Introduction to Electric Circuits

(Michael S) #1

164 Nodal and mesh analysis


Solution


There are two meshes whose currents are I~ and 12, respectively, and we note
that the mesh current I~ is equal to the current source Is. Applying KVL to
mesh 2 and taking the anticlockwise direction to be positive, we have


V s + R3I 2 + R2I 3 -0

Since 13 = 12 - 11 then


V s +R3I 2 + R2I 2-R2I 1 =0



  • R I,-
    = Rzls- Vs
    12 : (R2/s- Vs)/(R2 + R3)


Putting in the values we have


12 - [(2 • 1) - 6)]/(2 + 1) - (-4/3) A


The current through the resistor R2 is


13 - I2 - 11- I2 - Is- (-4/3) - 1 - -7//3 - -2.33 A


The negative sign indicates that the current is flowing in the opposite direction
to that shown in the circuit diagram (i.e. it flows downwards through the
resistor).

Supermeshes
We saw that in nodal voltage analysis two nodes having a voltage source
connected between them constitute a supernode. In mesh current analysis two
meshes which have a current source common to both of them form what is
known as a supermesh. As an example, consider the circuit of Fig. 7.13 which
has three meshes identified by the currents I1, 12 and 13. Meshes 2 and 3 have a
common current source Is and together they constitute a supermesh.

Figure 7.13
Free download pdf