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Electric Circuits Assessment Problems
Chapter 6 Circuit Elements
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Ans: i=Leq β«π‘π v dΟ+i(t0) (a) t Leq = 60(240) 60+240 = 48mH #
6.4 The initial values of i1 and i2 in the circuit shown are +3 A and -5 A, respectively. The voltage at the terminals of the parallel inductors for t > 0 is -30e-5t mV. a) If the parallel inductors are replaced by a single inductor, what is its inductance? b) What is the initial current and its reference direction in the equivalent inductor? c) Use the equivalent inductor to find i(t). d) Find i1(t) and i2(t). Verify that the solutions for i1(t), i2(t), and i(t) satisfy Kirchhoffβs current law. Ans: i=Leq β«π‘π v dΟ+i(t0) (a) Leq = 60(240) = 48mH # t
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t t t 1 48π β«π -0.03e-5ΟdΟ-2 I1(t) = 1 60π β«π -0.03e-5ΟdΟ+3
(b) i1(0)=+3A(εδΈ) i2(0)=-5A(εδΈ) i(0)=-2(εδΈ) # (c) 1 48π β«π -0.03e-5ΟdΟ-2 =0.125e-5t , tβ₯0 # (d) I1(t) = 1 60π β«π -0.03e-5ΟdΟ+3 =0.1e-5t+2.9 , tβ₯0 # I2(t) = π β«π -0.03e-5ΟdΟ-5 =0.025e-5t ,tβ₯0 # t t t
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6.5 The current at the terminals of the two capacitors shown is 240e-10tA for t β₯ 0. The initial values of v1 and v2 are - 10 V and -5V,respectively. Calculate the total energy trapped in the capacitors as t β. (Hint: Don't combine the capacitors in series β find the energy trapped in each, and then add.) Ans: V(t)= 1 πΆ β«π‘0 i dt+v(t0) V1(t)= 1 2ΞΌ β«0 240ΞΌe-10t dt-10 = 2V V2(t)= 1 8ΞΌ β«0 240ΞΌe-10t dt-5 = -2V W1 = 1 2 CV2 =0.5(1.6 ΞΌ) 22 = 4ΞΌJ W2= 1 2 CV2 =0.5(1.6 ΞΌ) -22 = 16ΞΌJ , Wt=16ΞΌ+4ΞΌ =20ΞΌJ # t β β
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Summing the voltages around the π1 mesh yields
a) Write a set of mesh-current equations for the circuit in Example 6.6 if the dot on the 4 H inductor is at the right-hand terminal,the reference direction of ig is reversed, and the 60Ξ© resistor is increased to 780 Ξ©. b) Verify that if there is no energy stored in the circuit at t = 0,and if ig = e-4t A, the solutions to the differential equations derived in (a) of this Assessment Problem are π1 = e-4t + 12e-5tA, π2 = e-4t + e-5tA. Ans: (a) Summing the voltages around the π1 mesh yields 25π1+4 ππ1 ππ‘ -20π2+5πg+8 πππ ππ‘ +8 ππ2 ππ‘ =0 # 780 Ξ©
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Summing the voltages around the π2 mesh yields
-20 π π2 +16 ππ2 ππ‘ +16 πππ ππ‘ + 8 ππ1 ππ‘ =0 # (b) 25π1+4 ππ1 ππ‘ -20π2+5πg+8 πππ ππ‘ +8 ππ2 ππ‘ = β ππ1 ππ‘ = 46.40eβ4t β 60eβ5t ; 4 ππ1 ππ‘ = eβ4t β 240eβ5t ππ2 ππ‘ = 3.96eβ4t β 5eβ5t ; 8 ππ2 ππ‘ = 31.68eβ4t β 40eβ5t πππ ππ‘ = 7.84eβ4t ; 8 πππ ππ‘ = 62.72eβ4t 25π1 = β10 β 290eβ4t + 300eβ5t 20π2 = β0.20 β 19.80eβ4t + 20eβ5t 5πg = 9.8 β 9.8eβ4t
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-10-290e-4t+300e-5t+185. 6e-4t-240e-5t+0. 2+19. 8e-4t-20e-5t+9. 8-9
e-4t+300e-5t+185.6e-4t-240e-5t e-4t-20e-5t e-4t+31.68e-4t- 40e-5t+62.72e-4t= β‘ β =β‘ OK -20 π π2 +16 ππ2 ππ‘ +16 πππ ππ‘ + 8 ππ1 ππ‘ = β’ 8 ππ1 ππ‘ =371.20eβ4t β 480eβ5t 16 ππ2 ππ‘ =63.36eβ4t β 80eβ5t 16 πππ ππ‘ =125.44eβ4t 20 π1 = β8 β 232eβ4t + 240eβ5t 800π2 = β8 β 792eβ4t + 800eβ5t 8+232e-4t-240e-5t-8-792e-4t+800e-5t+63.36e-4t-80e-5t e-4t e-4t -480e-5t= β£ β’=β£ OK
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