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i'm taking a course in Switched-mode power supplies and I am a bit confused about the theoretical explanation of what is happening in increasing voltage using a bootstrapped capacitor.

You connect a capacitor with a +Vdd. This places a charge +Q on one side and -Q on the other side of the capacitor. You then apply +Vdd to the other plate and use a diode on the other to stop the current flowing. 1)

  1. You've then surely got +Q on both plates now. Or is that even right?
  2. This confuses me a little further, if the equation for a capacitor is Q = CV, is Q in this equation the amount of charge that can be placed on one plate, i.e. +Q, or the total difference +Q and -Q, i.e. equal to a difference of 2Q?
  3. I read in multiple sources that a capacitor is the same as an inductor and it's voltage cannot change instaneously, in a similar way an inductor's current cannot change instaneously. However the latter's is due to the magnetic field collapsing, And I do not see anything happening to the electric field?

I think my problem probably lies in the definition's of these quantities and what is happening to the charge on the capacitor's plates and the electric field between them but cannot figure out what.

Please see an example circuit below of where this is applied.

enter image description here

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  • \$\begingroup\$ Could you draw a schematic of the connections you are trying to make? \$\endgroup\$ – sarthak Nov 8 '17 at 20:54
  • \$\begingroup\$ I think that if you would simulate the circuit, then most of your misconceptions would be answered. It's okay to be dumb, we're all dumb. \$\endgroup\$ – Harry Svensson Nov 8 '17 at 20:57
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    \$\begingroup\$ Try read this electronics.stackexchange.com/questions/111831/… And remember that when you have a charged capacitor. The capacitor behaves like a small voltage source. \$\endgroup\$ – G36 Nov 8 '17 at 21:03
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    \$\begingroup\$ @Hart22 Seriously? It's a simulator, you can make your design in there and test it out and see how the currents and voltages are changing, things that are difficult to grasp when you're sitting with a pen and paper. \$\endgroup\$ – Harry Svensson Nov 8 '17 at 21:09
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    \$\begingroup\$ @Harry Svensson, I do get that, it's more a theoretical understanding. I get if I simulate it, i will get the result but what a simulation won't tell me is what is happening on a theory basis? apologies! \$\endgroup\$ – Hart22 Nov 8 '17 at 21:10
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At first glance, you can treat capacitor as some kind of a voltage source. The capacitor act very similarly to a voltage source. The key equation is this I = C*dV/dt

Capacitor current is proportional the rate of voltage change across it (proportional to how quickly the voltage across the capacitor is changing).

The faster the voltage change (frequency of an AC signal is high) the large the current flow through the capacitor.

enter image description here

All this means that to sustain current through a capacitor the applied voltage must change. The more rapidly voltage changes the larger the current. On the other hand, if voltage is kept constant no current will flow no matter how large the voltage. Likewise, if the current through a capacitor is found to be zero, this means that the voltage across it must be constant, not necessarily zero.

And this circuit will try to show how Bootstrap capacitor work in switching application.

enter image description here

We have a switch in "B" position. So we apply a 1.5 volts to the circuit. At the beginning of the charging phase the capacitor is empty, and so Vc1 = 0V

The voltage on capacitor cannot change suddenly form 0V to 1.5V.

We need time to voltage on capacitor to grow (t ≈ 5*R*C).

So, immediately after we connect the supply voltage a current begins to flow. The capacitor will now charge on the right hand side through R1 starting at 0V toward 1.5V. After this the capacitor will stop charging and no current flow in the circuit Vc = 1.5V.

And now we flip the switch into A position, the lower side of the capacitor is immediately brought to 1.5V, but since the voltage across a capacitor can't change instantaneously, the voltage across it will remain 1.5V which will take (boost) the upper voltage to 3V

This diagram explain everything.

enter image description here

So, immediately after we flip the switch the voltage across the LED is equal to 3V. Exactly at the same time discharge current will start to flow. So the voltage across to cap will start to drop. So the LED will blink very shortly.

A path for capacitor's charging, and another for discharging it

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  • \$\begingroup\$ Thanks for the response, believe this is the understanding I was requiring... pretty simple explanation in the end... haha but thanks! \$\endgroup\$ – Hart22 Nov 9 '17 at 20:17
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The bootstrap cap is connected to its supply and the switching node in between your high and lowside fets.

Now consider the following:

Your lowside switch is conducting and your highside switch is off. Your bootstrap cap is therefore connected to ground and its supply. Therfore the cap is charged through the bootstrap diode to whatever voltage you are supplying it with (minus diode drop).

Now the low side switch is turned off and for a short amount of time (deadtime) both switches are off to avoid crossconduction. The voltage over the cap stays the same though.

depedent on the voltage of the switching node the voltage at the positive terminal of the fet referenced to ground is most likely higher than the bootstrap supply voltage which would discharge the cap, thats why the diode is there.

Since the diode is preventing the discharging of the cap you driver now has a supply which is higher than the source of your fet and can therefore apply a positive vgs to your high side fet.

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