BRIDGE RECTIFIER Graetz bridge for HVDC

From Venus Kohli 7 min Reading Time

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Named after German Physicist Leo Graetz, the Graetz bridge is one of the most common rectifiers used in modern electronics. This article explains the Graetz bridge and its use in High-Voltage Direct Current or simply HVDC converters.

The Graetz bridge, a common rectifier circuit, is used in HVDC converters to convert AC to pulsating DC with improved performance through a 12-pulse configuration.(Source:  frog - stock.adobe.com)
The Graetz bridge, a common rectifier circuit, is used in HVDC converters to convert AC to pulsating DC with improved performance through a 12-pulse configuration.
(Source: frog - stock.adobe.com)

Graetz bridges are essential components in various power electronic systems, offering efficient and reliable AC-to-DC conversion. Understanding the principles and operation of Graetz bridges is crucial for designing and analyzing power circuits.

What is the Graetz bridge and how is it different from other rectifiers?

Graetz bridge is a full-wave typical four or six-diode bridge without a centre-tapped transformer. Similar to other rectifiers, this circuit converts AC into DC. Graetz Bridge does not need a centre-tap transformer because all the diodes in the conduction cycle maintain the current flow in the desirable direction.

4-pulse Graetz bridge

The 4-pulse Graetz bridge uses four diodes. During the positive half cycle, two diodes D1 and D3 remain on while the other two diodes D2 and D4 remain off. Diodes D1 and D3 conduct while diodes D2 and D4 remain in the blocking mode.

During the negative half cycle, two diodes D2 and D4 remain on while the other two diodes D1 and D3 remain off. Diodes D2 and D4 conduct while diodes D1 and D3 remain in the blocking mode.

As a result, diodes conduct current in the desired direction to generate a pulsating DC output. The complete working of bridge rectifiers is explained in our basic knowledge rectifier article.

6-pulse Graetz bridge for HVDC converters

The 6-pulse Graetz bridge uses six diodes in three-phase systems. While each diode in a 4-pulse Graetz bridge conducts for half a cycle or 180 degrees, diodes in a 6-pulse Graetz bridge conduct for less than half a cycle or 120 degrees.

Construction

The three-phase AC supply has three voltages: VA (Phase A), VB (Phase B), and VC (Phase C).

6-pulse Graetz bridge.(Source:  Venus Kohli)
6-pulse Graetz bridge.
(Source: Venus Kohli)

Cathodes of diodes D1, D3, and D5 are connected to the positive terminal of the inductive load. Anodes of diodes D1, D3, and D5 are connected to input AC supply voltages.

Similarly, anodes of diodes D2, D4, and D6 are connected to the negative terminal of the inductive load. Cathodes of diodes D2, D4, and D6 are connected to input AC supply voltages.

Phases

The input voltage is fed from transformer winding arranged in a Wye or Delta configuration. In the general use case at substations, a Delta-Wye or Wye-Delta transformer supplies three-phase voltage to the Graetz bridge. In the above diagram, each voltage phase is connected to the anode of one diode and the cathode of the other diode.

Phase A
The anode of D1 and the cathode of D2 are connected to VA.
Phase B
The anode of D3 and the cathode of D4 are connected to VB.
Phase C
The anode of D5 and the cathode of D6 are connected to VC.

Operation

A diode conducts only when the anode is more positive with respect to the cathode. All six diodes do not conduct at the same time; instead, one pair of diodes conducts while the other remains in the blocking state. As each pair is separated by pi/3 or 60 degrees, each diode conducts for 120 degrees.
Case 1
Diodes D1, D2, D3, and D4 form a bridge rectifier in the phase network of A and B. As VC = 0 V, VA reaches the maximum positive peak voltage and VB reaches the maximum negative peak voltage.
Diodes D4 and D1 become forward-biased while D3 and D2 become reverse-biased. Diodes D3 and D2 function as open circuits. Diodes D4 and D1 form a series connection with the load and start conducting. As a result, we obtain a positive output voltage.
Case 2
Diodes D1, D2, D5, and D6 form a bridge rectifier in a phase network of A and C. As VB = 0 V, VA reaches the maximum positive peak voltage and VC reaches the maximum negative peak voltage.
Diodes D1 and D6 become forward-biased while D2 and D5 become reverse-biased. Diodes D2 and D5 function as open circuits. Diodes D1 and D6 form a series connection with the load and start conducting. As a result, we obtain a positive pulse at the output.
Case 3
Diodes D3, D4, D5, and D6 form a bridge rectifier in a phase network of B and C. As VA = 0 V, VB reaches the maximum positive peak voltage and VC reaches the maximum negative peak voltage.
Diodes D6 and D3 become forward-biased while D5 and D4 become reverse-biased. Diodes D5 and D4 function as open circuits. Diodes D6 and D3 form a series connection with the load and start conducting. As a result, we obtain a positive pulse at the output.
Case 4
Diodes D1, D2, D3, and D4 form a bridge rectifier in the phase network of B and A. As VC = 0 V, VB reaches the maximum positive peak voltage and VA reaches the maximum negative peak voltage.
Diodes D3 and D2 become forward-biased while D4 and D1 become reverse-biased. Diodes D4 and D1 function as open circuits. Diodes D3 and D2 form a series connection with the load and start conducting. As a result, we obtain a positive pulse at the output.
Case 5
Diodes D1, D2, D5, and D6 form a bridge rectifier in a phase network of C and A. As VB = 0 V, VC reaches the maximum positive peak voltage and VA reaches the maximum negative peak voltage.
Diodes D2 and D5 become forward-biased while D1 and D6 become reverse-biased. Diodes D1 and D6 function as open circuits. Diodes D2 and D5 form a series connection with the load and start conducting. As a result, we obtain a positive pulse at the output.
Case 6
Diodes D3, D4, D5, and D6 form a bridge rectifier in a phase network of C and B. As VA = 0 V, VC reaches the maximum positive peak voltage and VB reaches the maximum negative peak voltage.
Diodes D5 and D4 become forward-biased while D6 and D3 become reverse-biased. Diodes D6 and D3 function as open circuits. Diodes D5 and D4 form a series connection with the load and start conducting. As a result, we obtain a positive pulse at the output.

Commutation process

Please note that each diagram may have different names and arrangements of diodes. As a result, the conducting cycle varies from diagram to diagram. However, the operation remains the same. The successive conductive cycles of diode pairs are: D4 and D1, D1 and D6, D6 and D3, D3 and D2, D2 and D5, and D5 and D4. These cycles repeat till the device remains operational.

Initially only one set of diodes conduct while others remain off. When phase voltages of the AC supply change, the same set of diodes enter a blocking mode and another set of diodes start to conduct. The process of sequential switching in which the current flow transitions from one set of diodes to another is called commutation.

The commutation process ensures the stable operation of the 6-pulse Graetz bridge. There is always a pair of conducting diodes at any point in time. The current flow is never interrupted. As a result, this device performs effective rectification by generating a stable pulsating DC voltage at the output.

Graetz bridge in HVDC

12-pulse Graetz diode bridge

Two 6-pulse Graetz bridges are connected to form a 12-pulse Graetz bridge. Simply put, 12 diodes perform conducting-blocking action in this device. Such a configuration improves HVDC converter performance and reduces ripple and harmonic components.

Graetz diode bridges are used with converters and transformers to maintain a safe voltage level at substations. In addition to AC-to-DC power conversion, another common use is to maintain a galvanic separation between the AC and DC parts of an electrical system.

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LCC (Line Commutated Converter)

Replacing diodes with Thyristors enables the construction of an LCC device. The presence of Thyristors gives rise to another terminal called the gate. Now there are three terminals: cathode, anode, and gate. The gate terminal trigger turns on the conducting mode.

Firing angle is a term that describes the initiation of the Thyristor-pair conduction cycle. In simple words, it marks the onset of conducting mode. For a smaller firing angle, a Thyristor-based 12-pulse Graetz bridge functions like a diode-based 12-pulse Graetz bridge.

A higher firing angle delays Thyristor conduction mode. Therefore, the DC output waveform can be controlled through the adjustment of the firing angle for the gate terminal. The “natural” commutation causes a delay at the gate terminal and affects the power factor of the device.

VSC (Voltage Source Converter)

Instead of diodes and Thyristor, VSC uses transistor switches like IGBTs (Insulated Bipolar Junction Transistors) and GTOs (Gate Turn-off Thyristors) to overcome the lagging power factor of LCC in HVDC converters.

VSCs do not rely on AC voltage for natural commutation. Instead, VSCs use methods of PWM (Pulse Width Modulation) to implement “forced commutation”, irrespective of AC voltage strength. As a result, these devices operate in all quadrants and handle active and reactive power both with greater control over the output waveform.

References

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