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L3 5 3 Thevenin Exampe 1

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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.
Title:
L3 5 3 Thevenin Exampe 1
Description:

Example determining Thevenin Equivalent Circuit

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Video Language:
English
Duration:
07:34

English subtitles

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