Understanding Voltage Dividers: A Practical Approach

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The discussion centers on understanding voltage dividers and the assumptions behind their operation. Participants express confusion about why the current through R2 is considered equal to the current through R1, emphasizing that the voltage divider principle only holds true when resistors are in series without any branches. Clarifications are made regarding the potential difference across resistors and the implications of connecting a load at Vout. It is noted that the voltage divider is a theoretical tool for evaluating voltages, rather than a method for achieving specific voltages in practical circuits. Overall, the conversation highlights the importance of circuit configuration in applying the voltage divider principle effectively.
WarPhalange
*sigh* voltage divider...?

I've been going over basic circuitry and got to the voltage divider. I don't understand the proof here:

http://en.wikipedia.org/wiki/Voltage_divider#General_case

The first line makes sense. From Vi to Ground there are two resistors in series, so you add them, and V = IR and I is the same all around the whole circuit.

Then the 2nd line I don't get. Why is it R2 and not R1? I thought current would go From Vi through R1 and then to Vo, not Ground to Vo.
 
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The potential difference across R2 (or Z2) is given by V_{out} - 0, where 0 is the ground voltage. For a resistor, V = IR so this means V_{out} - 0 = IR_2[/tex]
 


Let me see if I have this right.

Current goes from Vin through R1, which gives a voltage drop. Then since there is a branch, i.e. two things are in parallel, V across both is equal, but current probably isn't. So then you exploit the fact that at V at the branching point = Vout, and then you do this:

Defennder said:
The potential difference across R2 (or Z2) is given by V_{out} - 0, where 0 is the ground voltage. For a resistor, V = IR so this means V_{out} - 0 = IR_2[/tex]
<br /> <br /> I think I got it. Thanks a lot. :D
 


Actually there isn't any "branch" in between R1 and R2. In fact I would say that if there is a branch there, the voltage divider principle does not work. It works only if the circuit elements are connected in series, which they would not be if there was a branch in between.
 


Sorry to revive this. I'm back in "electronics" mode and still stuck on this damn problem again...

By branch I mean it branches off between R1 and R2 to Vout.

I guess my next question is how do they know Iin = Iout? Wouldn't it be Vin = I_in(R1 + R2) and Vout = Iout*R2? Why do they use the same value for I?

EDIT: Or are you assuming it's an open circuit, so that no current actually goes to the right into Vout? Then how would that work with a Load?
 


The diagram is a little misleading. Vout does not denote a wire connected in between R1 and R2. It's just a line which indicates that the potential between the two resistors is V2. The same goes for Vin.

Iin = Iout is the assumption they make in order to derive the voltage divider principle. As said above, if that assumption is not true, ie. if there is a wire branching off from in between 2 resistors, then the potential divider principle does not work.

WarPhalange said:
EDIT: Or are you assuming it's an open circuit, so that no current actually goes to the right into Vout? Then how would that work with a Load?
EDIT: Yes you're right here. I don't know what you mean by "work with a load". It depends on whether you designate R2 as the load or something else.
 


Okay okay, that much makes sense. So how do you apply a voltage divider if you're not allowed to have anything between R1 and R2? I thought that was the whole point, where you kind of siphon off some of the current.
 


The voltage divider principle is just a principle of circuits for easy evaluation of voltages across a circuit element, not a technique for getting a desired voltage out of something. To get a desired voltage across some complicated linear network, you first reduce it to it's Thevenin equivalent, then add resistors in the appropriate manner until you get the desired voltage.
 


I see... but if I had Rload at Vout >> R1 and R2, wouldn't that be approximately correct still?

So if I used a voltmeter I could still read Vout from in between R1 and R2, right?

I guess that's what confused me above all. I had thought this was something practical, not just a thought experiment type of thing.
 

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