Worked problems on the supermesh technique: when a current source is shared between two meshes, the two meshes are combined into a single supermesh whose KVL equation is paired with the current-source constraint. Each problem is followed by a complete solution with the final result highlighted.
Network Analysis · Electric Circuit Analysis · 8 solved problems
Demonstrative VideoWalkthrough
Problem 1Supermesh
Find the current flowing through \(R_3\).
Solution
Applying KVL in the supermesh (meshes 1 and 3), KVL in mesh 2, and the current-source constraint between meshes 1 and 3:
Find the power of the sources, given \(V_S = 10\,\text{V},\ I_S = 4\,\text{A},\ R_1 = 2\,\Omega,\ R_2 = 6\,\Omega,\ R_3 = 1\,\Omega,\ R_4 = 2\,\Omega\).
Solution
Supermesh KVL, the second mesh KVL, and the current-source constraint:
Find the currents \(i_1\) to \(i_4\) using mesh analysis.
Solution
Meshes 1 and 2 form a supermesh through an independent current source; meshes 2 and 3 form a supermesh through a dependent current source. The two overlap into one larger supermesh. KVL around it:
A fully worked, self-contained supermesh example that shows the complete method step by step: identify the current source shared between two meshes, replace those meshes with a single supermesh, write one KVL equation around its outer boundary, and add the current-source constraint.
Problem 8Supermesh — Worked Method
A 3 A current source is shared between mesh 1 and mesh 2, so the middle branch cannot take an ordinary KVL equation. Using the supermesh method, find \(I_1\) and \(I_2\), and the power delivered by the current source.
Solution
Since a current source sits between the meshes, combine them into a supermesh and write one KVL equation around the outer boundary (skipping the source branch), with both resistor drops: