Abstract
A snubber circuit for a solid state circuit breaker (SSCB), the snubber circuit comprising a series connected capacitor and transient voltage suppressor, TVS, connected across switches of the SSCB, and a bidirectional solid state circuit breaker comprising: a main SSCB circuit configured to be connected between a power supply and a load, and comprising first and second semiconductor switches connected in series, and a snubber circuit as described above having a first end connected to a first end of the first semiconductor switch and a second end connected to a second end of the second semiconductor switch.
Claims
1. A snubber circuit for a solid state circuit breaker (SSCB) the snubber circuit comprising a series connected capacitor and transient voltage suppressor, TVS, connected across switches of the SSCB.
2. A bidirectional solid state circuit breaker comprising: a main SSCB circuit configured to be connected between a power supply and a load, and comprising first and second semiconductor switches connected in series, and a snubber circuit as claimed in claim 1 having a first end connected to a first end of the first semiconductor switch and a second end connected to a second end of the second semiconductor switch.
3. A bidirectional SSCB as claimed in claim 2, for connection to a DC power supply.
4. A bidirectional SSCB as claimed in claim 2, for connection to a three-phase AC power supply, whereby the SSCB includes a first and second switch connected in series for each phase of the power supply and a single snubber circuit for all phases.
5. The bidirectional SSCB of claim 4, further comprising rectifiers to rectify each of the three phases.
6. The bidirectional SSCB of claim 2, wherein the semiconductor switches are MOSFETs.
7. The bidirectional SSCB of claim 2, wherein the switches are Si MOSFETS.
8. The bidirectional SSCB of claim 2, wherein the switches are SiC MOSFETS.
9. The bidirectional SSCB of claim 2, wherein the switches are GaN MOSFETS.
10. An assembly including a voltage supply and a load to which voltage from the voltage supply is provided, the assembly further including a bidirectional SSCB as claimed in claim 2 between the voltage supply and the load.
11. An assembly as claimed in claim 10, the load being a power distribution system.
12. The assembly of claim 11, the power distribution system including multiplexed variable speed inverters
13. The assembly of claim 10, the load being a motor.
14. A method of dissipating voltage spikes from switching off an inductive load by means of a SSCB, the method comprising providing a snubber circuit as claimed in claim 1 across the switches of the SSCB.
Description
BRIEF DESCRIPTION
[0009] Examples of a SSCB circuit according to the disclosure will now be described with reference to the drawings. It should be noted that variations are possible within the scope of the claims.
[0010] FIG. 1 shows a conventional bi-directional SSCB circuit.
[0011] FIG. 1a shows a time-line chart showing the behaviour of one of the solid state devices of the circuit of FIG. 1.
[0012] FIG. 2 shows a known snubber solution to address the inductive turn-off spike problem discussed above.
[0013] FIG. 2a shows the waveforms for the circuit of FIG. 2.
[0014] FIG. 3 shows a DC implementation of a bi-directional SSCB snubber circuit according to the disclosure.
[0015] FIG. 4 shows the time-line for a circuit such as shown in FIG. 3.
[0016] FIG. 5 shows a 3-phase implementation of a circuit according to the disclosure.
[0017] FIG. 6 shows the time-line of the 3-phase implementation.
DETAILED DESCRIPTION
[0018] Referring first to FIG. 1, this shows a conventional SSCB for a three phase application. Each phase includes a solid state switch (e.g. a MOSFET). The graph of FIG. 1a shows, in the top row, the motor current for one of the three phases. The behaviour will be the same for each phase and so, for simplicity, only one phase will be described.
[0019] At time t.sub.0, the circuit breaker switch Q1 is turned off and the inductive load current (L1_i) falls rapidly to a minimum. The second row of the time graph shows the switch voltage (Q1_vds) which rapidly increases, when the current falls, to the switch avalanche voltage. The bottom line of the time graph shows how the switch power (Q1_pwrd) increases at turn off and then rapidly falls to zero at t.sub.1. The fourth row shows the SSCB switch avalanche energy (Q1_energy) which quickly ramps up to a high level during the switch avalanche condition. The resulting high energy causes a significant increase in switch junction temperature (Q1_tj) shown in the third row, which gradually reduces once the switch power dissipation reduces to zero at t.sub.1. Thus it can be seen that when the current is interrupted abruptly by the SSCB, the inductive load creates a back emf from the stored energy. The energy is high and can drive the switch into avalanche and destruction if the switch is not sufficiently highly rated (which either limits the use of conventional switches or requires large and expensive components).
[0020] FIG. 2 shows a typical RCD snubber. Snubbers are typically used to divert energy away from the solid state device of the SSCB in the event of abrupt current interruption to prevent damage to the SSCB. The RCD snubber consists of a capacitor 10 connected in series with a parallel connected diode 12 and resistor 14 connected in parallel with the SSCB switch 20. 3-phase loads require a back-to-back snubber configuration as shown in FIG. 2 per phase, which means that six capacitors are required for the three phases. When the current is interrupted at to energy stored in the inductive load is diverted away from switch 20 and instead transferred to the capacitor 10 (via diode 12), thereby minimising switch 20 avalanche mode duration t.sub.1˜t.sub.2. The voltage across the capacitor 10 thus clamps the voltage across the switch 20 to a level at or below the switch breakdown voltage and as a result, the power dissipation in switch 20 is very low. As shown in FIG. 2a, at t.sub.2, the energy transfer from the inductive load to the snubber capacitor is complete. The energy stored by the capacitor 10 is then gradually dissipated by resistor 14, allowing capacitor 10 voltage to discharge towards zero, as indicated by (C2_v). A comparison of the second plot of the graph of FIG. 1a with that of FIG. 2a shows that the snubber either prevents the switch voltage reaching avalanche or minimises the avalanche duration. Such snubbers, however, require the capacitor to be rated to avoid avalanche of the MOSFET (or other solid state device) which means that in many applications, the capacitor needs to be large and also expensive.
[0021] The present disclosure replaces the conventional RCD snubber circuit with a modified snubber design an example of which is shown in FIG. 3. The snubber circuit comprises a series connected transient voltage suppressor (TVS) 40 and a capacitor 50 connected across the switches 60, 70. The circuit shown in FIG. 3 is for a standard single phase DC application. For an AC application, such a circuit would be provided for each phase. A back-to-back design is still required, but in the snubber of the disclosure this is formed using a single TVS and a single capacitor. By using a combination of a TVS and a capacitor some of the energy from the inductive load will be dissipated by the TVS 40 and some will be stored by capacitor 50 and more slowly dissipated by the resistor 80. This avoids all of the energy being dissipated across the switch devices 60, 70. The capacitor does not dissipate energy power—this is done by the TVS, but because the TVS does not have to dissipate all of the energy it can be designed to have a lower peak pulse power rating than if the capacitor was not present to absorb some of the energy.
[0022] Operation of the modified snubber will now be described with reference to the time graph of FIG. 4.
[0023] At t.sub.0, the switch 70 turns off and the current falls during t.sub.0˜t.sub.1 period. Similarly to the arrangement in FIG. 2, the inductive load energy begins to charge the capacitor 50 (C2_v in the fourth row of the graph). At the same time the TVS 40 begins to conduct thus clamping the switch voltage to below the avalanche voltage (Q1_vds in the second row of the graph). By time t.sub.1, all of the inductive load energy has either been transferred to the snubber capacitor 50 or has been dissipated in the TVS 40. Between times t.sub.1 and t.sub.2, the capacitor discharges some of the energy back to the inductive load via the TVS until the TVS conduction ceases i.e. when the terminal voltage is less than the rated breakdown voltage. Resistor 80 provides a discharge path for the remaining energy stored on capacitor 50 beyond t.sub.2. As mentioned above, using the capacitor and the TVS in combination to deal with the energy spike means that relatively low peak pulse power TVS devices and relatively low rated capacitors can be used. The device is therefore simpler, smaller and less expensive. In addition, the presence of the capacitor 50 mitigates the risk of damage if the TVS fails. It is also not necessary to carefully size the components to avoid switch avalanche.
[0024] FIG. 5 shows how the snubber circuit can be used in a 3-phase AC application. A single TVS/capacitor snubber circuit as discussed above can be used for all three phases 1, 2, 3 with switches 100, 200, 300 if rectifiers R1, R2, R3 are provided at the AC phase outputs. As seen in FIG. 5, the common snubber for all three phases includes a capacitor 500 and a TVS 600 connected in series across each switch 100, 200, 300 via a respective rectifier R1, R2, R3.
[0025] For 3-phase applications using a conventional RCD snubber, a separate snubber would be required for each phase, each snubber requiring two suitably rated (I.e. relatively large) capacitors, so six capacitors in total or two high power rated TVS per phase (again, six in total) would be required.
[0026] The behaviour of the snubber of FIG. 5 can be seen in FIG. 6. When the switch is turned off at to, the stored energy is diverted to the TVS—capacitor circuit thus avoiding switch avalanche.
