00:01
In this problem, we are asked to rework problem 3 .11 using mesh analysis.
00:07
Now in problem 3 .11, we are asked to find for the current i1 and current i2.
00:16
Now, using mesh analysis, you could get three currents here as ix, iy, iz, where mesh ix gives us an equation of negative 24 plus 10 ix plus 40 times ix minus iy equals 0 so this is just the kvl across mesh ix now we could write a super mesh that goes from the second and the third loops here now, we could label it as color red here for the super mesh.
01:23
Using the kvl at the super mesh, we get 40 times iy minus ix plus 20 oms times iy minus ix plus 20 oms times iy plus 30 times iz.
01:53
Plus 20 times iz is equal to 0.
02:01
30 oms.
02:04
Now, we can simplify these equations as, the first equation being 25 ix minus 20 iy minus 12th is equal to 0.
02:22
That is our first equation.
02:27
For the super mesh, we could simplify it as 40 i .y.
02:32
Minus 40 i x plus 20 iy plus 50 i z equals 0 or 6 iy minus 4 i x plus 5 i z equals 0 now this is our second equation since we have three unknowns i y i z and i x we need three equations to solve for them the third equation can be acquired using junction rule here at this node, let's say node zero.
03:20
So at nodes zero, junction rule gives us i1 or iy is equal i z minus five ampiers.
03:48
Since iy here is to the right and i z is to the right.
03:55
And the 5 ampers is upwards.
04:02
So this is or you can say iy plus 5 ampers is equal to iz.
04:15
Now, rewriting equation, we get iy plus 5 ampers minus iz is equal to 0.
04:25
Now this is our third equation needed to solve for the system of equations...