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All righty,
let's work through some examples of
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finding Thevenin equivalent circuits.
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Take a look at this circuit right here.
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We want to determine
the Thevenin equivalent circuit
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between the terminals a and b.
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That means we need to find
the open circuit voltage and
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we need to determine the Thevenin
equivalent resistance.
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Now, you'll notice the open circuit
voltage is the voltage across here, but
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because it's open circuit, that means that
there's no current flowing through here.
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I equals zero, so if there's no
current flowing through that resister,
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there's no voltage drop
across that resister.
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And the voltage at the terminals,
the open circuit voltage then,
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is, in fact,
the voltage across this 30 ohm resistor.
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Again, because there's
no voltage drop here,
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the voltage that hit this point is
the same as the voltage at this point.
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And again, because there's no current
going here, the current source here,
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0.5 amps flowing is driving these
two in series at this point.
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And we have then that V open
circuit is simply equal
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to 0.5 times, 0.5 is the current,
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times the 30 ohms is equal to 15 volts.
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We now need to determine
the Thevenin equivalent resistance,
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which we're gonna do in
each of the three methods.
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Or at least consider whether each of those
three different methods will work for
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this circuit.
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Method one works when we have at least one
independent source, which we have here.
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Method one involves finding
the short circuit current.
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And then, forming the ratio, V,
open circuit divided by I, short circuit.
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So if we short this out,
short the terminals,
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the current flowing through
that short is I, short circuit.
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Now, how do we find I,
short circuit in this circuit?
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Well, by shorting that, out that brings
this, the voltage here, down to ground.
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We have 0.5 amps flowing into now
a node which consists of two resistors,
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this 30 ohm resistor and
this 5 ohm resistor.
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Some of the current's gonna through the 5
ohm resistor, that's our short circuit
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current, the rest of the current is
gonna come through this 30 ohm resistor.
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We have a current divider here.
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So using current divider,
we can calculate short circuit directly.
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I short circuit is equal to 0.5 times,
and remember from the current divider,
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the term that goes in the numerator is
the resistance in the other branch.
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So that would be 30 ohms divided
by the sum of those two,
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30 plus 5 is 35 ohms.
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And we get then the short circuit current
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is equal to 0.4286, 0.4286 amps.
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And then RTh is equal to Voc
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divided by Isc, which is 15
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divided by 0.4286.
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Which, when we get the calculator out on
that, you'll find that equals 35 ohms.
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So, method 1.
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Method 2,
let's clear this up just a little bit.
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All righty,
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now let's use method 2 to determine
the Thevenin equivalent resistance.
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In method 2, which works if you have,
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only, independent sources.
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Method two, you deactivate the sources.
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In this case,
we have an independent current source.
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We turn the independent
current source to zero.
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And, that is effectively,
open circuiting this branch,
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which means that there will be no
current flowing through this branch.
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Such that as we look
back in to the circuit,
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this is just hanging unconnected and
does not enter into this.
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Effectively, we have,
because this is open circuit here,
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this is effectively
an infinite resistance here.
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And we see coming back into this then,
the 5 ohms in series with the 35.
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So method 2,
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We get that R Thevenin is simply
the 30 + 5 ohms = 35 ohms,
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same value we got for method 1.
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Now, let's take a look at method 3.
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Method 3 works regardless of
the types of sources that we have,
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but in method 3,
we do deactivate the independent sources.
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So once again,
we have this independent current source.
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By deactivating it, we open the circuit.
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And then, method 3 says that
we apply a test voltage,
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which then forces a test
current into the AB terminals,
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and we then algebraically work to
make the ratio of V test over I test.
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So method 3 then Is form the ratio V
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test over I test to give us R Thevenin.
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All righty, with that open circuit,
this is a simple situation.
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I, going in here,
we can write a KVL loop going
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around this loop in the direction of IT.
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So KVL, we have then, minus v test
going in the direction of current flow.
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We have then a voltage drop of plus five
I sub t coming on down here plus 30.
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That's a plus sign, 30 I sub t,
the sum of those terms equals zero.
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Let's bring in V test over to
the other side of the positive V test,
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factor out the I test.
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We had I test x 5 + 30 is 35 = V test.
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Divide both sides by I test,
that gives us our R Thevenin,
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which is equal to the ratio of
V test over I test = 35 ohms.
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So we get the same results in
any one of the three methods,
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and we then, can or now can,
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Draw our Thevenin equivalent circuit,
where V Thevenin
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is equal to 15 volts, and
R Thevenin is equal to 35 ohms.
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Notice that the original
circuit had a current source.
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But the Thevenin Equivalent Circuit
replaces that source and
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all of the resistance, the effects of
the resistance within this circuit,
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are represented by a single voltage source
and the Thevenin Equivalent resistance.