Calculating capacitor charging time in a boost converter

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SUMMARY

This discussion focuses on calculating the charging time of a capacitor bank in a boost converter circuit. The key equations referenced include the continuous mode operation equation for boost converters and the relationship between inductor current and capacitor voltage. The conversation highlights the importance of considering current limits and transient behaviors when charging capacitors, particularly in scenarios where the boost converter is either starting up or already running with a load. The proposed method for implementing cycle-by-cycle current limiting using a resistor and transistor optocoupler is also discussed as a means to regulate charging current effectively.

PREREQUISITES
  • Understanding of boost converter operation and continuous mode equations
  • Knowledge of capacitor charging dynamics and current relationships
  • Familiarity with cycle-by-cycle current limiting techniques in power electronics
  • Basic circuit design principles involving inductors and capacitors
NEXT STEPS
  • Research "Boost Converter Cycle-by-Cycle Current Limiting" techniques
  • Study "Capacitor Charging Time Calculations in Power Electronics"
  • Explore "Transient Analysis in Boost Converter Circuits"
  • Learn about "Inductor Current and Capacitor Voltage Relationships in DC-DC Converters"
USEFUL FOR

Electrical engineers, power electronics designers, and students studying boost converter applications will benefit from this discussion, particularly those interested in capacitor charging dynamics and current limiting strategies in converter circuits.

bitrex
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This is close enough to a homework question so I've put it in this section, though maybe it should be posted in the EE section. I've been looking at the equations for boost converters today, and I'm interested in the problem of how long it would take a bank of capacitors to charge through an ideal boost converter, assuming there is not any load on the output. I couldn't find an equation for it - so far I've considered the problem like this: the equation for a boost converter operating in continuous mode is:

\frac{Vs}{L} * DT + \frac{Vs-Vo}{L} * (1-D)T = 0

The portion that describes the current through the inductor when the boost converter switch is open, allowing the current stored in the inductor to flow into the capacitor is:

\Delta I_{L} =\frac{Vs-Vo}{L} * (1-D)T

Since the capacitor is in series with the inductor, current will "flow" through the capacitor charging it based on:

I_{c} = C\frac{dV}{dT}

So I do this: \int \frac{dV}{dT} = \int \frac{Vs - Vo}{CL}(1-D)t =

V(t) = \frac{1}{2}\frac{Vs - Vo}{CL}(1-D)t^{2}

Vs is the source voltage and Vo is \frac{Vs}{1-D}

Does this look legit?
 
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Good post, bitrex. But I need to ask about what you mean by "charging up a bank of capacitors". Do you mean you are starting up the boost converter into a bank of capacitors as the load, or do you mean that the boost converter is already running into a light load, and you close a switch to a bank of capacitors as the full load? Either way, I think the transient equations will be different from what you've worked out above.

In the first case, the input storage cap for the boost converter will be charging up at the same time as you are trying to charge up the output load caps. In the second case, considerations about current limit and input storage capacitor size versus the output load capacitor bank come into play...
 
For the sake of argument for now I'm assuming that I'm running the boost converter from an ideal voltage source with zero output impedance, so that the input source doesn't come into play. The situation on the output is the first situation you describe, the capacitors are the total load for the boost converter. Again, assuming for the sake of argument that the inductor in the supply could handle the current and the input circuit doesn't come into play. In the site I'm looking at (http://services.eng.uts.edu.au/~venkat/pe_html/ch07s3/ch07s3p1.htm ) there are equations that describe how to calculate the output voltage in continuous mode (from the conservation of energy, the first equation in my post above) and the output ripple with a load connected, etc. but doesn't go into detail about how long it would take the capacitor bank to charge since it's assumed that this will be a design for a continuous power supply that's supplying current to a load, and the bank will be continuously "topped up." I'm more interested in the theory of how to go about calculating the charging time of a large capacitance that is then discharged through a load at once for uh, experiments. :biggrin:
 
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For charging up a capacitor bank, your boost converter will be in current limit for much of the charge-up. Do you know how to set the cycle-by-cycle current limit on a boost converter?
 
I haven't read much about boost converter design, but the way to limit the current into the capacitor bank seems straightforward enough - something like a small resistor in series with the output of the converter and a transistor optocoupler across it, and calculate the value for the voltage drop across the resistor at the current limit to be the turn on voltage of the optocoupler. When the voltage and therefore current goes above the limit the optocoupler could be used to inhibit the PWM and let the current in the inductor fall. I think if a feedback system like this were used and if the capacitor bank were in current limit for much of the charge up, then the circuit would behave kind of like a constant current source and the capacitor charging would be essentially linear?
 
Pretty close. You are correct about the small value resistor to sense the switch current, but you usually size it for a Vbe drop at the limit current, and put a transistor BE across it so that the transistor turns on at that current limit. Then use the collector current from the transistor to shut off that cycle of the boost. This is called cycle-by-cycle current limit, because it acts quickly and consistently.

So yes, for much of the charging of the output caps, it will just be the current limit giving a relatively constant charge time.
 

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