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Chapter 4 Experiment Parameters and Results

4.3. Fitting Techniques

4.3.2 Accuracy over Time

This section presents three different models for VSC-HVDC transmissions, namely Injection Model, Simple Model and HVDC Light Open Model. The Injection Model and Simple Model are used for the derivation of CLF-based control strategies. The HVDC Light Open Model is used for testing control strategies and analyzing the impact of VSC-HVDC transmissions on power systems.

2.12.1 Injection Model

The Injection Model is intended for power flow and electromechanical dynamics analyses. For this reason, it is sufficient to consider the voltage and current phasors in the ac system. The Injection Model can be considered as an element, which provides adequate interaction with other elements for enhancing the dynamic performance and stability of the system as a whole.

Harmonics and dc transient components are neglected, because they normally have a second order effect on the active and reactive powers. Voltages and currents are represented by phasors in the ac network, which vary with time during transients. The Injection Model is valid for symmetrical conditions, i.e., for positive sequence voltages and currents. The model is used in the derivation and test of control strategies. Figure 2.8 shows a basic structure of a VSC HVDC link connected in parallel with an ac transmission line.

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Figure 2.8: Basic Structure of a VSC-HVDC transmission(Van & Ghandhari, 2010).

From the connection nodes Bus i and Bus j, a VSC-HVDC transmission can be seen as a synchronous machine without inertia where the production or consumption of active power is independent of the production or consumption of reactive power. This interpretation leads to modeling a VSC-HVDC transmission as two controllable voltage sources in series with a reactance, which represents the impedance of the power transformer. This modeling is shown in Figure 2.9

Figure 2.9: Modeling of a VSC-HVDC transmission(Van & Ghandhari, 2010).

In Figure 3.2 π‘ˆ 𝑐𝑖 = π‘ˆπ‘π‘–π‘’π‘— 𝛾𝑖and π‘ˆ 𝑐𝑗 = π‘ˆπ‘π‘—π‘’π‘— 𝛾𝑗. 𝑃𝑠𝑖and 𝑄𝑠𝑖can be independentlycontrolled by 𝛾𝑖and π‘ˆπ‘π‘–. Likewise,𝑃𝑠𝑖and 𝑄𝑠𝑖can be independently controlled by 𝛾𝑗and π‘ˆπ‘π‘—It is assumed that dc

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voltage control keeps the dc voltage magnitude close to the rated voltage. Therefore, the losses of the converters are assumed constant, regardless of the current through the converters. The losses are consequently represented as a constant active load. The losses of the dc cables are neglected.

The relation between Bus i and Bus j is given by the active power: 𝑃𝑠𝑖 = βˆ’π‘ƒπ‘ π‘–.

Figure 2.10: Shows the Injection Model(Van & Ghandhari, 2010).

2.12.2 Simple Model

The Simple Model is a variation of the Injection Model where the active and reactive power are controlled directly, i.e., 𝛾𝑖, π‘ˆπ‘π‘–, 𝛾𝑗and π‘ˆπ‘π‘—do not control the active nor the reactive power injected into the respective converter. The main assumption in the Simple Model is that the control of the VSC has a very fast PI-regulator driving the active and reactive power injected into the VSC, whereπ›₯𝑃𝑠𝑖, π›₯𝑄𝑠𝑖and π›₯𝑄𝑠𝑗are inputs for control strategies or voltage support.

2.12.3 HVDC Light Open Model

The objective of the model is to provide the correct interaction between ac and dc systems. It interacts with ac networks through the injected currents. The node voltages of the networks are determined by the Kirchoff's current law. It defines an equation for each node, from which the node voltages can be solved, given the injected currents as function of the node voltages.

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Figure 2.11: Single line diagram of one end of a VSC-HVDC transmission (Latorre and Ghandhari 2010).

Hence, the modeling objective is to provide equations of the HVDC Light, which give the phasor of the ac current injected to the ac network as function of the phasor of the voltage of the ac node. The model is written for transient conditions. The model for steady state conditions is obtained by neglecting all time derivatives.

Reference values for the different controls in the ABB HVDC Light Open Model Version 1.1.6, such as active power, reactive power and ac voltage references can be set by the user and, if necessary, modified during the simulation. However, the dc voltage reference cannot be controlled by the user and is set by the model to match the nominal dc voltage of the dc nodes.

Figure 3.4 shows the single line diagram of one end of a VSC-HVDC transmission. The Figure shows a PWM converter, a series reactor, π‘₯𝐿, an ac filter and a transformer.

In the figure, π‘ˆ 𝑃𝐢𝐢and 𝐼 𝑃𝐢𝐢are the injected voltage and the current into the Point of Common Coupling (PCC). The active power through the converter reactor, π‘₯𝐿, is equal to the dc power injected into the dc nodes. The losses of the PWM converter are modeled inside and are divided into no-load losses and load losses.

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The PWM converter controls the internal ac voltage bus π‘ˆ1, so that the real and imaginary part of the current 𝐼 𝑃𝐢𝐢on the primary side of the converter transformer corresponds to current orders from internal controllers. For a converter in active power control mode, an internal active power PI-regulator controls the real part of the current 𝐼 𝑃𝐢𝐢so that the active power is equal to the active power reference. For a converter in dc voltage control mode, an internal dc voltage PI-regulator controls the real part of the current 𝐼 𝑃𝐢𝐢so that the set value for the dc node voltage, e.g. 1.0 p.u., is maintained.

For a converter in either reactive power control mode or ac voltage control mode, an internal PI-regulator controls the imaginary part of the current 𝐼 𝑃𝐢𝐢so that either the reactive power or ac voltage is equal to the reference value. Figure 3.5 shows a block diagram of the control of the HVDC Light Open Model. In the figure, π›₯𝑃𝑐, π›₯𝑄𝑐and π›₯π‘ˆπ‘Žπ‘ βˆ’π‘are user inputs and they are intended for supplementary control. In this thesis the input Ξ”Uacβˆ’c is not used.

Figure 2.12: Overview control of HVDC Light Open Model (Latorre and Ghandhari 2010)

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