Chapter 9.

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Presentation transcript:

Chapter 9

Summary Summary Simultaneous Equations Circuit analysis methods in Chapter 9 require use of simultaneous equations. To simplify solving simultaneous equations, they are usually set up in standard form. Standard form for two equations with two unknowns is constants coefficients variables

Summary Summary Simultaneous Equations Example: Solution: A circuit has the following equations. Set up the equations in standard form. Solution: Rearrange so that variables and their coefficients are in order and put constants on the right.

Summary Summary Solving Simultaneous Equations Three methods for solving simultaneous equations are Algebraic substitution The determinant method Using a calculator

Summary Summary Solving Simultaneous Equations Example: Solution: Solve for IA using substitution. Solution: Solve for IB in the first equation: Substitute for IB into the second equation: Rearrange and solve for IA. IA = 9.53 mA

Summary Summary Solving Simultaneous Equations If you wanted to find IB in the previous example, you can substitute the result of IA back into one of the original equations and solve for IB. Thus, 2.10 mA

Summary Summary Solving Simultaneous Equations Example: Solution: The method of determinants is another approach to finding the unknowns. The characteristic determinant is formed from the coefficients of the unknowns. Write the characteristic determinant for the equations. Calculate its value. Example: Solution: 1.134

Summary Summary Solving Simultaneous Equations To solve for an unknown by determinants, form the determinant for a variable by substituting the constants for the coefficients of the unknown. Divide by the characteristic determinant. To solve for x2: Constants Unknown variable Characteristic determinant

Summary Summary Solving Simultaneous Equations Example: Solution: Solve the same equations using determinants: Solution: 9.53 mA 2.10 mA

Summary Summary Solving Simultaneous Equations Many scientific calculators allow you to enter a set of equations and solve them “automatically”. The calculator method will depend on your particular calculator, but you will always write the equations in standard form first and then input the number of equations, the coefficients, and the constants. Pressing the Solve key will show the values of the unknowns.

Summary Summary Branch current method In the branch current method, you can solve for the currents in a circuit using simultaneous equations. Steps: Assign a current in each branch in an arbitrary direction. Show polarities according to the assigned directions. Apply KVL in each closed loop. Apply KCL at nodes such that all branches are included. Solve the equations from steps 3 and 4.

Summary Summary Branch current method Example: Solution: Solve the equations from steps 3 and 4 (see next slide). Apply KVL in each closed loop. Resistors are entered in kW in this example. Apply KCL at nodes such that all branches are included. Show polarities according to the assigned directions. Assign a current in each branch in an arbitrary direction. Solution: A + + +

Summary Summary Branch current method Solution: In standard form, the equations are (Continued) Solving: I1 = 9.53 mA, I2 = 7.43 mA, I3 = -2.10 mA The negative result for I3 indicates the actual current direction is opposite to the assumed direction.

Solving 3x3 Matrix

Summary Summary Loop current method OR Mesh Analysis In the loop current method, you can solve for the currents in a circuit using simultaneous equations. Steps: Assign a current in each nonredundant loop in an arbitrary direction. Show polarities according to the assigned direction of current in each loop. Apply KVL around each closed loop. Solve the resulting equations for the loop currents.

Summary Summary Loop current method Example: Solution: Apply KVL around each closed loop. Resistors are entered in kW in this example. Solve the resulting equations for the loop currents (see following slide). Show polarities according to the assigned direction of current in each loop. Assign a current in each nonredundant loop in an arbitrary direction. Solution: Notice that the polarity of R3 is based on loop B and is not the same as in the branch current method. + + + Loop A Loop B +

Summary Summary Loop current method Solution: Rearranging the loop equations into standard form: (Continued) I1=IA = 9.53 mA I2= IA-IB = 7.43 mA I3=IB = 2.10 mA + + + Loop A Loop B +

Solution has been given in Class

Summary Summary Loop current method applied to circuits with more than two loops The loop current method can be applied to more complicated circuits, such as the Wheatstone bridge. The steps are the same as shown previously. The advantage to the loop method for the bridge is that it has only 3 unknowns. Loop A Loop B Loop C

Summary Summary Example: Write the loop current equation for Loop A in the Wheatstone bridge: Loop A Loop B Loop C

Summary Summary Node voltage method In the node voltage method, you can solve for the unknown voltages in a circuit using KCL. Steps: Determine the number of nodes. Select one node as a reference. Assign voltage designations to each unknown node. Assign currents into and out of each node except the reference node. Apply KCL at each node where currents are assigned. Express the current equations in terms of the voltages and solve for the unknown voltages using Ohm’s law.

Summary Summary Node voltage method Example: Solution: Solve the same problem as before using the node voltage method. Solution: Write KCL in terms of the voltages (next slide). Apply KCL at node A (for this case). There are 4 nodes. A is the one unknown node. Currents are assigned into and out of node A. B is selected as the reference node. A B

Summary Summary Node voltage method Solution: (Continued) A B

Key Terms Branch One current path that connects two nodes. Determinant Loop Matrix Node Simultaneous equations One current path that connects two nodes. The solution of a matrix consisting of an array of coefficients and constants for a set of simultaneous equations. A closed current path in a circuit. An array of numbers. The junction of two or more components. A set of n equations containing n unknowns, where n is a number with a value of 2 or more.

Quiz In a set of simultaneous equations, the coefficient that is written a1,2 appears in a. the first equation b. the second equation c. both of the above d. none of the above

Quiz In standard form, the constants for a set of simultaneous equations are written a. in front of the first variable b. in front of the second variable c. on the right side of the equation d. all of the above

Quiz To solve simultaneous equations, the minimum number of independent equations must be at least a. two b. three c. four d. equal to the number of unknowns

Quiz In the equation a1,1x1 +a1,2x2 = b1, the quantity b1 represents a. a constant b. a coefficient c. a variable d. none of the above

Quiz 5. The value of the determinant is a. 4 b. 14 c. 24 d. 34

Quiz The characteristic determinant for a set of simultaneous equations is formed using a. only constants from the equations b. only coefficients from the equations c. both constants and coefficients from the equations d. none of the above

Quiz A negative result for a current in the branch method means a. there is an open path b. there is a short circuit c. the result is incorrect d. the current is opposite to the assumed direction

Quiz To solve a circuit using the loop method, the equations are first written for each loop by applying a. KCL b. KVL c. Ohm’s law d. Thevenin’s theorem

Quiz A Wheatstone bridge can be solved using loop equations. The minimum number of nonredundant loop equations required is a. one b. two c. three d. four

Quiz In the node voltage method, the equations are developed by first applying a. KCL b. KVL c. Ohm’s law d. Thevenin’s theorem

Quiz Answers: 1. a 2. c 3. d 4. a 5. b 6. b 7. d 8. b 9. c 10. a