A Z-source inverter is a type of power inverter, a circuit that converts direct current to alternating current. The circuit functions as a buck-boost inverter without making use of DC-DC converter bridge due to its topology.
Impedance (Z) source networks efficiently convert power between source and load from DC to DC, DC to AC, and from AC to AC.[1][2]
The numbers of modifications and new Z-source topologies have grown rapidly since 2002. Improvements to the impedance networks by introducing coupled magnetics have also been lately proposed for achieving even higher voltage boosting, while using a shorter shoot-through time.[3] They include the Γ-source, T-source, trans-Z-source, TZ-source, LCCT-Z-source that utilizes a high-frequency transformer connected in series with two DC-current-blocking capacitors,[4] high-frequency transformer-isolated, and Y-source networks.[5] Amongst them, the Y-source network is more versatile and can be viewed as the generic network, from which the Γ-source, T-source, and trans-Z-source networks are derived.[3] The incommensurate properties of this network open a new horizon to researchers and engineers to explore, expand, and modify the circuit for a wide range of power conversion applications.
Types of inverters
Inverters can be classified by their structure as[6]
Single-phase inverter: This type of inverter consists of two legs or two poles. (A pole is connection of two switches where source of one and drain of other are connected and this common point is taken out).
Three-phase inverter: This type of inverter consists of three legs or poles or four legs (three legs for phases and one for neutral).
Inverters are also classified based on the type of input source as follows:
Voltage-source inverter (VSI): In this type of inverter, a constant voltage source acts as input to the inverter bridge. The constant voltage source is obtained by connecting a large capacitor across the DC source.
Current-source inverter (CSI): In this type of inverter, a constant current source acts as input to the inverter bridge. The constant current source is obtained by connecting a large inductor in series with the DC source.
Operation
Normally, three-phase inverters have 8 vector states (6 active states and 2 zero states). There is an additional state known as the shoot through state, during which the switches of one leg are short-circuited. In this state, energy is stored in the impedance network, and when the inverter is in its active state, the stored energy is transferred to the load, thus providing boost operation. This shoot through state is prohibited in VSI.[7]
Achieving the buck-boost facility in ZSI requires pulse-width modulation. The normal sinusoidal pulse width modulation (SPWM) is generated by comparing carrier triangular wave with reference sine wave. For shoot through pulses, the carrier wave is compared with two complementary DC reference levels. These pulses are added in the SPWM. ZSI has two control freedoms: modulation index of the reference wave which is the ratio of amplitude of reference wave to amplitude of carrier wave and shoot through duty ratio which can be controlled by DC level.[7]
The source can be either a voltage source or a current source. The DC source of a ZSI can be a battery, a diode rectifier or a thyristor converter, a fuel cell stack or a combination of these.
The main circuit of a ZSI can either be the traditional VSI or the traditional CSI.
Works as a buck-boost inverter.
The load of a ZSC can be inductive or capacitive, or it can be another Z-source network.
Disadvantages
Typical inverters (VSI and CSI) have few disadvantages:[10][11]
They behave in a boost or buck operation only. Thus the obtainable output voltage range is either smaller or greater than the input voltage.
They are vulnerable to electromagnetic interference and the devices get damaged in either open or short circuit conditions.
The combined system of DC-DC boost converter and the inverter has lower reliability.
The main switching devices of VSI and CSI are not interchangeable.
^Siwakoti, Yam P.; Loh, Poh Chiang; Blaabjerg, Frede; Town, Graham (2014). "Y-source impedance network". 2014 IEEE Applied Power Electronics Conference and Exposition - APEC 2014. pp. 3362–3366. doi:10.1109/APEC.2014.6803789. ISBN978-1-4799-2325-0. S2CID21361731.
^Rashid, M. (2011) Power Electronics. Pearson Education. ISBN8131762297
^ abShen, Miaosen; Peng, Fang Zheng (2008). "Operation Modes and Characteristics of the Z-Source Inverter with Small Inductance or Low Power Factor". IEEE Transactions on Industrial Electronics. 55: 89–96. doi:10.1109/TIE.2007.909063. S2CID10619253.
^Florescu, A.; Stocklosa, O.; Teodorescu, M.; Radoi, C.; Stoichescu, D. A.; Rosu, S. (2010). "The advantages, limitations and disadvantages of Z-source inverter". CAS 2010 Proceedings (International Semiconductor Conference). pp. 483–486. doi:10.1109/SMICND.2010.5650503. ISBN978-1-4244-5782-3. S2CID33649768.
^Murali, M.; Gopalakrishnan, N.; Pande, V.N. (2012). "Z-sourced unified power flow controller". 6th IET International Conference on Power Electronics, Machines and Drives (PEMD 2012). pp. A74. doi:10.1049/cp.2012.0222. ISBN978-1-84919-616-1.
^Shen, M.; Joseph, A.; Wang, J.; Peng, F.Z.; Adams, D.J. (2004). "Comparison of traditional inverters and Z-source inverter for fuel cell vehicles". Power Electronics in Transportation (IEEE Cat. No.04TH8756). pp. 125–132. doi:10.1109/PET.2004.1393815. ISBN0-7803-8538-1. S2CID5782046.