Diploma i boee u 2 dc circuit analysis
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This document provides an overview of direct current (DC) circuits and circuit analysis techniques. It defines key concepts like voltage sources, current sources, ideal and real sources, and dependent and independent sources. It also explains Kirchhoff's laws, nodal analysis, and mesh analysis. Kirchhoff's current law states that the algebraic sum of currents at a node is zero. Kirchhoff's voltage law states that the algebraic sum of voltages in a closed loop is zero. Nodal analysis uses Kirchhoff's current law to set up equations relating node voltages. Mesh analysis uses Kirchhoff's voltage law to set up equations relating mesh currents.
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Diploma i boee u 2 dc circuit analysis
- 1. DC circuit analysis Course: Diploma Subject: Basics of Electrical Engineering Unit: II
- 2. What is DC circuit? • Direct current (DC) circuits basically consist of a loop of conducting wire (like copper) through which an electric current flows. An electric current consists of a flow of electric charges, analogous to the flow of water (water molecules) in a river. In addition to the copper wire in a circuit there usually are components such as resistors which restrict the flow of electric charge, similar to the way rocks and debris in a river restrict the flow of the river water.
- 3. Continue.. • Common DC circuit diagram is shown in figure containing resistors and battery. Fig 1
- 4. Voltage source • A voltage source is a two terminal device which can maintain a fixed voltage. An ideal voltage source can maintain the fixed voltage independent of the load resistance or the output current. However, a real-world voltage source cannot supply unlimited current. A voltage source is the dual of a current source. Real-world sources of electrical energy, such as batteries, generators, and power systems, can be modeled for analysis purposes as a combination of an ideal voltage source and additional combinations of impedance elements.
- 5. Cont.. A schematic diagram of a real voltage source, V, driving a resistor, R, and creating a current I Fig 2
- 6. Ideal voltage source • An ideal voltage source is a two-terminal device that maintains a fixed voltage drop across its terminals. It is often used as a mathematical abstraction that simplifies the analysis of real electric circuits. If the voltage across an ideal voltage source can be specified independently of any other variable in a circuit, it is called an independent voltage source. Conversely, if the voltage across an ideal voltage source is determined by some other voltage or current in a circuit, it is called a dependent or controlled voltage source.
- 7. Cont.. • A mathematical model of an amplifier will include dependent voltage sources whose magnitude is governed by some fixed relation to an input signal, for example. In the analysis of faults on electrical power systems, the whole network of interconnected sources and transmission lines can be usefully replaced by an ideal (AC) voltage source and a single equivalent impedance
- 8. Cont.. Ideal Voltage Source Controlled Voltage Source Single cell Battery of cells Fig 3
- 9. Current sources • A current source is an electronic circuit that delivers or absorbs an electric current which is independent of the voltage across it. • A current source is the dual of a voltage source. The term constant-current 'sink' is sometimes used for sources fed from a negative voltage supply. Figure 1 shows the schematic symbol for an ideal current source, driving a resistor load. There are two types – an independent current source (or sink) delivers a constant current. A dependent current source delivers a current which is proportional to some other voltage or current in the circuit.
- 10. Cont.. Ideal Current Source Controlled Current Source Fig 3
- 11. Dependent and independent source • Dependent sources:- • In the theory of electrical networks, a dependent source is a voltage source or a current source whose value depends on a voltage or current somewhere else in the network. • Dependent sources are useful, for example, in modeling the behavior of amplifiers. A bipolar junction transistor can be modeled as a dependent current source whose magnitude depends on the magnitude of the current fed into its controlling base terminal.
- 12. Cont.. • An operational amplifier can be described as a voltage source dependent on the differential input voltage between its input terminals. Practical circuit elements have properties such as finite power capacity, voltage, current, or frequency limits that mean an ideal source is only an approximate model. Accurate modelling of practical devices requires using several idealized elements in combination.
- 13. Classification Dependent sources can be classified as follows: a)Voltage-controlled voltage source: The source delivers the voltage as per the voltage of the dependent element. b)Voltage-controlled current source: The source delivers the current as per the voltage of the dependent element. c)Current-controlled current source: The source delivers the current as per the current of the dependent element. d)Current-controlled voltage source: The source delivers the voltage as per the current of the dependent element.
- 14. Circuits Voltage-controlled voltage source Voltage controlled current source Current controlled current source Current controlled voltage source Fig 4
- 15. Independent sources • An independent voltage source maintains a voltage (fixed or varying with time) which is not affected by any other quantity. Similarly an independent current source maintains a current (fixed or time-varying) which is unaffected by any other quantity. The usual symbols are shown in figure
- 16. Symbols • Symbols for dependent sources
- 17. Star Delta connection circuit • The Y-Δ transform, also written wye-delta and also known by many other names, is a mathematical technique to simplify the analysis of an electrical network. The name derives from the shapes of the circuit diagrams, which look respectively like the letter Y and the Greek capital letter Δ. This circuit transformation theory was published by Arthur Edwin Kennelly in 1899. It is widely used in analysis of three- phase electric power circuits. • The Y-Δ transform can be considered a special case of the star-mesh transform for three resistors.
- 18. Cont.. Page No. 1.19 from Elements of Electrical Engineering ( J.N.Swamy)
- 19. Cont.. • The transformation is used to establish equivalence for networks with three terminals. Where three elements terminate at a common node and none are sources, the node is eliminated by transforming the impedances. For equivalence, the impedance between any pair of terminals must be the same for both networks. The equations given here are valid for complex as well as real impedances. • Equations for the transformation from Δ-load to Y- load 3-phase circuit • The general idea is to compute the impedance at a terminal node of the Y circuit with impedances , to adjacent node in the Δ circuit by
- 20. Cont.. • where are all impedances in the Δ circuit. This yields the specific formulae
- 21. Cont.. • Equations for the transformation from Y-load to Δ-load 3-phase circuit. • The general idea is to compute an impedance in the Δ circuit by • where is the sum of the products of all pairs of impedances in the Y circuit and is the impedance of the node in the Y circuit which is opposite the edge with . The formula for the individual edges are thus
- 22. Cont..
- 23. Kirchhoff's laws • Kirchoff’s current law:- • This law is also called Kirchhoff's first law, Kirchhoff's point rule, or Kirchhoff's junction rule (or nodal rule). • The principle of conservation of electric charge implies that: • At any node (junction) in an electrical circuit, the sum of currents flowing into that node is equal to the sum of currents flowing out of that node, or:The algebraic sum of currents in a network of conductors meeting at a point is zero.Recalling that current is a signed (positive or negative) quantity reflecting direction towards or away from a node, this principle can be stated as:
- 24. Cont.. • n is the total number of branches with currents flowing towards or away from the node. • The law is based on the conservation of charge whereby the charge (measured in coulombs) is the product of the current (in amperes) and the time (in seconds).
- 25. Cont.. The current entering any junction is equal to the current leaving that junction. i2 + i3 = i1 + i4 Page No: 1.16 from Elements of Electrical Engineering ( J.N.Swamy)
- 26. Kirchoff’s voltage law • This law is also called Kirchhoff's second law, Kirchhoff's loop (or mesh) rule, and Kirchhoff's second rule. • The principle of conservation of energy implies that • The directed sum of the electrical potential differences (voltage) around any closed network is zero, or:More simply, the sum of the emfs in any closed loop is equivalent to the sum of the potential drops in that loop, or:The algebraic sum of the products of the resistances of the conductors and the currents in them in a closed loop is equal to the total emf available in that loop.Similarly to KCL, it can be stated as:
- 27. Cont.. The sum of all the voltages around the loop is equal to zero. v1+ v2 + v3 - v4 = 0 Page No: 1.17 from Elements of Electrical Engineering ( J.N.Swamy)
- 28. Cont.. • Here, n is the total number of voltages measured. The voltages may also be complex: • This law is based on the conservation of energy whereby voltage is defined as the energy per unit charge. The total amount of energy gained per unit charge must equal the amount of energy lost per unit charge, as energy and charge are both conserved.
- 29. Nodal Analysis • Circuit Nodes and Loops:- • Node:- A node is a point where two or more circuit elements are connected. • Loop:- A loop is formed by tracing a closed path in a circuit through selected basic circuit elements without passing through any intermediate node more than once
- 30. Example: Find the Nodes + - Vs node Page No: 2.35 self making from Circuits and Networks (U.A.Patel)
- 31. Example: Find the loops loop Page No: 2.35 self making from Circuits and Networks (U.A.Patel)
- 32. Equivalent Circuits:- Source Transformation Vs + - Rs Is Rs sss IRV s s s R V I Page No: 2.61 self making from Circuits and Networks (U.A.Patel)
- 33. 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
- 34. 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.
- 35. Common symbols for indicating a reference node, (a) common ground, (b) ground, (c) chassis. self making from Circuits and Networks (U.A.Patel)
- 36. 1. Reference Node The reference node is called the ground node where V = 0 + – V 500W 500W 1kW 500W 500W I1 I2 Page No: 2.53 self making from Circuits and Networks (U.A.Patel)
- 37. 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.
- 38. 2. Node Voltages V1, V2, and V3 are unknowns for which we solve using KCL 500W 500W 1kW 500W 500W I1 I2 1 2 3 V1 V2 V3 Page No: 2.37 self making from Circuits and Networks (U.A.Patel)
- 39. 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.
- 40. 3. 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
- 41. (a) A Planar circuit with crossing branches, (b) The same circuit redrawn with no crossing branches. self making from Circuits and Networks (U.A.Patel)
- 42. • Steps to Determine Mesh Currents: 1. Assign mesh currents i1, i2, .., in to the n meshes. 2. Apply KVL to each of the n meshes. Use Ohm’s law to express the voltages in terms of the mesh currents. 3. Solve the resulting n simultaneous equations to get the mesh currents.
- 43. Figure: A circuit with two meshes. Page No: 1.53 from Circuits and Networks (U.A.Patel)
- 44. • Apply KVL to each mesh. For mesh 1, • For mesh 2, 123131 213111 )( 0)( ViRiRR iiRiRV 223213 123222 )( 0)( ViRRiR iiRViR
- 45. • 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 2 1 2 1 323 331 V V i i RRR RRR 2132211 ,, iiIiIiI
- 46. • Find the branch current I1, I2, and I3 using mesh analysis. self making from Circuits and Networks (U.A.Patel)
- 47. • For mesh 1, • For mesh 2, • We can find i1 and i2 by substitution method or Cramer’s rule. Then, 123 010)(10515 21 211 ii iii 12 010)(1046 21 1222 ii iiii 2132211 ,, iiIiIiI
- 48. • Use mesh analysis to find the current I0 in the circuit. self making from Circuits and Networks (U.A.Patel)
- 49. • Apply KVL to each mesh. For mesh 1, • For mesh 2, 126511 0)(12)(1024 321 3121 iii iiii 02195 0)(10)(424 321 12322 iii iiiii
- 50. • For mesh 3, • In matrix from become we can calculus i1, i2 and i3 by Cramer’s rule, and find I0. 02 0)(4)(12)(4 ,A,nodeAt 0)(4)(124 321 231321 210 23130 iii iiiiii iII iiiiI 0 0 12 211 2195 6511 3 2 1 i i i
- 51. Mesh Analysis with Current Sources A circuit with a current source. Page no. 2.36 self making from Circuits and Networks (U.A.Patel)
- 52. • Case 1 – Current source exist only in one mesh – One mesh variable is reduced • Case 2 – Current source exists between two meshes, a super-mesh is obtained. A21 i
- 55. REFERENCE • B.L.Theraja, “Electrical Technology Vol.1”, S.Chand Publication. • D.P.Kothari, “Basic Electrical Engineering”, Tata McGraw-Hill publication. • U.A.Patel “Circuits and Networks”.