Stability Analysis and Active Damping Scheme for Solar Grid-Tied Inverters Under Low Switching Frequency Conditions

1. Introduction

Solar grid-tied inverters are pivotal components in renewable energy systems, enabling efficient power conversion from photovoltaic (PV) arrays to the utility grid. Among various topologies, the LCL-filtered grid-connected inverter stands out due to its superior harmonic attenuation capabilities. However, stability challenges arise under low switching frequency (LSF) conditions, especially in high-power applications where switching frequencies are constrained to reduce losses and electromagnetic interference (EMI). This paper addresses the dual-resonance instability caused by digital control delays and LCL resonance peaks in solar grid-tied inverters operating at LSF. A novel dual-state feedback active damping (AD) scheme is proposed to suppress oscillations across both mid- and high-frequency bands, ensuring robust performance under wide-ranging switching frequencies.


2. System Modeling and Stability Analysis

2.1 LCL-Filtered Solar Grid-Tied Inverter Model

The structure of an LCL-filtered solar grid-tied inverter is illustrated in Figure 1 (omitted per guidelines). The system comprises:

  • Inverter-side inductor LmLm​: Filters high-frequency switching harmonics.
  • Grid-side inductor LgLg​: Limits grid current harmonics.
  • Parallel capacitor CC: Attenuates voltage ripple.

The grid current igig​ is regulated via a proportional-resonant (PR) controller with digital control delay Td=1.5TsTd​=1.5Ts​, where TsTs​ is the switching period. The open-loop transfer function T(s)T(s) is derived as:T(s)=Gi(s)LmLgCs3+(Lm+Lg)s,Gi(s)=(Kp+∑k=0nKr,ks−jkω)e−TdsT(s)=LmLgCs3+(Lm​+Lg​)sGi​(s)​,Gi​(s)=(Kp​+k=0∑nsjkωKr,k​​)eTds

where KpKp​ and Kr,kKr,k​ are proportional and resonant gains, respectively.

2.2 Stability Challenges Under Low Switching Frequency

At LSF (fs<2fresfs​<2fres​, where fres=12πLm+LgLmLgCfres​=2π1​LmLgCLm​+Lg​​​), two instability mechanisms emerge:

  1. Mid-Frequency Oscillations: Digital control delays cause phase lag, triggering -180° phase crossings in the control bandwidth.
  2. High-Frequency Oscillations: LCL resonance peaks induce -540° phase crossings.

The combined effect creates a double-resonance instability (Table 1).

Table 1: Stability Regions Under Different Switching Frequencies

Switching Frequency (fsfs​)Instability MechanismPhase Crossings
fs>6fresfs​>6fresHigh-frequency resonance-180° at fresfres
2fres<fs<6fres2fres​<fs​<6fresStableNone
fs<2fresfs​<2fresMid- & high-frequency resonance-180° and -540°

3. Dual-State Feedback Active Damping Scheme

3.1 Adaptive Capacitor Current Feedback (ACCF)

ACCF suppresses high-frequency oscillations by reshaping the loop gain. The feedback gain KcKc​ is designed as:Kc=11+LgLm+λ(λ>0)Kc​=1+LmLg​​1​+λ(λ>0)

This introduces a second-order zero to cancel the LCL resonance pole. The stability criterion is:1KcLgC<fresKcLgC​1​<fres

3.2 Mid-Frequency Damping via Inner-Loop Feedback

To address mid-frequency instability, an inner-loop feedback path Hb(s)Hb​(s) is added:Hb(s)=Kbs−jωb+KbHb​(s)=sjωb​+KbKb​​

where ωbωb​ is the center frequency below fs/6fs​/6. This provides phase lead and gain attenuation at critical frequencies.

Table 2: Performance Comparison of Damping Methods

MethodHigh-Frequency DampingMid-Frequency DampingComplexity
Capacitor Current FeedbackExcellentPoorLow
Inner-Loop FeedbackPoorExcellentModerate
Dual-State FeedbackExcellentExcellentHigh

The combined dual-state feedback transfer function becomes:TD(s)=Gi(s)+Kce−Tds(1+KfHb(s))LgCs2[LmLgCs3+(Lm+Lg)s](1+KfHb(s))TD​(s)=[LmLgCs3+(Lm​+Lg​)s](1+KfHb​(s))Gi​(s)+KceTds(1+KfHb​(s))LgCs2​


4. Simulation and Validation

4.1 Simulation Parameters

The solar grid-tied inverter model is simulated in PLECS with parameters listed in Table 3.

Table 3: Simulation Parameters

ParameterValue
Grid Voltage (ugug​)10 kV
DC Link Voltage20 kV
LmLm​, LgLg1.2 mH, 1.3 mH
CC10 μF
KpKp​, KrKr8.0, 500

4.2 Results

  • Case 1 (fs=15 kHzfs​=15kHz): ACCF eliminates high-frequency oscillations (THD reduced from 8.2% to 1.5%).
  • Case 2 (fs=3 kHzfs​=3kHz): Dual-state feedback suppresses both mid- (500 Hz) and high-frequency (2 kHz) resonances (Figure 2).

5. Conclusion

This paper analyzes the dual-resonance instability in solar grid-tied inverters under LSF conditions and proposes a dual-state feedback AD scheme. Key contributions include:

  1. Adaptive Damping: ACCF autonomously adjusts to LCL resonance shifts.
  2. Wideband Stability: Inner-loop feedback eliminates mid-frequency oscillations.
  3. Scalability: The scheme is applicable to high-power solar inverters in urban distribution networks.

Future work will extend this method to multi-inverter systems with adaptive resonance tracking.

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