Understanding Basic Rectifiers: Question and Explanation

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The discussion centers on the behavior of a half-wave rectifier circuit with and without a reservoir capacitor. The key confusion arises from understanding why the capacitor maintains its voltage when the input voltage drops, despite being a passive component. The explanation highlights that the current through the capacitor is defined by the equation i_c = C * (dv/dt), indicating that if the voltage source decreases, the capacitor cannot discharge back into the source due to the diode's reverse bias. This results in the capacitor holding its voltage until the source voltage drops sufficiently to reverse bias the diode. The conversation emphasizes the importance of grasping the relationship between voltage and current in capacitor behavior for a clearer understanding of rectification.
Abdullah Almosalami
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This has been frustrating me to no end, and I can't really find an answer in any textbook. So, here's my issue. A basic half-wave rectifier circuit with just a reservoir capacitor looks like this:

Half-Wave Rectifier Circuit with Reservoir Capacitor.png


And the output, as expected, is this "rippled DC" voltage:

Half-Wave Rectifier With 10uF Reservoir Capacitor.png


Alright. My issue is if we take a step back and get the voltage output of the circuit without the reservoir capacitor, like so (slightly different diode but shouldn't change anything):

Half-Wave Rectifier Circuit without Reservoir Capacitor.png


The output, as you would expect, would be a half-rectified sine wave:

Output on Half-Wave Rectifier Without Reservoir Capacitor.png


So, where is the link between the latter and former case! Most textbooks and literally everybody everywhere says that once the voltage source reaches peak, the capacitor will also be at peak minus the voltage drop across the diode, and then as the voltage source drops, it will become less than the capacitor's voltage and so the diode will become reverse-biased and that part of the circuit essentially gets disconnected until the voltage source rises back up again to meet back with the capacitor's voltage, and in the meantime the capacitor discharges its charge and maintains the slightly decreasing voltage across it. My issue is, why would the capacitor hold its voltage while the voltage source drops! It is a passive component. It should just follow the voltage as seen ^ in the latter case. For example, if I had this case:

Snapchat-1848085985.jpg


You wouldn't expect the voltage across the capacitor to be that rippling DC of a half-wave rectifier. You would just expect it to follow the voltage source. It would be a contradiction violating KVL if the capacitor's voltage and the source's voltage differed! And also violate the idea that the capacitor is a passive component!

Of course, I know that the capacitor voltage will be that rippling DC, but my question is why? What analysis can show this? Where's the math or the model to show this, say to someone who wouldn't know that the output would be rippled DC?
 

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What is a diode? A diode conduct current in one direction, from Anode to Cathode. In order for the diode to conduct, the Anode has to be about 0.7V higher than the Cathode. If Anode is less than 0.7V higher or Anode is more negative, the diode turns off and no current will flow.

What is a capacitor? It's to hold charge! So when the voltage goes up D1 will conduct and charge up the cap. The voltage on the cap follows ( with a diode drop of cause). But then when the voltage of the driving source goes do, you know that the diode D1 will be reverse biased and turn off. What is the path that discharge the cap? The answer is R1 only as D1 is off.

The charge of the cap holds the voltage, after D1 turns off, the only path of discharge the cap is R1. So the voltage drops in the cap is ONLY depend on the value of R1. If R1 is high and the charge is discharged slowly, the voltage across the cap will drop slowly like you showed as saw tooth wave.

Remember, when the input drops below the voltage on the cap, D1 is off, no charge will be discharged through D1. Why should the voltage on the cap follow the input? You forgot the function of D1 all together.
 
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yungman said:
What is a capacitor? It's to hold charge! So when the voltage goes up D1 will conduct and charge up the cap. The voltage on the cap follows ( with a diode drop of cause). But then when the voltage of the driving source goes do, you know that the diode D1 will be reverse biased and turn off. What is the path that discharge the cap? The answer is R1 only as D1 is off.

Yes. This is what I mentioned in my question. When the voltage source drops from peak, at some point the voltage source minus the voltage across the capacitor will be less than the forward voltage needed to keep the diode conducting when forward biased. But this is assuming that the voltage of the capacitor stays constant, waiting for the voltage source to drop below it. I'm asking why would the capacitor do that?
 
I just got the answer after asking an EE professor. I swear this should be taught more clearly and put in textbooks. The reason is the current running through the capacitor is given by the defining equation ## i_c = C * \frac {dv} {dt} ##, and so if the capacitor was following the half-rectified wave after the peaks, we see that ## \frac {dv} {dt} ## is negative, which would mean that the current running through the capacitor was moving backwards into the source's positive terminal, but the diode would not allow this, and so ##i_c## must equal to 0, which means ## \frac {dv} {dt} ## must also equal to 0, and hence the capacitor will maintain it's voltage at constant until the voltage source drops enough so that the diode becomes reverse biased. Holy moly freaken finally. I've been going crazy with this. Seems so obvious though now that I know. Ayaaa.
 
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We have to train our brain to think in that derivative-integral relationship between voltage and current and it's unnatural at first.

Practice it - you're going to really need it for inductance !.
 
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jim hardy said:
We have to train our brain to think in that derivative-integral relationship between voltage and current and it's unnatural at first.

Practice it - you're going to really need it for inductance !.
Absolutely! The more you know :D.
 
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I am trying to understand how transferring electric from the powerplant to my house is more effective using high voltage. The suggested explanation that the current is equal to the power supply divided by the voltage, and hence higher voltage leads to lower current and as a result to a lower power loss on the conductives is very confusing me. I know that the current is determined by the voltage and the resistance, and not by a power capability - which defines a limit to the allowable...

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