Question
Question: The current from the battery in the circuit diagram shown is:  1A
B) 2A
C) 1.5A
D) 3A
Solution
We will apply here Kirchhoff’s second law, i.e., ∑ir=∑e. It is an application of mesh analysis. After analyzing the loops one by one by, we have to solve the two equations to get the value of the current.
Formula used:
let, the current from the battery in the loop is i and resistance of the loop is r. Then the product of these two will be the electromotive force acting in that loop, i.e., ∑ir=∑e.
Complete step by step solution:
Kirchhoff formulated two laws. One is Kirchhoff’s first law or Kirchhoff’s current law (KCL). It states that in an electrical circuit (or network of wires) the algebraic sum of currents through the conductors meeting at a point is zero, i.e., ∑i=0.
Another one is Kirchhoff’s second law or Kirchhoff’s voltage law (KVL). It states that the algebraic sum of the product of the current and resistance in any closed loop of a circuit is equal to the algebraic sum of electromotive force acting in that loop, i.e., ∑ir=∑e
The given circuit is a mesh, a complicated circuit formed by a number of adjacent loops. So, it can be analyzed one by one by applying Kirchhoff’s second law.
Let, current i1 flow in the 1st mesh and current i2 flow in the 2nd mesh.
Now, applying Kirchhoff’s second law in the mesh 1, we get,
2i1+6i1−6i2+8i1+0.5i1=15
or, 16.5i1−6i2=15 …(1)
Applying Kirchhoff’s second law in the mesh 2, we get,
7i2+i2+10i2+6i2−6i1=0
or, 24i2−6i1=0
or, 4i2−i1=0 …(2)
From equation (2) we get, i1=4i2
Putting the value of i1 in the equation (1), we get,
16.5×4i2−6i2=15
or, 66i2−6i2=15
or, 60i2=15
or, i2=6015=41
Now, putting this value of i2 in equation (2), we get,
(4×41)−i1=0
or, i1=1
So, the current from the battery in the circuit is 1A.
Note: While applying this law, we have to keep in mind the sign convention. In traversing a loop, the currents flowing in the clockwise direction are taken as positive while currents flowing in the anticlockwise direction are taken as negative. Also, while traversing the loop, the electromotive force of the source, which sends current in the clockwise direction, is taken as positive and the emf of the source, which sends current in the anticlockwise direction, is negative.