طرق تحليل الدوائر الكهربائية

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Presentation transcript:

طرق تحليل الدوائر الكهربائية Methods of Analysis

Methods of Analysis – طرق التحليل Nodal analysis. التحليل العقدي Mesh analysis. تحليل شبكة

Nodal Analysis التحليل العقدي It provides a general procedure for analyzing circuits using node voltages as the circuit variables. طريقة تستخدم لتحليل الدوائر بمعرفى فولتية كل عقدة Example 1 3

Steps to determine the node voltages: طريقة التحليل Select a node as the reference node. اختيار نقطة كمرجعية يكون جهدها صفر Assign voltages v1,v2,…,vn-1 to the remaining n-1 nodes. The voltages are referenced with respect to the reference node. ترقيم باقى النقاط Apply KCL to each of the n-1 non-reference nodes. Use Ohm’s law to express the branch currents in terms of node voltages. كتابة معادلات التيار لكل نقطة ( عدد المعادلات هو n-1 ) ثم تحويلها الى شكل معادلة بدلالة الجهود Solve the resulting simultaneous equations to obtain the unknown node voltages. حل المعادلات لايجاد قيم الجهود

v1 v2 Example 2 – circuit independent current source only Apply KCl at node 1 and 2 v1 v2 3 answer v1 = -2V, v2 = -14V

Example 3 – current with dependant current source answer v1= 4.8V, v2 = 2.4V, v3 = -2.4V

Example 4 –circuit with independent voltage source How to handle the 2V voltage source?

Example 6 – circuit with two independent voltage sources

3.4 Mesh Analysis (1) Mesh analysis provides another general procedure for analyzing circuits using mesh currents as the circuit variables. Nodal analysis applies KCL to find unknown voltages in a given circuit, while mesh analysis applies KVL to find unknown currents. A mesh is a loop which does not contain any other loops within it.

3.4 Mesh Analysis (2) Steps to determine the mesh currents: Assign mesh currents i1, 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.

3.4 Mesh Analysis (3) Example 8 – circuit with independent voltage sources Note: i1 and i2 are mesh current (imaginative, not measurable directly) I1, I2 and I3 are branch current (real, measurable directly) I1 = i1; I2 = i2; I3 = i1 - i2

3.4 Mesh Analysis (4) Apply mesh analysis to find vo in the circuit *answer Vo = 20V

3.4 Mesh Analysis (5) Example 9 – circuit with dependent voltage source answer Io = 1.5A

3.5 Mesh Analysis with Current Source (1) Circuit with current source A super-mesh results when two meshes have a (dependent or independent) current source in common as shown in (a). We create a super-mesh by excluding the current source and any elements connected in series with it as shown in (b).

3.5 Mesh Analysis with Current Source (2) The properties of a super-mesh: The current source in the super-mesh is not completely ignored; it provides the constraint equation necessary to solve for the mesh currents. A super-mesh has no current of its own. A super-mesh requires the application of both KVL and KCL.

3.7 Nodal versus Mesh Analysis (1) To select the method that results in the smaller number of equations. For example: Choose nodal analysis for circuit with fewer nodes than meshes. *Choose mesh analysis for circuit with fewer meshes than nodes. *Networks that contain many series connected elements, voltage sources, or supermeshes are more suitable for mesh analysis. *Networks with parallel-connected elements, current sources, or supernodes are more suitable for nodal analysis. If node voltages are required, it may be expedient to apply nodal analysis. If branch or mesh currents are required, it may be better to use mesh analysis.

3.6 Nodal and Mesh Analysis with Inspection (2) Example 10 – By inspection, write the nodal voltage equations for the circuit

3.6 Nodal and Mesh Analysis with Inspection (3) Example 11 – By inspection, write the mesh-current equations for the circuit