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The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson Section number ________ Student Name _______________________________________ Electric Circuits I Midterm #1 Problems Points 1. _____ 4 2. _____ 6 3. _____ 5 Total _____ 15 Was the exam fair ? yes no f11m1s_elci.fm - 1 The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson Problem 1 Section number ________ f11m1s_elci.fm - 2 Student Name _______________________________________ 4 points Given is the electric circuit model, shown in Figure 1.1. RV b VV = 24V R1 + VR1 - VV R2 Vab IR1 RV = 10 kΩ R1= 30 kΩ R2= 20 kΩ a Fig.1.1 An electric circuit model and its parameter values. For the electric circuit model of Figure 1.1, demonstrate: 1. an ability to apply the voltage divider formula, by using it to calculate the value of voltage VR1 across the resistor R1 indicated in the circuit model of Figure 1.1; 2. an ability to apply the Ohm’s Law, by using the Ohm’s Law to calculate the value of the current IR1 flowing through resistor R1 in the circuit model of Figure 1.1. Hint #1 For full credit: all equations, all answers to questions, all circuit models and other graphical representations are expected to be entered into the space designated for them; all shown numerical results must be preceded by the symbolic and numeric expressions whose evaluation produces the numerical results. Solution For full credit, an explicit demonstration of understanding the following solution steps is expected. 1 1.1 Applying the voltage divider formula, calculate the value of the indicated voltage VR1 accross the resistor R1 in the circuit model of Figure 1.1; show your work in the space reserved for equation (1-1). VR1 = 1 1.2 R1 RV + R2 + R1 VV = 30⋅103 24 = 12V (10 + 20 + 30)⋅103 (1-1) Applying the passive convention for coupled positive reference directions of the voltage and current of the resistor R1, indicate in the circuit model of Figure 1.1 the positive reference direction of the current IR1. The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson 1 f11m1s_elci.fm - 3 Student Name _______________________________________ 1.3 Using the positive reference direction determined for current IR1 in part 1.2 and applying the Ohm’s Law, calculate the value of the current IR1 through resistor R1 in the circuit model of Figure 1.1; show your work in the space reserved for equation (1-2). IR1 = 1 Section number ________ 1.4 VR1 R1 = 12 = 0.4mA 30⋅103 (1-2) Determine the positive reference direction, and the value of the magnitude, of the voltage Vab between the terminals a and b in the circuit model of Figure 1.1; show the positive reference direction of Vab in the circuit model of figure 1.1 and show your calculatiuon of the magnitude’s value in the space reserved for equation (1-3). Vab = R1⋅( −IR1) = 30⋅103 ⋅ ( −0.4⋅10-3) = - 12V Or alternatively, using the calculated value of the voltage VR1, Vab = - Vba = - VR1 = - 12V (1-3) The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson Problem 2 Section number ________ f11m1s_elci.fm - 4 Student Name _______________________________________ 6 points Given is the electric circuit model, shown in Figure 2.1. R 1= 4 Ω R 3= 5 Ω II = 15A R 2= 2 Ω R4= 10 Ω VV = 25V 1 II R1 R2 V1 2 R3 Vv V2 -+ IVV II R4 R2 1 R1 2 R3 V1 V2 0 (a) R4 IV 0 (b) Figure 2.1 The electric circuit model with positive reference directions for currents and voltages that ought to be calculated. (a)Drawing of the circuit model. (b)Equivalent representationof the circuit model if one will be used in the solution process. For the electric circuit model of Figure 2.1, demonstrate an ability to use the Nodal Voltage Method to determine a partial solution that includes: (a) voltage VI across the current source II, (b) power delivered by the energy source VV to the circuit of Figure 2.1, (c) electrical energy delivered by the energy source VV to the circuit of Figure 2.1 during a time interval ∆t=5 minutes.. Hint #1 For full credit: all equations, all answers to questions, all circuit models and other graphical representations are expected to be entered into the space designated for them; all shown numerical results must be preceded by the symbolic and numeric expressions whose evaluation produces the numerical results. Solution For full credit, an explicit demonstration of understanding the following solution steps is expected. 2.1 1 In any case, select and show in Figure 2.1 the positive reference directions for the nodal-voltages. Additionally, when the solution processt, or just a simplification of the drawing, involves replacement of a part of the circuita by an equivalent circuit, show the new equivalent form of the whole electric circuit model in the space reserved for Figure 2.1(b); also write in the space reserved for equation (2-1) any volttage-current relation needed to complete the electrical model shown in Figure 2,1(b). . As NVM is based on the application of the KCL, and a current-voltage relation does not exist for an ideal voltage source, the application of NVM requires that part of the circuit consisting of the series connection of the voltage source VV and resistor R4 be replaced by the equivalent Norton’s circuit. After this replacement is applied, the circuit model of Figure 2.1(b) is obtained, and the The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson Section number ________ f11m1s_elci.fm - 5 Student Name _______________________________________ equation (2-1) explicitely defines the introduced Norton’s current source parameter IV . IV = G4VV 0.5 2.2 (2-1) For the circuit model of Figure 2.1(b), prepare the set of canonical form nodal-voltage equations. Show your work in the space reserved for equations (2-2). Since the circuit model of Figure 2.1(b) does not contain any voltage sources, direct application of the NVM is applicable to it, and its corresponding normal form NVM system of equations is, G11V1 - G12V2 = II (2-2) -G21V1 + G22V2 = - IV 1 2.3 Prepare the symbolic expressions and calculate the numerical values of the coefficients in equations (2-2) (the self and mutual conductancess of the nodes); show the calculation in the space reserved for equations (2-3). G1 = G2 = G3 = G4 = 2.4 1 ∆= 1 R1 1 R2 1 R3 = = = 1 4 1 2 1 5 = 0.25 S = 0.5 S G11= G2 + G1 = 0.5 + 0.25 = 0.75 S G22= G4 + G3 + G2 = 0.1 + 0.2 + 0.5 = 0.8 S G12 = G21 = G2 = 0.5 S = 0.2 S (2-3) 1 1 R4 = 10 = 0.1 S Prepare symbolic expressions (in terms of the nodal-voltage equation coefficients), and calculate the values of determinants involved in the solution of equations (2-2); show the calculation in the space reserved for equations (2-4). G11 -G12 -G21 G22 = G11G22 -G21G12 = 0.75.0.8 - 0.5.0.5 = 0.35 S2 (2-4) ∆ 1= ∆ 2= II -G12 -G4VV G22 G11 II -G21 -G4VV = G22 II - G4VV G12 = 0.8.15 -0.1.25.0.5 = 12 - 1.25= 10.75 SA = - G4VV G11 + G21II = - 0.1.25.0.75 + 0.5.15= -1.875+7.5= 5.625 SA The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson 0.5 2.5 2.6 1 Section number ________ f11m1s_elci.fm - 6 Student Name _______________________________________ Based on the values of determinants obtained in the step 2.4, calculate the numerical values of the nodal-voltages; show the calculation in the space reserved for equations (2-5). V1= ∆1 10.75 = = 30.71 V ∆ 0.35 V2 = ∆2 5.625 ∆ = 0.35 = 16.07 V (2-5) Indicate in the circuit of Figure 2.1(a) the active convention positive reference direction for the:current IVV flowing through the voltage source VV and then determine the value of current IVV; show the calculation in the space reserved for equation (2-6). Since there exists no current-voltage relation for an ideal voltage source, the currrent IVV can not be determined directly; instead, as the voltage source VV and resistor R4 are connected in series, their currents are equal, and determining the current IR4 of the resistor provides the value of the current IVV too. OL: IR4 = VR4⋅G4 = (VV + V2)⋅G4 = [25 + 16.07]⋅0.1 = 4.1A IVV = IR4 = 4.1A 0.5 2.7 (2-6) Calculate the power which the energy source VV delivers/consumes to/from the circuit of Figure 2.1; show the calculation in the space reserved for equations (2-7). The power delivered by the energy sourceVV is (2-7) PV = VVIVV = 25⋅4.1 = 102.5 W 0.5 2.8 Calculate the amount of electrical energy WV deliverd/consumed by the energy source VV in the circuit of Figure 1.1 during the time interval ∆t; show the calculation in the space reserved for equations (2-8). The energy deliverd/consumed by the energy source VV to the circuit during the time interval ∆t is calculated as WV = PV⋅∆t = 102.5⋅300 = 30.75 kJ ⇒ delivered (2-8) The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson Problem 3 Section number ________ f11m1s_elci.fm - 7 Student Name _______________________________________ 5 points Given is a resistive network whose electrical model is shown in Figure 3.1. a R1 R2= 6 Ω R5 = 20 Ω R3 =60 Ω R6 = 40 Ω Rab VV R3 → R5 R4 - R4 = 20 Ω + R1 = 9 Ω R2 b VV = 25V R6 Figure 3.1 Electrical model of a resistive network and its parametr values. For the electric circuit model of Figure 3.1, demonstrate : 1. an ability to apply the series/parallel reduction method, to calculate the value of the equivalent resistance Rab seen by the voltage source VV between terminals a and b, 2. an ability to calculate the amount of power that the ideal voltage source VV delivers to the resistive network in Figure 3.1. Hint #1 For full credit: all equations, all answers to questions, all circuit models and other graphical representations are expected to be entered into the space designated for them; all shown numerical results must be preceded by the symbolic and numeric expressions whose evaluation produces the numerical results. Solution For full credit, an explicit demonstration of understanding the following solution steps is expected .3.1 2 For the resistive part of the network of Figure 3.1, prepare the graphical representations of three equivalent networks of gradually decreasing complexity, which result when resistors connected in series/parallel are replaced by an equivalent resistor. Show the three graphical representations, in the order of their creation, in the space reserved for Figure 3.2. Label the equivalent resistances at each reduction step by Rxy, where x and y are texts of your own choice. a R1 Rab → R2 R34 b R56 (a) a a R1 Rab → R2 Rab → R1 b b R23456 R3456 (b) Figure 3.2 Reduction steps for the resistive network of Figure 3.1. (c) The University of Toledo EECS:2300 Electric Circuits Dr. Anthony D. Johnson 3.2 2 Section number ________ f11m1s_elci.fm - 8 Student Name _______________________________________ Calculate the values of all equivalent resistances indicated in Figure 3.2; show the work in the space reserved for equations (3-1). R34 = R3|| R4 = R3⋅R4 60⋅ 20 = 15Ω R3+ R4 = 60 + 20 R56 = R5+ R6 = 20 + 40 = 60Ω R3456 = R34|| R56 = R34⋅R56 R34+ R56 = 15⋅ 60 = 12Ω 15 + 60 (3-1) R23456 = R2+ R3456 = 6 + 12 = 18Ω R1⋅R34567 R12 + R34567 = Rab = R1|| R23456 = 3.3 1 9⋅ 18 9 + 18 = 6Ω Calculate the power PV which the voltage source VV delivers to the resistive network in Figure 3.1. Show the calculation in the space reserved for equation (3-2). 2 PV = VV = Rab 25 6 2 = 104W (3-2)