전기 입구에서의 고조파 발생

6-펄스 VFD 고조파: <span class ="tr_" id="tr_0" data-source="" data-srclang="en" data-orig="Theoretical vs Practical Spectra">Theoretical vs Practical Spectra</span>

소개

가변 주파수 드라이브 (VFD를) based on the 6-pulse rectifier topology are among the most widely deployed power conversion devices in industrial applications. Their inherent non-linear input characteristic makes them a significant source of harmonic distortion on electrical distribution systems. While the theoretical harmonic spectrum of a 6-pulse rectifier is well established and commonly described by the \(1/n\) amplitude model [1], practical measurements consistently reveal meaningful deviations from this ideal behaviour — deviations that carry real consequences for system design, filter sizing, and compliance with harmonic standards such as IEEE 519 [2] 및 IEC 61000-3-6 [3].

이 기사에서는 6펄스 VFD의 이론적이고 실제적인 고조파 스펙트럼을 비교 분석합니다., 고조파 차수 조사 3 ~을 통해 50 네 가지 부하 조건에 걸쳐 (25%, 50%, 75% 과 100% 정격 부하의). 고조파 크기, 위상각, 및 순서가 논의됩니다., 실제 시스템 동작을 고려하여 이상적인 전류 주입 모델의 한계를 조사합니다..

01 이론적 배경

6펄스 정류기는 기본 사이클당 6개의 전류 펄스를 생성하는 3상 전파 다이오드 또는 사이리스터 브리지로 구성됩니다.. 이상적인 조건에서 - 완벽하게 균형 잡힌 3상 공급, 완벽하게 부드러운 DC 전류를 생성하는 순수 유도성 DC 부하, 이상적인 스위칭 장치 - AC 라인 전류 파형은 푸리에 분해에 특정 고조파 차수만 포함된 준 구형파입니다. [1].

특성 고조파

These characteristic harmonics follow the relationship:

Characteristic harmonic orders
$$h = 6k \pm 1, \quad k = 1, 2, 3 \ldots$$

This yields harmonic orders 5, 7, 11, 13, 17, 19, 23, 25 등. The theoretical amplitude of each characteristic harmonic relative to the fundamental is given by:

Ideal 1/n amplitude model
$$I_h = \frac{I_1}{H}$$

어디에서 \(I_h\) is the RMS magnitude of the \(h\)-th harmonic current, \(I_1\) is the RMS magnitude of the fundamental current, 과 \(h\) is the harmonic order. This gives a 5th harmonic of 20% 기본의, a 7th of 14.3%, an 11th of 9.1%, 등 [1][4].

The total harmonic distortion under the ideal model is:

총 고조파 왜곡
$$\text{THD} = \frac{\sqrt{\displaystyle\sum_{h=2}^{\infty} I_h^2}}{I_1} \times 100\%$$

For a 6-pulse rectifier with purely inductive DC load this converges to approximately 28.6% [4].

Under this ideal model, all even harmonics and all triplen harmonics (3회, 9일, 15일, 21st…) are theoretically absent from the line currents. Triplen harmonics are zero-sequence — all three phases carry them with identical phase angles — and in a balanced three-phase system they cannot circulate in the line conductors. Even harmonics are suppressed by the half-wave symmetry of the rectifier waveform:

$$에프(티) = -f\!\왼쪽(티 + \frac{티}{2}\권리)$$

Harmonic sequence

The characteristic harmonics follow a defined sequence pattern with direct implications for rotating machinery and power system behaviour:

Sequence classification
$$\text{Sequence} = \begin{cases} \text{부정} & h = 6k – 1 \quad (5, 11, 17, 23 \ldots) \\ \text{긍정적 인} & h = 6k + 1 \quad (7, 13, 19, 25 \ldots) \end{cases}$$

Negative-sequence harmonics rotate in opposition to the fundamental, producing reverse torque effects in induction motors and contributing to rotor heating. 포지티브 시퀀스 고조파는 기본과 동일한 방향으로 회전합니다. [4][5].

02 Practical Harmonic Spectra — Deviations from the Ideal Model

실제로, 이상형이 요구하는 조건 \(1/n\) 모델이 완전히 충족되지 않음. 최신 VFD의 이상적인 동작에서 가장 크게 벗어나는 것은 유도성 DC 부하 가정을 DC 버스의 대형 전해 커패시터로 대체한 것입니다.. 원활하게 연속적인 DC 전류를 끌어오는 것보다, 커패시터 공급 정류기는 순간 공급 전압이 DC 버스 전압을 초과하는 간격 동안에만 전류를 끌어옵니다., 좁은 생산, 고진폭 전류 펄스 [6].

그림 1 — 파형 비교

이상적인 6펄스 정류기 - 유도성 DC 부하 준사각형 AC 라인 전류 실용적인 6펄스 VFD - 용량성 DC 버스 Peaked AC line current — narrower conduction angle, higher crest factor 나는1 One fundamental cycle (티) 나는pk Narrow conduction angle Ideal (inductive load) Practical (capacitive bus)
그림 1. Comparison of AC line current waveforms. The ideal rectifier (inductive DC load) produces a quasi-square wave with flat-topped pulses and a wide conduction angle. The practical VFD (capacitive DC bus) draws narrow, peaked current pulses with a significantly higher crest factor, concentrating energy at lower harmonic orders and rolling off faster at higher orders.

The Fourier decomposition of the peaked waveform reveals two systematic deviations from the \(1/n\) model. 에 lower harmonic orders (5th and 7th), practical magnitudes exceed or approach ideal values, driven by the narrow pulse shape concentrating energy in lower-frequency components. 에 higher harmonic orders (17th and above), the opposite dominates — AC-side inductance and finite pulse rise time attenuate these components more rapidly than \(1/n\) predicts. The crossover typically occurs between the 11th and 13th harmonic [4][6].

This behaviour is expressed by introducing a correction factor \(k_h\) to the ideal model:

Corrected model
$$I_h = \frac{k_h \cdot I_1}{H}$$

어디에서 \(k_h > 1\) for lower-order harmonics, \(k_h < 1\) for higher-order harmonics, and \(k_h \approx 1\) near the 11th–13th. The value of \(k_h\) varies with load level, DC bus capacitance, and AC-side impedance [7].

Phase angle of harmonic currents also shifts with load, reflecting the changing commutation overlap angle \(\mu\) governed by:

Commutation overlap angle
$$\mu = \arccos\!\왼쪽(1 – \frac{2\,\omega L_s\, I_d}{\sqrt{2}\, V_{LL}}\권리)$$

어디에서 \(\omega\) is the angular frequency, \(L_s\) is the AC-side inductance per phase, \(I_d\) is the DC load current, 과 \(V_{LL}\) is the line-to-line supply voltage [5][8].

그림 2 — Harmonic spectrum: ideal vs practical at 100% 하중

Ideal 1/n model Practical (100% 하중) Crossover region (h11–h13)

Both ZH(H) and Z체계(H) 주파수에 따라 증가 - 각 차수에 주입된 고조파 전류는 두 임피던스 간의 비율의 결과입니다., 고정된 값이 아닌. 그림 참조 3.

그림 2. 고조파 전류 스펙트럼 100% 하중: 이상적인 1/n 모델과 실제 VFD 값 (% 기본 I의1). 5차 및 7차 고조파는 피크 파형으로 인해 이상적인 값을 초과하거나 이에 접근합니다.; 높은 주문은 1/n이 예측하는 것보다 빠르게 롤오프됩니다.. h11-h13 근처의 교차 영역이 강조 표시됩니다.. 드라이브의 내부 임피던스 Z는 모두H(H) 공급 임피던스 Z체계(H) 고조파 순서에 따라 달라짐, 즉, 소스나 네트워크 모두 스펙트럼 전반에 걸쳐 일정한 임피던스를 제공하지 않습니다..

표 1 — 고조파 크기 및 위상: 모든 부하 조건에서 h3 ~ h50

아래 표는 고조파 차수를 다루고 있습니다. 3 ~을 통해 50 4가지 부하 수준에서, 두 가지 크기를 모두 표시 (% 기본의) 및 위상각 (°) 각각에 대해. 특성 고조파가 강조 표시됩니다.. 값은 게시된 드라이브 측정값을 기반으로 한 실제 추정치입니다. 섹션을 참조하세요. 2 방법론에 대한.

표 2 — 이상적 vs 실용적 100% 하중: h3 ~ h50

이 표는 이상적인 모습을 비교한 것입니다. 1/N 실제 추정값에 대한 모델 진폭 100% 각 고조파 차수에 대한 부하, 시퀀스 분류 및 부호 있는 차이 포함. 실제 값이 이상적인 값을 초과하는 고조파는 ▲로 표시됩니다.; 이상보다 빨리 굴러가는 것들은 ▼로 표시되어 있습니다..

03 시스템 상호 작용 및 현재 소스 모델의 한계

전력 시스템의 고조파 분석은 전통적으로 전류 소스 주입 모델에 의존해 왔습니다., 각 비선형 부하는 공통 결합 지점에서 네트워크에 고정 고조파 전류를 주입하는 이상적인 전류원으로 표시됩니다. (PCC). 이 모델은 IEEE와 IEEE의 조화 평가 방법론을 뒷받침합니다. 519 [2] 및 IEC 61000-3-6 [3]. 그러나, the current source model is a significant simplification of the actual behaviour of a 6-pulse VFD.

그림 3 — Norton equivalent of a 6-pulse VFD on a distribution network

Supply network supply 제트체계(H) ↑ with frequency PCC Norton equivalent — 6-pulse VFD 나는H harmonic source 제트H(H) ↑ with frequency 나는injected(H) = IH × ZH(H) / ( 제트H(H) + 제트체계(H) ) Both impedances vary with harmonic order h — Iinjected is not constant across the spectrum Impedance magnitude vs harmonic order (illustrative) 차수 (H) |제트| (제트) 1 5 7 11 13 17 23 50 Resonance 피크 제트체계(H) — inductive, rises linearly 제트H(H) — internal, rises then flattens 나는injected(H) — peaks near resonance (dashed) Parallel resonance (example near h11) Arrows show interactions absent from the ideal current source model
그림 3. Norton equivalent representation of a 6-pulse VFD connected to a distribution network. The drive is modelled as a harmonic current source IH in parallel with an internal harmonic impedance ZH(H). Both ZH(H) and Z체계(H) 고조파 차수에 따라 증가 - 따라서 각 고조파에 주입된 전류는 주파수에 따라 달라집니다., 이상적인 전류원 모델이 가정하는 것처럼 일정하지 않음. 특성 고조파 근처의 병렬 공진으로 인해 I에 상당한 스파이크가 발생합니다.injected.

공급 임피던스 의존성

실제 전류원은 그것이 주입되는 네트워크의 임피던스와 무관합니다.. 6펄스 드라이브는 그렇지 않습니다.. A 3% 라인 리액터는 일반적으로 5차 고조파 전류를 대략적으로 감소시킵니다. 18% 에 12% 최대 부하 시 기본의 [6][7]. Norton의 동등한 공식은 이러한 종속성을 포착합니다.:

$$I_\text{injected}(H) = I_h \cdot \frac{Z_h(H)}{Z_h(H) + Z_\text{체계}(H)}$$

Resonance

커패시터 뱅크와 공급 인덕턴스 간의 병렬 공진은 특정 고조파 주파수에서 고임피던스 노드를 생성합니다.. 공진 주파수는:

$$f_r = f_1 \sqrt{\frac{에스_{sc}}{Q_c}}$$

어디에서 \(에스_{sc}\) 는 PCC의 단락 전력이고 \(Q_c\) is the reactive power of the capacitor bank [9].

Multiple drive interaction

Arithmetic addition of individual drive harmonic spectra consistently overestimates actual distortion at the PCC [2][3]. IEC 61000-3-6 addresses this through a summation law:

$$U_h = \left(\sum_i U_{H,나는}^{\,\alpha}\권리)^{1/\alpha}$$

표 3 — IEC 61000-3-6 summation exponent α by harmonic order

차수 Exponent α Summation type
2nd – 5th1.4Partially correlated (특성)
6일2.0Random phase (non-characteristic)
7일1.4Partially correlated (특성)
8th – 10th2.0Random phase (non-characteristic)
11일1.4Partially correlated (특성)
12일2.0Random phase (non-characteristic)
13일1.4Partially correlated (특성)
14th – 16th2.0Random phase (non-characteristic)
17th – 19th1.4Partially correlated (특성)
20th – 22nd2.0Random phase (non-characteristic)
23rd – 25th1.4Partially correlated (특성)
26th – 50th2.0Random phase (non-characteristic)

In systems dominated by a single drive type, arithmetic summation (\(\alpha = 1\)) may be more representative than \(\alpha = 1.4\) for characteristic orders. Engineering judgement and where possible actual measurement remain essential [2][3].

04 Practical Implications and Mitigation

Transformer and cable sizing

Harmonic currents increase the RMS line current above the fundamental value:

$$I_\text{RMS} = I_1\sqrt{1 + \text{THD}^2}$$

Transformers supplying non-linear loads must be evaluated using the K-factor:

$$K = \frac{\displaystyle\sum_{h=1}^{N} I_h^2 \cdot h^2}{\displaystyle\sum_{h=1}^{N} I_h^2}$$

A typical 6-pulse drive installation without mitigation may present a K-factor of 4 에 8 depending on load level and system impedance [6][9].

Neutral conductor loading

Triplen harmonics are zero-sequence and circulate freely in the neutral conductor of four-wire systems. Installations combining VFDs with single-phase non-linear loads can produce significant neutral currents at the 3rd and 9th harmonic. The neutral conductor must be sized accordingly [9].

Motor and connected load considerations

Negative-sequence harmonics — the 5th, 11일, 17th and higher following the \(6k-1\) pattern — produce counter-rotating magnetic fields in the air gap, generating braking torque and elevated rotor temperature. Inverter-rated motors conforming to NEMA MG1 Part 31 or IEC 60034-25 incorporate design features that improve tolerance to harmonic content and are the recommended choice for all VFD applications. A detailed treatment of motor harmonic impedance, rotor loss mechanisms, and derating methodology is reserved for a subsequent article in this series.

Mitigation strategies

The tuning frequency of a passive filter is deliberately set below the target harmonic to avoid series resonance:

$$f_\text{tuned} \약 0.95 \cdot h \cdot f_1$$
Mitigation Typical THD at full load
No mitigation35 - 45%
3% AC line reactor20 - 25%
5% AC line reactor15 - 20%
DC bus choke20 - 28%
Passive 5th/7th filter8 - 12%
18-pulse drive5 - 8%
Active front end (AFE)< 5%

05 Measurement Considerations and Interpretation of Field Results

Instrument requirements

Harmonic measurement requires a power quality analyser capable of resolving individual harmonic components to at least the 50th order, implementing a synchronised DFT with a rectangular window of exactly 10 사이클 (200 ms at 50 Hz에서) as specified by IEC 61000-4-7 [10]. Rogowski coils are generally preferred for harmonic work above the 25th order due to their superior frequency response and absence of core saturation.

Measurement point selection

For compliance assessment against IEEE 519 [2] or IEC 61000-3-6 [3], measurement must be performed at the PCC as defined in those standards. Recording simultaneously at the drive input and the PCC provides direct information about the harmonic impedance of the intervening network — valuable for resonance risk assessment.

Operating condition during measurement

IEC 61000-3-6 recommends that harmonic assessment be based on the 95th percentile of measured values over a representative observation period — typically one week [3]. Where continuous monitoring is not practical, measurements should be taken at a minimum of three load points spanning the expected operating range.

상호 고조파

Modern VFDs may generate interharmonic currents — components at non-integer multiples of the fundamental — particularly during speed ramps and transient operating conditions. IEC 61000-4-7 defines the measurement methodology using sub-group analysis with a 200 ms window [10]. Their presence should be noted as they can contribute to flicker, ripple control interference, and sub-synchronous torque oscillations.

Emission studies and compliance with utility limits

Most utilities will not accept field measurements alone as the basis for a connection approval or compliance demonstration. A formal harmonic impact study, conducted in accordance with the utility’s accepted methodology and submitted prior to commissioning, is the standard requirement in the majority of jurisdictions [2][3]. The utility’s need to assess cumulative impact on all customers connected to the same network is fundamental to the IEC 61000-3-6 framework, which allocates emission limits based on the agreed power of the installation relative to the short-circuit capacity of the network [3].

Recommended three-stage approach Use theoretical values and the 1/n model for initial screening. Progress to high-fidelity simulation (PSCAD, EMTP-RV, MATLAB/Simulink) for detailed compliance studies and mitigation design. Validate with field measurement after commissioning. This avoids the systematic over-estimation of the 1/n model, reduces the risk of over-designed mitigation, and produces the documentary evidence utilities require [2][3][11].
High-fidelity simulation vs theoretical calculation Simulation tools that model DC bus capacitance, AC-side impedance, background distortion, and multi-drive interaction consistently produce harmonic spectra closer to measured field values than the 1/n model. Where a theoretical study indicates a borderline result, simulation may demonstrate compliance without mitigation — or identify the most cost-effective mitigation path without over-engineering [7][8].

결론

The ideal \(1/n\) amplitude model systematically misrepresents the harmonic spectrum of a modern capacitor-fed 6-pulse drive. Lower-order characteristic harmonics are more load-sensitive than the model predicts; higher-order harmonics roll off faster. The crossover occurs near the 11th–13th harmonic. THD varies from approximately 22% at full load to 45% or more at 25% load — a range that spans the boundary between compliant and non-compliant for many utility connection agreements.

The representation of a 6-pulse drive as an ideal harmonic current source breaks down in the presence of supply impedance variation, background voltage distortion, network resonance, and multi-drive interaction. The Norton equivalent provides a more faithful description, and the frequency dependence of both \(Z_h(H)\) 과 \(Z_\text{체계}(H)\) must be accounted for in any rigorous analysis.

For compliance studies submitted to electrical utilities, field measurement alone is unlikely to be accepted. A formal harmonic impact study is the standard requirement. High-fidelity simulation tools produce spectra significantly closer to measured field values, reducing the risk of unnecessary mitigation measures and over-designed filter solutions. The three-stage approach — theoretical screening, high-fidelity simulation, and post-commissioning measurement — provides a proportionate and technically defensible framework across the full project lifecycle.

참조

  1. Mohan, N., Undeland, T.M., Robbins, W.P., 전력 전자: 컨버터, Applications and Design, 3rd ed., 존 와일리 & 자제, 2003.
  2. IEEE 표준 519-2022, IEEE Standard for Harmonic Control in Electric Power Systems, IEEE, 2022.
  3. IEC 61000-3-6:2008, Electromagnetic Compatibility — Limits — Assessment of Emission Limits for the Connection of Distorting Installations to MV, HV and EHV Power Systems, IEC, 2008.
  4. Arrillaga, J., 왓슨, N.R., 전원 시스템 고조파, 2nd ed., 존 와일리 & 자제, 2003.
  5. Boldea, I., Nasar, S.A., The Induction Machine Handbook, CRC 보도, 2002.
  6. Skibinski, G., Kerkman, R., Schlegel, D., “EMI emissions of modern PWM AC drives,” IEEE Industry Applications Magazine, 비행. 5, 아니. 6, PP. 47–81, 1999.
  7. Rockwell Automation, Harmonics and IEEE 519, Application Guide DRIVES-AP001A, 2013.
  8. 모레이라, J.C., Lipo, T.A., “Modeling of saturated AC machines including air-gap flux harmonic components,” 산업 응용 프로그램에 IEEE 거래, 비행. 28, 아니. 2, PP. 343–349, 1992.
  9. Dugan, R.C., McGranaghan, M.F., Santoso, S., Beaty, H.W., 전력 시스템 품질, 3rd ed., McGraw 언덕, 2012.
  10. IEC 61000-4-7:2002+A1:2008, Electromagnetic Compatibility — Testing and Measurement Techniques — General Guide on Harmonics and Interharmonics Measurements and Instrumentation, IEC, 2008.
  11. IEC 61000-4-30:2015, Electromagnetic Compatibility — Testing and Measurement Techniques — Power Quality Measurement Methods, IEC, 2015.

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