1. Lect5EEE 2021 Loop (Mesh) Analysis Dr. Holbert January 30, 2008

2. Lect5EEE 2022 Loop Analysis Nodal analysis was developed by applying KCL at each non-reference node Loop analysis is developed by applying KVL around loops in the circuit Loop (mesh) analysis results in a system of linear equations which must be solved for unknown currents

3. Lect5EEE 2023 Another Summing Circuit + – V out 1k  V1V1 V2V2 +–+– +–+– The output voltage V of this circuit is proportional to the sum of the two input voltages V 1 and V 2

4. Lect5EEE 2024 Steps of Mesh Analysis 1.Identify mesh (loops). 2.Assign a current to each mesh. 3.Apply KVL around each loop to get an equation in terms of the loop currents. 4.Solve the resulting system of linear equations for the mesh/loop currents.

5. Lect5EEE 2025 Mesh 2 1k  1. Identifying the Meshes V1V1 V2V2 Mesh 1 +–+– +–+–

6. Lect5EEE 2026 Steps of Mesh Analysis 1.Identify mesh (loops). 2.Assign a current to each mesh. 3.Apply KVL around each loop to get an equation in terms of the loop currents. 4.Solve the resulting system of linear equations for the mesh/loop currents.

7. Lect5EEE 2027 1k  2. Assigning Mesh Currents V1V1 V2V2 I1I1 I2I2 +–+– +–+–

8. Lect5EEE 2028 Steps of Mesh Analysis 1.Identify mesh (loops). 2.Assign a current to each mesh. 3.Apply KVL around each loop to get an equation in terms of the loop currents. 4.Solve the resulting system of linear equations for the mesh/loop currents.

9. Lect5EEE 2029 Voltages from Mesh Currents R I1I1 +– VRVR V R = I 1 R R I1I1 +– VRVR I2I2 V R = (I 1 – I 2 ) R

10. Lect5EEE 20210 3. KVL Around Mesh 1 –V 1 + I 1 1k  + (I 1 – I 2 ) 1k  = 0 I 1 1k  + (I 1 – I 2 ) 1k  = V 1 1k  V1V1 V2V2 I1I1 I2I2 +–+– +–+–

11. Lect5EEE 20211 3. KVL Around Mesh 2 (I 2 – I 1 ) 1k  + I 2 1k  + V 2 = 0 (I 2 – I 1 ) 1k  + I 2 1k  = –V 2 1k  V1V1 V2V2 I1I1 I2I2 +–+– +–+–

12. Lect5EEE 20212 Steps of Mesh Analysis 1.Identify mesh (loops). 2.Assign a current to each mesh. 3.Apply KVL around each loop to get an equation in terms of the loop currents. 4.Solve the resulting system of linear equations for the mesh/loop currents.

13. Lect5EEE 20213 Matrix Notation The two equations can be combined into a single matrix/vector equation

14. Lect5EEE 20214 4. Solving the Equations Let:V 1 = 7V and V 2 = 4V Results: I 1 = 3.33 mA I 2 = –0.33 mA Finally V out = (I 1 – I 2 ) 1k  = 3.66V

15. Lect5EEE 20215 Another Example 1k  2k  12V4mA 2mA I0I0 +–+–

16. Lect5EEE 20216 Mesh 2 Mesh 3 Mesh 1 1. Identify Meshes 1k  2k  12V4mA 2mA I0I0 +–+–

17. Lect5EEE 20217 2. Assign Mesh Currents I1I1 I2I2 I3I3 1k  2k  12V4mA 2mA I0I0 +–+–

18. Lect5EEE 20218 Current Sources The current sources in this circuit will have whatever voltage is necessary to make the current correct We can’t use KVL around any mesh because we don’t know the voltage for the current sources What to do?

19. Lect5EEE 20219 Current Sources The 4mA current source sets I 2 : I 2 = –4 mA The 2mA current source sets a constraint on I 1 and I 3 : I 1 – I 3 = 2 mA We have two equations and three unknowns. Where is the third equation?

20. Lect5EEE 20220 1k  2k  12V4mA 2mA I0I0 I1I1 I2I2 I3I3 The Supermesh surrounds this source! The Supermesh does not include this source! +–+–

21. Lect5EEE 20221 3. KVL Around the Supermesh -12V + I 3 2k  + (I 3 - I 2 )1k  + (I 1 - I 2 )2k  = 0 I 3 2k  + (I 3 - I 2 )1k  + (I 1 - I 2 )2k  = 12V

22. Lect5EEE 20222 Matrix Notation The three equations can be combined into a single matrix/vector equation

23. Lect5EEE 20223 4. Solve Using MATLAB >> A = [0 1 0; 1 0 -1; 2e3 -1e3-2e3 2e3+1e3]; >> v = [-4e-3; 2e-3; 12]; >> i = inv(A)*v i = 0.0012 -0.0040 -0.0008

24. Lect5EEE 20224 Solution I 1 = 1.2 mA I 2 = – 4 mA I 3 = – 0.8 mA I 0 = I 1 – I 2 = 5.2 mA

25. Lect5EEE 20225 Advantages of Nodal Analysis Solves directly for node voltages Current sources are easy Voltage sources are either very easy or somewhat difficult Works best for circuits with few nodes Works for any circuit

26. Lect5EEE 20226 Advantages of Loop Analysis Solves directly for some currents Voltage sources are easy Current sources are either very easy or somewhat difficult Works best for circuits with few loops

27. Lect5EEE 20227 Disadvantages of Loop Analysis Some currents must be computed from loop currents Does not work with non-planar circuits Choosing the supermesh may be difficult. FYI: Spice uses a nodal analysis approach

28. Lect5EEE 20228 Class Examples Drill Problems P2-12, P2-14, P2-15