电气入口谐波的来源

6-脉冲VFD谐波: <span class ="tr_" id="tr_12" data-source="" data-srclang="en" data-orig="Theoretical vs Practical Spectra">Theoretical vs Practical Spectra</span>

介绍

变频驱动器 (变频驱动器) 基于 6 脉冲整流器拓扑的电源转换器件是工业应用中部署最广泛的电源转换器件之一. 它们固有的非线性输入特性使其成为配电系统谐波失真的重要来源. 虽然 6 脉冲整流器的理论谐波频谱已得到很好的建立,并且通常由 \(1/n\) 幅度模型 [1], 实际测量始终揭示与这种理想行为的有意义的偏差——这种偏差会给系统设计带来真正的后果, 过滤器尺寸, 并符合 IEEE 等谐波标准 519 [2] 和IEC 61000-3-6 [3].

本文对 6 脉冲 VFD 的理论和实际谐波频谱进行了比较分析, 检查谐波次数 3 通过 50 跨越四种负载条件 (25%, 50%, 75% 和 100% 额定负载). 谐波幅度, 相位角, 和顺序进行了讨论, 并根据现实系统行为检查了理想电流注入模型的局限性.

01 理论背景

6 脉冲整流器由三相全波二极管或晶闸管桥组成,每个基本周期产生六个电流脉冲. 理想条件下——完美平衡的三相电源, 产生完美平滑直流电流的纯感性直流负载, 和理想的开关器件 - 交流线路电流波形是准方波,其傅里叶分解仅包含特定的谐波次数 [1].

特征谐波

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 等. The theoretical amplitude of each characteristic harmonic relative to the fundamental is given by:

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

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

The total harmonic distortion under the ideal model is:

总谐波失真
$$\text{总谐波失真} = \frac{\sqrt{\displaystyle\sum_{h=2}^{\infty} I_h^2}}{I_1} \times 100\%$$

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 (3路, 9日, 15日, 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:

$$f(ţ) = -f\!\左(ţ + \压裂{Ţ}{2}\右边)$$

Harmonic sequence

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

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

Negative-sequence harmonics rotate in opposition to the fundamental, producing reverse torque effects in induction motors and contributing to rotor heating. Positive-sequence harmonics rotate in the same direction as the fundamental [4][5].

02 Practical Harmonic Spectra — Deviations from the Ideal Model

在实践中, the conditions required by the ideal \(1/n\) model are never fully met. The most significant departure from idealised behaviour in a modern VFD is the replacement of the inductive DC load assumption with a large electrolytic capacitor on the DC bus. Rather than drawing a smooth continuous DC current, a capacitor-fed rectifier draws current only during the intervals when the instantaneous supply voltage exceeds the DC bus voltage, producing narrow, high-amplitude current pulses [6].

图 1 — Waveform comparison

Ideal 6-pulse rectifier — inductive DC load Quasi-square AC line current Practical 6-pulse VFD — capacitive DC bus Peaked AC line current — narrower conduction angle, higher crest factor 1 One fundamental cycle (Ţ) pk Narrow conduction angle Ideal (inductive load) Practical (capacitive bus)
图 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. 在 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. 在 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
$$I_h = \frac{k_h \cdot I_1}{Ĥ}$$

哪里 \(k_h > 1\) 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
$$\mu = \arccos\!\左(1 – \压裂{2\,\omega L_s\, I_d}{\sqrt{2}\, V_{LL}}\右边)$$

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

图 2 — Harmonic spectrum: ideal vs practical at 100% load

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

Both ZĤ(Ĥ) and Z系统(Ĥ) increase with frequency — the injected harmonic current at each order is the result of the ratio between the two impedances, not a fixed value. 见图 3.

图 2. Harmonic current spectrum at 100% load: ideal 1/n model vs practical VFD values (% of fundamental I1). The 5th and 7th harmonics exceed or approach ideal values due to the peaked waveform; higher orders roll off faster than 1/n predicts. The crossover region near h11–h13 is highlighted. Note that both the drive’s internal impedance ZĤ(Ĥ) and the supply impedance Z系统(Ĥ) vary with harmonic order, meaning neither the source nor the network presents a constant impedance across the spectrum.

表 1 — Harmonic magnitude and phase: h3 to h50 across all load conditions

The table below covers harmonic orders 3 通过 50 at four load levels, showing both magnitude (% 基本) and phase angle (°) for each. Characteristic harmonics are highlighted. Values are practical estimates based on published drive measurements — see Section 2 for methodology.

表 2 — 理想与实用 100% load: h3 至 h50

该表比较了理想的 1/Ñ 模型振幅与实际估计值的比较 100% 每个谐波次数的负载, 具有序列分类和符号差. 实际值超过理想值的谐波被标记为▲; 那些滚降速度比理想速度快的被标记为 ▼.

03 系统交互和电流源模型的限制

电力系统中的谐波分析传统上依赖于电流源注入模型, 其中每个非线性负载表示为理想电流源,在公共耦合点将固定谐波电流注入网络 (PCC). 该模型支持 IEEE 和 IEEE 的谐波评估方法 519 [2] 和IEC 61000-3-6 [3]. 然而, the current source model is a significant simplification of the actual behaviour of a 6-pulse VFD.

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

Supply network supply 系统(Ĥ) ↑ with frequency PCC Norton equivalent — 6-pulse VFD Ĥ harmonic source Ĥ(Ĥ) ↑ with frequency injected(Ĥ) = IĤ × ZĤ(Ĥ) / ( 在Ĥ(Ĥ) + 在系统(Ĥ) ) Both impedances vary with harmonic order h — Iinjected is not constant across the spectrum Impedance magnitude vs harmonic order (illustrative) 谐波次数 (Ĥ) |在| (Ž) 1 5 7 11 13 17 23 50 Resonance 高峰 系统(Ĥ) — inductive, rises linearly Ĥ(Ĥ) — internal, rises then flattens injected(Ĥ) — peaks near resonance (dashed) Parallel resonance (example near h11) Arrows show interactions absent from the ideal current source model
图 3. Norton equivalent representation of a 6-pulse VFD connected to a distribution network. The drive is modelled as a harmonic current source IĤ in parallel with an internal harmonic impedance ZĤ(Ĥ). Both ZĤ(Ĥ) and Z系统(Ĥ) increase with harmonic order — the injected current at each harmonic is therefore frequency-dependent, not constant as the ideal current source model assumes. A parallel resonance near a characteristic harmonic causes a significant spike in Iinjected.

Supply impedance dependence

A true current source is independent of the impedance of the network into which it injects. A 6-pulse drive is not. 一 3% line reactor typically reduces 5th harmonic current from approximately 18% 至 12% of fundamental at full load [6][7]. The Norton equivalent formulation captures this dependency:

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

Resonance

Parallel resonance between capacitor banks and supply inductance creates high-impedance nodes at specific harmonic frequencies. The resonant frequency is:

$$f_r = f_1 \sqrt{\压裂{S_{sc}}{Q_c}}$$

哪里 \(S_{sc}\) is the short-circuit power at the PCC and \(Q_c\) 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]. 符合IEC 61000-3-6 addresses this through a summation law:

$$U_h = \left(\sum_i U_{Ĥ,我}^{\,\alpha}\右边)^{1/\alpha}$$

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

谐波次数 Exponent α Summation type
2nd – 5th1.4Partially correlated (特征)
6日2.0Random phase (non-characteristic)
7日1.4Partially correlated (特征)
8th – 10th2.0Random phase (non-characteristic)
11日1.4Partially correlated (特征)
12日2.0Random phase (non-characteristic)
13日1.4Partially correlated (特征)
14th – 16th2.0Random phase (non-characteristic)
17th – 19th1.4Partially correlated (特征)
20th – 22nd2.0Random phase (non-characteristic)
23rd – 25th1.4Partially correlated (特征)
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:

$$I_\text{有效值} = I_1\sqrt{1 + \text{总谐波失真}^2}$$

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

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

A typical 6-pulse drive installation without mitigation may present a K-factor of 4 至 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, 11日, 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:

$$f_\text{tuned} \约 0.95 \cdot h \cdot f_1$$
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 周期 (200 ms at 50 赫兹) 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

符合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.

间谐波

Modern VFDs may generate interharmonic currents — components at non-integer multiples of the fundamental — particularly during speed ramps and transient operating conditions. 符合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].

结论

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 \(Z_h(Ĥ)\) 和 \(Z_\text{系统}(Ĥ)\) 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.

参考文献

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  2. IEEE StD里 519-2022, IEEE Standard for Harmonic Control in Electric Power Systems, IEEE, 2022.
  3. 符合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, 符合IEC, 2008.
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  7. Rockwell Automation, Harmonics and IEEE 519, Application Guide DRIVES-AP001A, 2013.
  8. 莫雷拉, J.C., Lipo, T.A., “Modeling of saturated AC machines including air-gap flux harmonic components,” 对工业电机工程学报, 飞行. 28, 不. 2, PP. 343–349, 1992.
  9. 杜根, R.C., McGranaghan, M.F., Santoso, S., Beaty, H.W., 电力系统质量, 3rd ed., 麦格劳 - 希尔, 2012.
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  11. 符合IEC 61000-4-30:2015, Electromagnetic Compatibility — Testing and Measurement Techniques — Power Quality Measurement Methods, 符合IEC, 2015.

内容由人工智能辅助起草并由作者根据以下内容进行验证 30 多年电能质量领域经验.

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