1 / 66

Basic Nodal and Mesh Analysis

Basic Nodal and Mesh Analysis. Al-Qaralleh. Methods of Analysis. Introduction Nodal analysis Nodal analysis with voltage source Mesh analysis Mesh analysis with current source Nodal and mesh analyses by inspection Nodal versus mesh analysis. Steps of Nodal Analysis.

lorant
Download Presentation

Basic Nodal and Mesh Analysis

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Basic Nodal and Mesh Analysis Al-Qaralleh PSUT

  2. Methods of Analysis • Introduction • Nodal analysis • Nodal analysis with voltage source • Mesh analysis • Mesh analysis with current source • Nodal and mesh analyses by inspection • Nodal versus mesh analysis PSUT

  3. Steps of Nodal Analysis 1. Choose a reference (ground) node. 2. Assign node voltages to the other nodes. 3. Apply KCL to each node other than the reference node; express currents in terms of node voltages. 4. Solve the resulting system of linear equations for the nodal voltages. EEE 202

  4. Common symbols for indicating a reference node, (a) common ground, (b) ground, (c) chassis. PSUT

  5. 1. Reference Node The reference node is called the ground node where V = 0 500W 500W + I1 V 1kW 500W I2 500W – EEE 202

  6. Steps of Nodal Analysis 1. Choose a reference (ground) node. 2. Assign node voltages to the other nodes. 3. Apply KCL to each node other than the reference node; express currents in terms of node voltages. 4. Solve the resulting system of linear equations for the nodal voltages. EEE 202

  7. 2. Node Voltages V1, V2, and V3 are unknowns for which we solve using KCL 500W 500W V1 V2 V3 1 2 3 I1 1kW 500W I2 500W EEE 202

  8. Steps of Nodal Analysis 1. Choose a reference (ground) node. 2. Assign node voltages to the other nodes. 3. Apply KCL to each node other than the reference node; express currents in terms of node voltages. 4. Solve the resulting system of linear equations for the nodal voltages. EEE 202

  9. Currents and Node Voltages 500W V1 V2 V1 500W EEE 202

  10. 3. KCL at Node 1 500W V1 V2 I1 500W EEE 202

  11. 3. KCL at Node 2 500W 500W V1 V2 V3 1kW EEE 202

  12. 3. KCL at Node 3 500W V2 V3 500W I2 EEE 202

  13. Steps of Nodal Analysis 1. Choose a reference (ground) node. 2. Assign node voltages to the other nodes. 3. Apply KCL to each node other than the reference node; express currents in terms of node voltages. 4. Solve the resulting system of linear equations for the nodal voltages. EEE 202

  14. 4. Summing Circuit Solution Solution: V = 167I1 + 167I2 500W 500W + I1 V 1kW 500W I2 500W – EEE 202

  15. Typical circuit for nodal analysis PSUT

  16. PSUT

  17. PSUT

  18. Calculus the node voltage in the circuit shown in Fig. 3.3(a) PSUT

  19. At node 1 PSUT

  20. At node 2 PSUT

  21. In matrix form: PSUT

  22. Practice PSUT

  23. Determine the voltage at the nodes in Fig. below PSUT

  24. At node 1, PSUT

  25. At node 2 PSUT

  26. At node 3 PSUT

  27. In matrix form: PSUT

  28. 3.3 Nodal Analysis with Voltage Sources • Case 1: The voltage source is connected between a nonreference node and the reference node: The nonreference node voltage is equal to the magnitude of voltage source and the number of unknown nonreference nodes is reduced by one. • Case 2: The voltage source is connected between two nonreferenced nodes: a generalized node (supernode) is formed. PSUT

  29. 3.3 Nodal Analysis with Voltage Sources A circuit with a supernode. PSUT

  30. A supernode is formed by enclosing a (dependent or independent) voltage source connected between two nonreference nodes and any elements connected in parallel with it. • The required two equations for regulating the two nonreference node voltages are obtained by the KCL of the supernode and the relationship of node voltages due to the voltage source. PSUT

  31. Example 3.3 • For the circuit shown in Fig. 3.9, find the node voltages. i2 i1 PSUT

  32. Find the node voltages in the circuit below. PSUT

  33. At suopernode 1-2, PSUT

  34. At supernode 3-4, PSUT

  35. 3.4 Mesh Analysis • Mesh analysis: another procedure for analyzing circuits, applicable to planar circuit. • A Mesh is a loop which does not contain any other loops within it PSUT

  36. (a) A Planar circuit with crossing branches, (b) The same circuit redrawn with no crossing branches. PSUT

  37. A nonplanar circuit. PSUT

  38. Steps to Determine Mesh Currents: • Assign mesh currentsi1, i2, .., in to the n meshes. • Apply KVL to each of the n meshes. Use Ohm’s law to express the voltages in terms of the mesh currents. • Solve the resulting n simultaneous equations to get the mesh currents. PSUT

  39. Fig. 3.17 A circuit with two meshes. PSUT

  40. Apply KVL to each mesh. For mesh 1, • For mesh 2, PSUT

  41. Solve for the mesh currents. • Use i for a mesh current and I for a branch current. It’s evident from Fig. 3.17 that PSUT

  42. Find the branch current I1, I2, and I3 using mesh analysis. PSUT

  43. For mesh 1, • For mesh 2, • We can find i1 and i2 by substitution method or Cramer’s rule. Then, PSUT

  44. Use mesh analysis to find the current I0 in the circuit. PSUT

  45. Apply KVL to each mesh. For mesh 1, • For mesh 2, PSUT

  46. For mesh 3, • In matrix from becomewe can calculus i1, i2 and i3 by Cramer’s rule, and find I0. PSUT

  47. 3.5 Mesh Analysis with Current Sources A circuit with a current source. PSUT

  48. Case 1 • Current source exist only in one mesh • One mesh variable is reduced • Case 2 • Current source exists between two meshes, a super-meshis obtained. PSUT

  49. a supermesh results when two meshes have a (dependent , independent) current source in common. PSUT

  50. Properties of a Supermesh • The current is not completely ignored • provides the constraint equation necessary to solve for the mesh current. • A supermesh has no current of its own. • Several current sources in adjacency form a bigger supermesh. PSUT

More Related