1. 1 © Unitec New Zealand DE4401&APTE 5601 Topic 4 N ETWORK A NALYSIS

2. Introduction Review: –Ohm’s Law –Resistors connected in series, in parallel or combination –Kirchhoff’s Voltage Law –Kirchhoff’s Current Law –Voltage and current dividers Today: –Network analysis: Branch current method Loop current method (AK only) Node voltage method 2 © Unitec New Zealand

3. Revision 3 © Unitec New Zealand

4. Branch, Nodes and Loop KVL can be used to determine an unknown voltage in a complex circuit, where all other voltages around a particular "loop" are known. 4 © Unitec New Zealand

5. Kirchhoff's Current Law (KCL) The algebraic sum of all currents entering and exiting a node must equal zero. 5 © Unitec New Zealand or

6. Kirchhoff's Voltage Law "The algebraic sum of all voltages in a loop must equal zero“ 6 © Unitec New Zealand

7. Voltage divider 7 © Unitec New Zealand The ratio of individual resistance to total resistance is the same as the ratio of individual voltage drop to total supply voltage in a voltage divider circuit. This is known as the voltage divider formula

8. Current divider 8 © Unitec New Zealand It is sometimes necessary to find the individual branch currents in a parallel circuit if the resistances and total current are known, but the voltage across the resistance bank is not known. When only two branches are involved, the current in one branch will be some fraction of the total current. This fraction is the quotient of the second resistance divided by the sum of the resistances.

9. Network Analysis Generally speaking, network analysis is any structured technique used to mathematically analyze a circuit (a “network” of interconnected components). Usually, a single equation will not be useful and we will need a system of equations. –The rule is: we need as many equations as we have unknown currents. The techniques developed for DC circuits will be used for AC circuits as well. 9 © Unitec New Zealand

10. Network Analysis Methods Branch current method Loop current method Node voltage method 10 © Unitec New Zealand

11. Branch current method The first and most straightforward network analysis technique is called the Branch Current Method. In this method, we assume directions of currents in a network, then write equations describing their relationships to each other through Kirchhoff's and Ohm's Laws. Once we have one equation for every unknown current, we can solve the simultaneous equations and determine all currents, and therefore all voltage drops in the network. 11 © Unitec New Zealand

12. Branch current method steps Steps to follow for the “Branch Current” method of analysis: (1) Choose a node and assume directions of currents. (2) Write a KCL equation relating currents at the node. (3) Label resistor voltage drop polarities based on assumed currents. (4) Write KVL equations for each loop of the circuit, substituting the product IR for E in each resistor term of the equations. (5) Solve for unknown branch currents (simultaneous equations). –If any solution is negative, then the assumed direction of current for that solution actually flows the opposite way! (6) Solve for voltage drops across all resistors (E=IR). 12 © Unitec New Zealand

13. Example 1 13 © Unitec New Zealand

14. (1) Choose a node and assume directions of currents. 14 © Unitec New Zealand

15. (2) Write a KCL equation relating currents at the node. 15 © Unitec New Zealand If any for current solution is negative, then the assumed direction of current for that solution is wrong!

16. (3) Label resistor voltage drop polarities based on assumed currents. The following is not the case in our example here, but just so you know: It is OK if the polarity of a resistor's voltage drop doesn't match with the polarity of the nearest battery, so long as the resistor voltage polarity is correctly based on the assumed direction of current through it. In some cases we may discover that current will be forced backwards through a battery, causing this very effect. 16 © Unitec New Zealand

17. (4) Write KVL equations for each loop of the circuit, substituting the product IR for E in each resistor term of the equations. 17 © Unitec New Zealand

18. (6) Solve for voltage drops across all resistors (V=IR). 18 © Unitec New Zealand

19. (5) Solve for unknown branch currents (simultaneous equations). If any solution is negative, then the assumed direction of current for that solution is wrong! 19 © Unitec New Zealand

20. Loop (Mesh) Current Method The Loop Current Method, also known as the Mesh Current Method, is quite similar to the Branch Current method in that it uses simultaneous equations, Kirchhoff's Voltage Law, and Ohm's Law to determine unknown currents in a network. It differs from the Branch Current method in that it does not use Kirchhoff's Current Law. 20 © Unitec New Zealand

21. Example We will analyze the same circuit: 21 © Unitec New Zealand

22. Step one: identify “loops” Identify “loops” within the circuit, encompassing all components. –In our example circuit: First loop is formed by E 1, R 1, and R 2 Second loop is formed by E 2, R 2, and R 3 –The choice of each current's direction is arbitrary, but the equations are easier to solve if the currents are going the same direction through intersecting components (here, R 2 ). 22 © Unitec New Zealand

23. Step two: label all voltage drop polarities The next step is to label all voltage drop polarities across resistors according to the assumed directions of the loop currents. –The battery polarities, of course, are dictated by their symbol orientations in the diagram, and may or may not “agree” with the resistor polarities (assumed current directions) 23 © Unitec New Zealand

24. Step three: write equation for each loop Write KVL equations for each loop, substituting the product IR for E in each resistor term of the equation. –Where two loop currents intersect through a component, express the current as the algebraic sum of those two loop currents (i.e. I 1 + I 2 if the currents go in the same direction through that component or I 1 - I 2 if not.) 24 © Unitec New Zealand

25. Step four: solve the equations In this example we have two equations with two unknowns 25 © Unitec New Zealand

26. Step five: calculating branch currents The result we have obtained is for the loop currents, not branch currents. So, in this step, we must go back to our diagram to see how they fit together to give currents through all components (branch currents). –Remember: negative current value means that the current flows in the direction opposite from the assumed. (see figure below) 26 © Unitec New Zealand This change of current direction from what was first assumed will alter the polarity of the voltage drops across R 2 and R 3 due to current I 2.

27. Step five (cont.) We can say that the current through R 1 is 5 amps. Also, we can safely say that the current through R 3 is 1 amp, with a voltage drop of 1 volt (E=IR), positive on the left and negative on the right. To determine the actual current through R 2, we must see how mesh currents I 1 and I 2 interact in this case they're in opposition 27 © Unitec New Zealand We algebraically add them (minding the sign +/-) : Since I 1 is going “down” at 5 amps, and I 2 is going “up” at 1 amp, the real current through R 2 must be the difference, 4 amps, going “down”

28. Step six: calculate voltages Using Ohm’s law, calculate voltages on all resistors. V = IR 28 © Unitec New Zealand

29. Loop current method: advantages The primary advantage of Loop Current analysis is that it generally allows for the solution of a large network with fewer unknown values and fewer simultaneous equations than Branch Current method. –Our example problem took three equations to solve the Branch Current method and only two equations using the Loop Current method. 29 © Unitec New Zealand

30. Revise Steps for Loop Current Method ( 1) Draw currents in loops of circuit, to account for all components. (2) Label resistor voltage drop polarities based on assumed directions of loop currents. (3) Write KVL equations for each loop, substituting the product IR for E in each resistor term of the equation. Where two mesh currents intersect through a component, express the current as the algebraic sum of those two mesh currents (i.e. I 1 + I 2 if the currents go in the same direction through that component or I 1 - I 2 if not.) (4) Solve for unknown loop currents (simultaneous equations). If any solution is negative, the assumed current direction is wrong! (5) Algebraically add loop currents to find current in components which share multiple loop currents. (6) Solve for voltage drops across all resistors (V=IR). 30 © Unitec New Zealand

31. Task 1 Analyse the following circuit using: –Loop current method –Branch current method 31 © Unitec New Zealand

32. Task 2 Analyse the following circuit using: –Loop current method –Branch current method 32 © Unitec New Zealand

33. Node Voltage Method Node Voltage Method is one of the major techniques in circuit analysis. It reduces the number of equations you have to deal with. Node Voltage Method for solving a circuit uses node voltage drops to specify the currents at a node. Then, node equations of currents are written to satisfy Kirchhoff's current law. By solving the node equations, we can calculate the unknown node voltages. 33 © Unitec New Zealand

34. Terminology A node is a common connection for two or more components in a circuit. A principal node has three or more connections (some call it ‘junction’) One of the principal nodes is chosen as a reference node and this node is connected to the ground (defined as 0 volts). –Because a reference node has 0 volts, you can simplify analysis by choosing a node where a large number of devices are connected as your reference node. A node voltage is the voltage of a given node with respect to the reference node (i.e.to the ground). 34 © Unitec New Zealand

35. Node, principal node and reference node A node voltage is the voltage of a given node with respect to the reference node 35 © Unitec New Zealand

36. Notation used in this class To each node in a circuit, a letter or number is assigned. Example: A, B, G, and N are nodes, and G and N are principal nodes. Select node G connected to ground as the reference node. –Then V AG is the voltage between nodes A and G, V BG is the voltage between nodes B and G, and V NG is the voltage between nodes N and G. –Since the node voltage is always determined with respect to a specified reference node, the notations V A for V AG, V B for V BG, and V N for V NG are used. 36 © Unitec New Zealand

37. Steps for Node Voltage Method 1.Mark nodes (use letters i. e. A, B, C, G). Select a reference (ground) node. 2.Assume the direction of currents. Mark the voltage polarity across each resistor, consistent with assumed direction of current. 3.Formulate a Kirchhoff’s Current Law (KCL) equation for each non-reference principal node. 4.Express all branch currents in terms of voltage drops on components (e.g. resistor in the branch) by using relationships such as Ohm’s law ( I = V/R) and the rule for the voltage in parallel branches (“ all parallel branches have the same voltage”). Resulting equations are now expressed in terms of unknown principal voltages. 5.With the equations from step 4, go back to the KLC equations from step 3. Simplify the equations to put them in standard form. 6.Solve the system of equations to find principal node voltages. 7.Next, find all voltage drops and currents in the branches. 37 © Unitec New Zealand

38. Example: we analyse the same circuit Step one: Mark nodes and select a reference (ground) node. 38 © Unitec New Zealand

39. Step two: current directions, polarities Assume the direction of currents. Mark the voltage polarity across each resistor, consistent with assumed direction of current. 39 © Unitec New Zealand

40. Step three: KCL Formulate a Kirchhoff’s Current Law (KCL) equation for each non-reference principal node. –In this case, only one principal node, N. 40 © Unitec New Zealand

41. Step four: Voltage equations Express all branch currents in terms of voltage drops on components (e.g. resistor in the branch) by using relationships such as Ohm’s law ( I = V/R) and the rule for the voltage in parallel branches (“ all parallel branches have the same voltage”). Resulting equations are now expressed in terms of unknown principal voltages. 41 © Unitec New Zealand

42. Step five and step six: Step five: With the equations from step 5, go back to the KLC equations from step 4. Simplify the equations to put them in standard form. –In this example, we have a single equation only. 42 © Unitec New Zealand Step six: Solve the system of equations to find principal node voltages. (again: here it’s only one equation, not a system)

43. Step seven Next, find all voltage drops and currents in the branches. 43 © Unitec New Zealand

44. Task 3 Analyse the circuit from Task 1 using Node Voltage Method 44 © Unitec New Zealand

45. Task 4 Analyse the circuit from Task 2 using Node Voltage Method 45 © Unitec New Zealand

46. Literature for Node Voltage Method Chapter 5 in book: ‘Circuit Analysis For Dummies’ Santiago, John; available online from Unitec Library Page 105 Schaum’s Basic Electricity ; available from Moodle in pdf format for download or a book from Unitec Library 46 © Unitec New Zealand

47. Maths revision If algebra is a problem for you, please look up “system of equations” in Khan academy. –In the class, we will use Elimination method. –Please practice Substitution and Matrix methods as well. 47 © Unitec New Zealand