Figure 4: Over a day, solar and battery energy can fulfil load requirements
SiC switch technology
In all solar power applications, from residential to utility scale, efficiency of energy conversion is a key parameter. Every watt dissipated in equipment represents a step away from the goal of carbon neutrality and a reduction in the cost-effectiveness of the installation. Conversely, even a fraction of a percentage point saved can mean lower operating costs, smaller, lighter and cooler-running equipment, longer backup run time from batteries, and quicker capital payback.
Semiconductor switches employed in PV power conversion not only represent a significant loss contributor in themselves, but can also limit the choice of other components of the system. IGBTs for example, although they can have low static losses, cannot operate at very high frequency due to their slow switching, causing excessive dynamic losses. However, low-frequency operation generally requires larger and heavier magnetic and capacitive components. An ideal choice therefore is a switch that matches the on-state losses of an IGBT at high currents, but that can switch at higher frequency with fast edge rates. This will enable low dynamic loss and smaller passive components. Silicon MOSFETs are a contender at low power from a few kW to 10 kW, but lose out to IGBTs for static losses at high power, due to the MOSFET’s finite on-resistance. This is caused by the increase of power dissipated in a MOSFET channel resistance with the square of the current, whereas an IGBT has a near constant saturation voltage, with dissipation consequently just proportional to current.
A better proposition is a MOSFET using silicon carbide (SiC) technology, now ten years on from the launch of the first 1200 V device. SiC MOSFETs are wide band-gap semiconductors that have several advantages over silicon: critical breakdown field strength, so that the active layer is thinner at a given voltage rating and can be doped at higher level. Thus, the on-resistance is much lower for a given chip size. The smaller die dimensions also yield lower device capacitances, which allow faster switching with lower loss. Electron saturation velocity of SiC is anyway around twice the silicon value, enabling higher switching speed. Additionally, thermal conductivity of SiC is about three times better than silicon, allowing lower die temperatures for a given power dissipation and consequent lower uplift in on resistance.
Implementing SiC in solar technology
SiC MOSFETs up to 1200 V rating can be used directly in the MPPT DC-DC boost stage at up to 1000 V PV array voltage in residential, small and medium-scale commercial installations, and in the downstream single-phase or three-phase DC-AC inverter. In large commercial/utility installation panels with up to 1500 VDC output, SiC MOSFETs can still be used in a DC-DC 3-level boost arrangement, keeping the MOSFET voltage stress below the 1200 V rating. Subsequent three-phase inverters can be multilevel types, where the voltage is shared across series switches, again allowing 1200 V SiC MOSFETs to be used. DC-AC inverter switching frequency is not usually pushed very high; even though SiC can switch at MHz rates efficiently, inverters only have magnetic components for filtering rather than energy storage and coupling, so magnetics do not scale down as dramatically as in AC-DC or DC-DC converters, with their large transformers and storage chokes. SiC inverters switching around 100 kHz are therefore a good choice for very low dynamic and static loss, along with reasonable size filter components.
Installations with energy storage employ bidirectional DC-DC buck-boost converters for battery charging, and discharge to the local load with the battery being wall-mounted, in an EV, or both. Useable hours of a PV installation can be extended by controlling the contributions of solar and battery energy (Figure 4). A bidirectional, AC-DC/DC-AC power factor-corrected converter similarly provides battery energy to charge from, or feed into, the utility supply. These power conversion stages require ‘third quadrant’ or reverse switch conduction. In this mode, current momentarily flows through the MOSFET body diode before the device channel conducts, and the recovery of the stored charge leads to dynamic power loss when the channel turns off. SiC MOSFET body diodes have much lower stored charge (QRR) than silicon types, therefore improving conversion efficiency significantly. SiC MOSFET output capacitance and channel on-resistance is also comparatively lower than for silicon types, leading to yet more efficiency savings.
As an additional advantage, both uni- and bidirectional battery chargers boost DC-DC converters to provide DC links, while other associated power converters and power factor correction stages can all operate at higher frequency with SiC. This has the effect of reducing associated magnetic component size, weight, loss and cost dramatically. SiC MOSFETs can therefore be used to advantage in all power conversion stages in solar applications, yielding low overall losses and smaller passive components, with consequential lower energy and system costs, and longer back-up storage run-time.