit length.
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Secondary Ionization: Positive ions drift to cathode, cause secondary electron emission (via ion impact, photon impact). Described by Townsend's second ionization coefficient (γ): number of secondary electrons emitted per incident positive ion.
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Breakdown Condition: Avalanche growth becomes self-sustaining.
$$ \boxed{e^{\alpha d} = 1 + \frac{1}{\gamma}} $$
For large gaps, simplified to **αd ≈ constant** (typically 15-20).
Streamer Theory (for Non-Uniform Fields)
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Improvement over Townsend: Explains fast breakdown (nanoseconds) in highly non-uniform fields (e.g., rod-plane gap).
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Mechanism:
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Electron avalanche develops.
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Space charge of ions distorts the electric field at avalanche head.
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Field enhancement at the tip creates a conductive ionized channel (streamer) that propagates rapidly towards the anode.
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Streamer bridging the gap leads to breakdown.
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Paschen's Law
- Statement: Breakdown voltage ($$\displaystyle V_b $$) in a gas is a unique function of the product of gas pressure ($p$) and electrode gap distance ($d$).
$$ \boxed{V_b = f(pd)} $$
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Derivation (Simplified): From Townsend's condition ($$\displaystyle \alpha d = \text{constant} $$) and $$\displaystyle \alpha/p = A e^{-Bp/E} $$, where $$\displaystyle E = V/d $$. Solving yields $$\displaystyle V_b $$ as a function of $pd$.
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Paschen Minimum:
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$$\displaystyle V_b $$ vs. $pd$ curve has a minimum ($$\displaystyle V_{\text{min}} $$) at an optimal $$\displaystyle (pd)_{\text{min}} $$.
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For air: $$\displaystyle V_{\text{min}} \approx 327 $$ V at $$\displaystyle (pd)_{\text{min}} \approx 0.567 $$ Torr·cm.
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Practical Implications:
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Insulation Design: For a given $V$, there is a minimum safe gap at a specific pressure. Too small a gap → breakdown; too large → Paschen minimum may be exceeded.
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SF₆ Circuit Breakers: Operate at high pressure to shift $(pd)$ to the right of Paschen minimum, achieving high dielectric strength.
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Time Lags
| Type | Definition | Factors |
|---|---|---|
| Statistical Time Lag | Time from voltage application to first free electron appearance. | Radiation level, gap geometry, surface conditions. |
| Formative Time Lag | Time from first electron to complete avalanche/streamer formation. | Overvoltage magnitude, gap length, gas type/pressure. |
| Total Time Lag | Sum of both. Inherent randomness in breakdown. |
Vacuum Breakdown
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Mechanism in Deep Vacuum (< 10⁻³ Torr):
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Field Emission: High electric field at microprotrusions on cathode emits electrons.
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Microspot Heating: Localized heating at emission sites.
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Cathode Spot Formation: Vaporization of electrode material → metallic plasma → arc.
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Key Point: Vacuum has excellent dielectric strength but fails via surface phenomena (microprotrusions), not bulk gas ionization.
Solid Dielectrics
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Intrinsic Strength: Maximum electric field a perfect, defect-free material can withstand (typically 10-100 MV/m).
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Breakdown Mechanisms:
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Electronic/Avalanche: High field accelerates electrons → impact ionization → thermal runaway (similar to gas, but in lattice).
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Thermal: Local heating from losses (dielectric, conduction) → thermal runaway.
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Electrical Treeing: Partial discharge-induced carbonized path growth.
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Partial Discharge (PD):
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Concept: Localized dielectric breakdown within a small cavity or defect in a solid dielectric or at an interface, not a complete bridge.
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Significance: Indicator of insulation degradation. Causes progressive damage (erosion, treeing).
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PD Test on Cables: Apply AC voltage above operating level. Detect PD pulses using coupling capacitors and high-frequency current transformers (HFCT).
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Fault Location: Measure time difference between PD pulses detected at both cable ends → calculate distance to defect using wave propagation velocity.
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[!TIP] Common Pitfall: Do not confuse streamer (gas, fast) with treeing (solid, slow progressive). Paschen's law applies only to gaseous uniform fields.
III. HIGH VOLTAGE GENERATION
Series Resonant Circuit (Tesla Transformer Principle)
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Circuit: HV winding (L₂, C₂) in series with low-voltage winding (L₁) and capacitor (C₁).
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Resonance Condition:
$$ \boxed{\omega L = \frac{1}{\omega C}} \quad \text{or} \quad f = \frac{1}{2\pi\sqrt{LC}} $$
At resonance, impedance is minimum, current is maximum → high voltage across L₂C₂.
- Advantage: High voltage at low current, frequency transformation (high f).
Cockcroft-Walton (CW) Voltage Multiplier
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Principle: Cascaded voltage doubler stages using diodes and capacitors.
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Operation (2-stage):
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Positive half-cycle: C₁ charges to Vₘ via D₁.
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Negative half-cycle: C₂ charges to 2Vₘ (C₁ in series with supply).
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Next cycle: C₃ charges to 2Vₘ (via D₂, C₂ in series), C₄ to 3Vₘ, etc.
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Output Voltage (No Load): $$\displaystyle V_{\text{out}} \approx 2nV_{\text{peak}} $$ (n = stages).
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Advantages: No HV transformer needed for DC, compact, simple.
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Limitations: High ripple, poor regulation under load, voltage drop ∝ $$\displaystyle n^2 $$ due to capacitor charging currents.
Tesla Coil
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Construction:
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Primary: Low turns, heavy gauge, few turns, in series with capacitor (C₁) and spark gap (SG).
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Secondary: Many turns of fine wire, forms resonant LC circuit with inter-winding capacitance (C₂).
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Coupling: Loose (magnetically coupled).
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Working:
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C₁ charges from supply.
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SG fires → oscillatory discharge in primary LC circuit.
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Resonant coupling excites secondary → high-frequency, high-voltage oscillation.
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Why current flows in nearby objects? High frequency → capacitive coupling to objects (displacement current) and skin effect confines current to surface.
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Application: HV AC source for testing, demonstration.
Impulse Voltage Generation (Marx Circuit)
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Basic Marx Generator: n identical capacitor stages (C) charged in parallel to Vₘ through resistors (Rₚ), then discharged in series via triggered spark gaps.
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Triggering Mechanism (Three-Electrode Gap):
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Construction: Main gap (G₁) between stages, triggering gap (Gₜ) with third electrode (trigger pin) connected to a triggering pulse source.
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Principle: A high-voltage pulse applied to the trigger pin creates a leader spark that bridges Gₜ, initiating breakdown of the main gap G₁.
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Why Preferred? Provides synchronized, precise, and simultaneous triggering of all stages → clean, reproducible impulse waveform.
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Control Tripping: Using triggered spark gaps (as above) or ignitrons (gas-filled tubes) to initiate the discharge sequence at a precise instant.
[!TIP] Exam Focus: Be able to sketch the CW circuit, Tesla coil, and Marx generator with triggering. Know why Tesla coil current flows in nearby objects (high f → capacitive coupling).
IV. HIGH VOLTAGE MEASUREMENT
Potential Dividers for Impulse Voltages
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Conditions:
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Time Constant Matching: $$\displaystyle \tau_R = RC $$ (resistance-capacitance product) of divider must match that of the cable + oscilloscope input ($$\displaystyle \tau_C $$).
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Low Capacitance: To avoid loading the test circuit.
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Low Inductance: For fast impulse fronts.
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Resistance Value: High enough to minimize power draw, low enough to avoid excessive noise.
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| Type | Principle | Advantages | Disadvantages | Application |
|---|---|---|---|---|
| Resistance Divider | Pure resistive voltage division. | Simple, robust. | Power loss, frequency limitation (inductance distorts fast impulses). | Power frequency, slow impulses. |
| Capacitance Divider | Pure capacitive division (C₁ >> C₂). | Low loss, good for fast impulses (low inductance). | Sensitive to stray capacitance (Cₛ), requires guarding. | Standard for lightning impulse measurement. |
| Mixed RC (R-C) Divider | Series RC in each arm (R₁C₁, R₂C₂). | Compensates both R and C effects, excellent impulse response. | More complex, needs careful design. | Preferred for all impulse measurements (LI, SI). |
Sphere Gap
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Standard Sphere Gap: Two identical metal spheres of diameter D, separated by gap g.
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Principle: Breakdown voltage ($$\displaystyle V_b $$) is a function of D and g, independent of wave shape (for sufficiently long wavefronts).
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Measurement: Adjust g until breakdown occurs at the voltage peak. Read $$\displaystyle V_b $$ from standard tables (IEC 60052) corrected for atmospheric conditions.
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Factors Influencing Measurement:
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Sphere Diameter (D): Determines maximum measurable voltage.
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Gap Spacing (g): Must be within specified limits (0.1D < g < 0.5D).
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Atmospheric Conditions: Pressure (p), Temperature (T), Humidity (h). Apply correction factor:
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$$ K = \frac{p}{p_0} \cdot \frac{T_0}{T} \cdot \frac{1}{1 + 0.00012 \cdot (h - h_0)} $$
where subscript 0 = standard conditions (20°C, 760 Torr, 11 g/m³).
4. **Polarity:** Positive polarity gives lower $$\displaystyle V_b $$ than negative for same gap.
5. **Wavefront Time:** For very fast fronts (< 1 µs), $$\displaystyle V_b $$ is higher than for 50 µs wave.
Electrostatic Voltmeter
- Principle: Force of attraction between fixed and moving plates in a high-voltage electric field.
$$ F \propto V^2 \quad \Rightarrow \quad \text{Deflection} \propto V^2 $$
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Construction: Fixed electrode (connected to HV), movable vane/plate (spring-loaded), pointer, scale.
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Operation: For DC, direct reading. For AC, requires a rectifier (e.g., half-wave) to produce unidirectional force; scale calibrated for RMS.
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Advantages: No loading (high impedance), good accuracy, independent of frequency.
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Disadvantages: Bulky, limited range, sensitive to vibrations.
Generating Voltmeter
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Principle: Rotating vane or disk in the electric field between HV electrode and grounded case. The electric field induces charges on the rotating parts → AC current generated, proportional to V.
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Construction: Motor-driven rotor (vanes or segmented disk) inside an insulated, grounded housing connected to HV.
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Working: Rotor speed constant → generated current $$\displaystyle I_g \propto V $$. Measure $$\displaystyle I_g $$ with a sensitive microammeter.
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Application: High DC voltage measurement (kV to MV), where resistive dividers would have excessive power loss.
[!TIP] Common Pitfall: Sphere gap measures peak value of AC/impulse. For AC, if RMS is needed, divide peak by √2. Always correct for atmospheric conditions.
V. HIGH VOLTAGE TESTING OF EQUIPMENT
Circuit Breakers
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Short-Circuit Test (Making & Breaking):
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Objective: Verify ability to interrupt (break) and make (close against) fault currents.
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Method: Connect breaker in a test circuit with a synchronous generator or capacitor bank to simulate fault current. Measure current interruption, re-ignition, recovery voltage.
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Dielectric (Insulation) Test:
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Objective: Verify insulation strength of main and auxiliary circuits.
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Method: Apply power frequency (50/60 Hz) or impulse voltage between:
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Live parts and ground.
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Between poles (for multi-pole breakers).
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Between auxiliary circuits and main circuits.
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Insulators (Power Systems)
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Flash-Over Voltage Test:
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Method: Apply increasing voltage (AC/impulse) across insulator string until surface flashover occurs.
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Objective: Determine withstand voltage and critical flashover voltage.
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Mechanical Strength Test:
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Objective: Verify ability to withstand tensile, compressive, bending, torsional loads (from conductor weight, wind, ice).
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Method: Apply specified mechanical load in a testing machine.
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Puncture Voltage Test:
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Objective: Verify internal dielectric strength of insulator material (porcelain, polymer).
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Method: Apply voltage between metal fittings (pin & cap) with surface clean and dry to prevent flashover → forces breakdown through the body.
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Necessity: Ensures insulators can withstand electrical (flashover, puncture) and mechanical stresses in service, preventing line outages.
Power Transformers
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High Voltage (HV) Test (Withstand Test):
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Purpose: Test main insulation (windings to ground, inter-winding).
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Method: Apply AC voltage (typically 1.5-2x rated voltage) or impulse voltage (simulating lightning) for specified duration (e.g., 60s AC, 1.2/50 µs impulse).
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Acceptance: No breakdown, discharge, or excessive leakage current.
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Difference from Insulation Resistance (IR) Test:
| HV Test | IR Test | | :--- | :--- | | High Voltage (kV range), short duration. | Low Voltage (DC, 2.5-5 kV), long duration (10 min). | | Tests dielectric strength under stress. | Measures bulk insulation resistance (quality, moisture, contamination). | | Destructive if failure occurs. | Non-destructive, diagnostic. | | Pass/Fail based on withstand. | Quantitative (MΩ/GΩ), trend analysis. |
High-Voltage Cables
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Partial Discharge (PD) Test:
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Procedure:
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Apply AC voltage (typically 1.5-2x rated) to cable sample (length ~100m).
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Use coupling capacitor and high-frequency current transformer (HFCT) to detect PD pulses in the ground wire.
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Measure PD magnitude (pC) and PD inception/extinction voltages.
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Objective: Detect manufacturing defects (voids, impurities, poor splicing) in insulation.
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Fault Location with PD:
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Principle: PD pulses travel along cable at propagation velocity ($v$).
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Method: Install sensors at both ends. Measure time difference ($\Delta t$) between pulse arrivals at ends.
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Distance to Fault: $$\displaystyle \boxed{L_1 = \frac{v \cdot \Delta t}{2}} $$ (for fault in middle). Requires known $v$ and synchronized measurement.
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[!TIP] Key Distinction: HV Test on transformer is a high-stress withstand test. IR Test is a low-stress diagnostic. For cables, PD test is a sensitive diagnostic for internal defects.
VI. SPECIALIZED TOPICS & COMPARISONS
Surge Current Measurement
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Methods/Instruments:
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Rogowski Coil: Air-cored toroidal coil around conductor. Output voltage $$\displaystyle V_o \propto di/dt $$. Requires integration to get current $i(t)$. Advantage: No magnetic saturation, wide bandwidth.
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Shunt Resistor: Low-value, non-inductive resistor (e.g., manganin). $$\displaystyle V = iR $$. Challenge: Must handle high $di/dt$, isolation, bandwidth.
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Magnetic Field Probes (B-dot probes): Measure $dB/dt$ near conductor → derive $di/dt$.
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Challenges:
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Very High Magnitude: kA to MA range.
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Extremely Fast Rise Time: ns to µs (lightning, switching).
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Isolation: Instrument must be isolated from HV ground.
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Bandwidth: Oscilloscope and sensor must have sufficient bandwidth ($$\displaystyle BW > 0.35 / t_r $$).
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Cavity Breakdown
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Definition: Breakdown occurring within an enclosed cavity inside a solid dielectric or between metal parts (e.g., in a transformer bushing, GIS).
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Mechanism: Similar to gaseous breakdown but geometry confined. Paschen's law applies to the cavity dimensions and internal pressure (may be air, SF₆, or vacuum).
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Significance: Internal cavities are weak points. PD activity in cavities is a major degradation mechanism in composite insulation systems.
Motor Coil Insulation
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Pouring/Varnishing Methods:
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Dip: Coil immersed in varnish, drained.
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Trickle: Varnish slowly dripped onto rotating coil.
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Vacuum Pressure Impregnation (VPI): Coil placed in pressure vessel, vacuumed to remove air/moisture, then varnish forced in under pressure. Best method → voids eliminated, excellent adhesion, high dielectric strength.
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Comparative Summaries
| Feature | Resistance Divider | Capacitance Divider | RC Divider |
|---|---|---|---|
| Primary Element | R | C | RC Series |
| Power Loss | High | Negligible | Moderate |
| Impulse Response | Poor (L distortion) | Excellent (low L) | Best (matched τ) |
| Sensitivity to Stray C | Low | Very High | Moderate |
| Best For | PF, slow impulses | Fast impulses (with guard) | All impulse work |
| HV Measurement Method | Principle | Best For | Limitation |
| :--- | :--- | :--- | :--- |
| Sphere Gap | Air breakdown voltage | Reference standard, peak AC/impulse | Bulky, slow, atmospheric correction |
| Potential Divider | Voltage division | Continuous monitoring, recording | Requires calibration, loading |
| Electrostatic Voltmeter | Electrostatic force | DC & low-f AC, high accuracy | Low frequency, bulky |
| Generating Voltmeter | Rotating vane in E-field | High DC (> 100 kV) | AC not suitable, rotating parts |
[!TIP] Final Exam Checklist: You must be able to:
- Derive/Explain Townsend, Streamer, Paschen's Law.
- Sketch & Explain CW, Tesla Coil, Marx (with 3-electrode trigger).
- Compare all three potential divider types.
- List factors for sphere gap measurement.
- Differentiate HV test vs. IR test; PD test procedure for cables.
- Explain vacuum breakdown mechanism and cavity breakdown.
- State surge current measurement challenges.