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The problem is to write the mesh equations for the circuit that we have shown below.
This is our first example of mesh analysis, so
we’re going to go through a few points of interest and important
steps in performing mesh analysis and coming up with the mesh equations.
First thing we want to know is that mesh analysis is the same thing as loop
analysis.
The terms are used interchangeably.
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In this problem, we can identify several meshes.
We have a mesh on the left-hand side of the circuit, which is the left loop,
if you will, but also the mesh on the right-hand side, which is the right mesh,
or right loop of the circuit.
We also have mesh which is around the outside of the circuit, and
so we have three different meshes.
They're not independent of one another because
the outside mesh composes the left and the right meshes, so
we're going to write mesh equations for two different meshes.
Mesh 1 and Mesh 2 for this problem.
So, first of all, we're going to identify the meshes.
This is our Mesh 1 and this is the mesh current associated with Mesh 1,
and this is Mesh 2, the right-hand side mesh, and
we're going to assign currents for Mesh 2 to I sub 2.
So, we have two meshes, Mesh 1 and Mesh 2, and mesh currents I1 and I2.
So, the first step in writing the Mesh equation is to
use the passive sign convention to assign polarity is across the different elements.
Our voltage sources already have polarities assigned so
we don't have to do that.
But we have to identify polarities for the resistors and
the voltage drop across the resistors.
So using the passive sign convention, if we start with the left most loop and
we're looking at the current I1 It flow through R1.
And positive sign convention tells us that the positive current flows
into the positive polarity of the voltage drop across those resistors.
So this would be identified like this, as V R1.
So V R1. We also have when
we continue around that loop, past resistor one,
we have resistor three So we have a voltage drop across it, V R3.
And if we continue around that mesh, we have R2 at the bottom of that loop.
And the voltage drop, again using the passive sign convention is V R2
across the resistor at the bottom of the left hand loop.
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Okay.
So now we're going to turn to the right hand loop and
we're going to assign polarities for it.
So if we look at that, and starting at the lower left hand side of that loop, and
going around the loop.
We already have a polarity assigned for R3 so we don't need to do that.
We have our voltage drop at the top VS2 As a polarity already assigned.
And then we come around to the right-hand side of the circuit, we have resistor R4.
Using the pass of we know that the positive direction of the current
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meets the positive polarity of the voltage drop across R4 first.
So he assigned.
That voltage drop, VR4, as shown.
And then we go around that loop, continuing around the loop to R5.
Same technique, we have a voltage drop VR5 across resistor 5.
So that's what our polarities and
our voltage drop assignments Are based on the passive sign convention.
The next thing we're going to do is we're going to add up,
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as a way of solving These problems in mesh analysis.
And Kirchoff’s voltage law tells us that, the sum of the voltage
around any closed loop is equal to zero at any instant in time.
So whether we take loop one,
loop two, or if we even choose the outside loop around the outside of the circuit.
If we add up those voltage drops,
the sum of them is going to be zero at any instant of time.
So let's do that, let's start mesh one and let's add up the voltage Around that loop.
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Starting with the lower left hand corner of that mesh,
travelling upward in a clockwise direction.
The first thing we come across is voltage source VS1 and
we, in fact hit the negative polarity of that voltage source first.
So we have minus VS1 For our first voltage rock.
We continue on that circuit and we encounter resister R 1 with
voltage drop V R 1 and counting the positive polarity of it first.
We have plus V R1 and we have
continuing around that circuit the voltage drop across R3 so we have a plus VR3.
And we continue around that loop and
we encounter resistor R2 and the drop across it.
And that's V R2.
We hit the positive polarity of each one of those resistor
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Again, doing the same thing with loop two, starting at the lower left and
corner of loop two, traveling clockwise around the loop.
The first thing we encounter as we start that journey is we encounter the voltage
up across resister R three.
We get the negative polarity first, so it's minus VR3.
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Okay.
So now we have these two equations and ultimately these will allow us to
solve for The loop currents I1 and I2.
We can make some exchanges here and they're easy in some cases.
We know that Ohm's Law V = IR can be used wherever
we have a resistor we can replace The voltage,
for instance, VR1, we can replace that by
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R3 has A current I1 flowing through it, and it also has a current
I2 flowing through it, but they're flowing in opposite directions.
So if you remember, using the passive sign convention, we assign the positive
polarity across R3, the voltage drop across R3 to be at the top of R3,
based on A positive current I one flowing in to the top of R three.
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And we chose I1 as the positive current because using the passive sign convention
That was our positive current flowing into that voltage drop across R3.
And the I2 is the opposite direction, so it has the negative sign in front of it.
So now we have R1, R2, R3, R4, and R5 identified, we see that
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if we plug those into equation one and equation two, That we have two unknowns.
Our only unknowns would be I1 and I2.
So we'd have two equations which are independent of each other, and
we'd have two unknowns, I1 and I2.
We could solve for I1 and I2 if we knew values for the resistors and for
the voltage sources.
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And if we solve for I1 and I2,
then we have everything else that we would need for the circuit.
We could solve for the power, absorb the power supply.
We could solve for the voltage drops across any element in the circuit.
So, that's all we need in order to able to solve for all the values of interest for
this circuit.
Dr. Bonnie H. FerriProfessor
Dr. Joyelle HarrisDirector of the Engineering for Social Innovation Center
Dr Mary Ann Weitnauer
