I've finished designing, simulating, building, and, finally, installing, my 0.6 Farad capacitor bank to reduce the microcycling that the Outback GS8048 does to the 410 Ah AGM battery in my hybrid grid-tie and backup 6 kW solar installation. It works.
Here's the capacitor bank in its steel enclosure (with front panel off) alongside the Outback load center. There are two pairs of copper busbars that each connect three capacitors in parallel. The negative busbars are connected together inside the enclosure with a short length of flattened copper tubing, which is in turn connected to the negative busbar of the GS8048 inverter via #2 compact stranded wire. Each positive busbar connects via #4 wire to an 80A circuit breaker and then to the positive plate of the load center. The #4 wires from the capacitor enclosure to the breakers are wrapped in red and orange electrical tape for easy identification and to further protect the THHN/2 insulation, as I'd really hate for these big capacitors to get shorted out at any point.
Fig-01.jpg
The wires are longer than I'd like them to be, but the voltage drop across them is still substantially less than the total remaining ripple voltage. The #4 positive wires only get a little warm with the inverter pulling 120 A, maybe ten degrees F over ambient.
Here's a close-up of the capacitor bank with the underside of a circuit board I designed to facilitate safe and gradual charge-up and discharge of the capacitors. Pushing a button on the top activates a high-side P-channel MOSFET to charge each busbar of capacitors through its own 50 W, 75 Ohm power resistor. Tripping the 3-gang circuit breaker automatically activates a low-side N-channel MOSFET to discharge the capacitors through the same power resistors. NEC 490.6(A) calls for the residual voltage to be reduced to 50 V nominal or less within one minute after disconnection. Since the nominal voltage of the battery bank is already less than 50 V, the discharge circuit isn't strictly necessary per code, but I wanted to implement it anyway because I have a healthy respect for large charged-up capacitors. I implemented the discharge circuit to conform with one of two options under NEC 490.6(B), "automatic means of connecting it to the terminals of the capacitor bank on removal of voltage from the line." A third, low-current breaker in the 3-gang breaker device disconnects when the high-current breakers do, and that activates the N-channel MOSFET to discharge the capacitors.
Fig-02.jpg
Here's the control board mounted on its non-conductive nylon spacers with the power resistors in the background. I confirmed with my simulations that no heatsinks are required for either MOSFET.
Fig-03.jpg
Here's the connection from the ganged breakers to the positive plate with two short #4 wires. The small yellow wire is the discharge control line, which gets shorted to ground and deactivates the N-channel MOSFET when the breaker is set. When the breaker is tripped (manually or by overcurrent), the discharge control line gets pulled high and the capacitors automatically discharge through the power resistors.
Fig-04.jpg
Now, the part you were waiting for: how well it works. Here is the normal 120 Hz ripple voltage at the positive plate (directly from the battery positive) with the Outback GS8048 pulling about 120 A and the capacitors not connected:
Fig-05.jpg
Then switch on the charged-up capacitors, and presto! About 1/4 as much ripple current and 1/4 the chemical reactions causing wear and tear on my battery, replaced with infinitely repeatable electrostatic charge and discharge in the capacitors.
Fig-06.jpg
This is not a project for everyone. Big capacitors connected to high-current sources can be dangerous, and I put a lot of thought into how to do it right. The amount of time and even money (each capacitor cost about $40) involved may not pay off in extra battery life. But I'm an electrical engineer and really wanted to do this, and am very pleased with the result.
Here's the capacitor bank in its steel enclosure (with front panel off) alongside the Outback load center. There are two pairs of copper busbars that each connect three capacitors in parallel. The negative busbars are connected together inside the enclosure with a short length of flattened copper tubing, which is in turn connected to the negative busbar of the GS8048 inverter via #2 compact stranded wire. Each positive busbar connects via #4 wire to an 80A circuit breaker and then to the positive plate of the load center. The #4 wires from the capacitor enclosure to the breakers are wrapped in red and orange electrical tape for easy identification and to further protect the THHN/2 insulation, as I'd really hate for these big capacitors to get shorted out at any point.
Fig-01.jpg
The wires are longer than I'd like them to be, but the voltage drop across them is still substantially less than the total remaining ripple voltage. The #4 positive wires only get a little warm with the inverter pulling 120 A, maybe ten degrees F over ambient.
Here's a close-up of the capacitor bank with the underside of a circuit board I designed to facilitate safe and gradual charge-up and discharge of the capacitors. Pushing a button on the top activates a high-side P-channel MOSFET to charge each busbar of capacitors through its own 50 W, 75 Ohm power resistor. Tripping the 3-gang circuit breaker automatically activates a low-side N-channel MOSFET to discharge the capacitors through the same power resistors. NEC 490.6(A) calls for the residual voltage to be reduced to 50 V nominal or less within one minute after disconnection. Since the nominal voltage of the battery bank is already less than 50 V, the discharge circuit isn't strictly necessary per code, but I wanted to implement it anyway because I have a healthy respect for large charged-up capacitors. I implemented the discharge circuit to conform with one of two options under NEC 490.6(B), "automatic means of connecting it to the terminals of the capacitor bank on removal of voltage from the line." A third, low-current breaker in the 3-gang breaker device disconnects when the high-current breakers do, and that activates the N-channel MOSFET to discharge the capacitors.
Fig-02.jpg
Here's the control board mounted on its non-conductive nylon spacers with the power resistors in the background. I confirmed with my simulations that no heatsinks are required for either MOSFET.
Fig-03.jpg
Here's the connection from the ganged breakers to the positive plate with two short #4 wires. The small yellow wire is the discharge control line, which gets shorted to ground and deactivates the N-channel MOSFET when the breaker is set. When the breaker is tripped (manually or by overcurrent), the discharge control line gets pulled high and the capacitors automatically discharge through the power resistors.
Fig-04.jpg
Now, the part you were waiting for: how well it works. Here is the normal 120 Hz ripple voltage at the positive plate (directly from the battery positive) with the Outback GS8048 pulling about 120 A and the capacitors not connected:
Fig-05.jpg
Then switch on the charged-up capacitors, and presto! About 1/4 as much ripple current and 1/4 the chemical reactions causing wear and tear on my battery, replaced with infinitely repeatable electrostatic charge and discharge in the capacitors.
Fig-06.jpg
This is not a project for everyone. Big capacitors connected to high-current sources can be dangerous, and I put a lot of thought into how to do it right. The amount of time and even money (each capacitor cost about $40) involved may not pay off in extra battery life. But I'm an electrical engineer and really wanted to do this, and am very pleased with the result.
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