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Problems 
Section 2-2 Engineering and Linear Models 
P2.2-1 
The element is not linear. For example, doubling the current from 2 A to 4 A does not double the voltage. Hence, the property of homogeneity is not satisfied. 
P2.2-2 
(a) The data points do indeed lie on a straight line. The slope of the line is 0.12 V/A and the line passes through the origin so the equation of the line is 0.12v=. The element is indeed linear. 
(b) When i = 40 mA, v = (0.12 V/A)×(40 mA) = (0.12 V/A)×(0.04 A) = 4.8 mV 
(c) When v = 4 V, 433.3A0.12i== 
P2.2-3 
(a) The data points do indeed lie on a straight line. The slope of the line is 256.5 V/A and the line passes through the origin so the equation of the line is 256.5v=. The element is indeed linear. 
(b) When i = 4 mA, v = (256.5 V/A)×(4 mA) = (256.5 V/A)×(0.004 A) = 1.026 V 
(c) When v = 12 V, 120.04678256.5i== A = 46.78 mA. 
P2.2-4 
Let i = 1 A , then v = 3i + 5 = 8 V. Next 2i = 2A but 16 = 2v ≠ 3(2i) + 5 = 11.. Hence, the property of homogeneity is not satisfied. The element is not linear. 
P2.2-5 
(a) 0.4 3.2 V10408vvvv=+=⇒= 0.08 A40vi== 
(b) 220.4 0.801025vvvv=+⇒+−= 
Using the quadratic formula 0.21.80.8, 1.0 V2v−± ==− 
When v = 0.8 V then 20.80.32 A2i==. When v = -1.0 V then ()210.5 A2i− ==.
(c) 220.40.8 0.801025vvvv=++⇒++= 
Using the quadratic formula 0.20.043.22v−±− = 
So there is no real solution to the equation.
Section 2-4 Resistors 
P2.4-1 3 A and = 7 3 = 21 Vand adhere to the passive convention 21 3 = 63 W is the power absorbed by the resistor. siivRiviPvi===×∴==× 
P2.4-2 333 mA and 24 V24 8000 8 k.003= (310)24 = 7210 72 mWsiivvRiP−− === ====Ω×××= 
P2.4-3 =10 V and 5 10 2A5and adhere to the passive convention 210 20 Wis the power absorbed by the resistorsvvRviRvipvi==Ω=== ∴==⋅= 
P2.4-4 24V and 2 A24 122 242 = 48 WsvvivRipvi=== ===Ω==⋅ 
P2.4-5 121211111 150 V; 50 ; 25 and adhere to the passive convention so 150 3 A50svvvRRviviR=== =Ω=Ω=== 22222150 and do not adhere to the passive convention so 6 A25vviiR=−=−=−
1111The power absorbed by is 1503450 WRPvi==⋅= 2 2 2 2The power absorbed by is 150(6) 900 WRPvi=−=−−= 
P2.4-6 1 2 12 1 1 1 1 1 1 1 1 12 A ; =4 and 8 and do not adhere to the passive convention so 428 V. The power absorbed by is (8)(2) 16 W. siiiRRvivRiRPvi=== Ω=Ω=−=−⋅=− =−=−−= 2 22 2 2 2 2 2 2 and do adhere to the passive convention so 82 16 V . The power absorbed by 16232 W. vivRiRisPvi==⋅= ==⋅= 
P2.4-7 22222Model the heater as a resistor, then(250)with a 250 V source: 62.51000(210)with a 210 V source: 705.6 W62.5vvPRRPvPR=⇒=== === 
P2.4-8 2225000125The current required by the mine lights is: A1203Power loss in the wire is : Thus the maximum resistance of the copper wire allowed is 0.050.055000 0.144 (125/3) now PiviRPRi=== ×===Ω662since the length of the wire is 2100 200 m 20,000 cmthus / with = 1.710cm from Table 2.511.71020,000 0.236cm0.144LRLALAR ρρρ − − =×== =×Ω⋅ ××===
*P2.4-9 3804200.78840.810810238098420gain=≤≤= ++ 0.78840.81080.79962nominalgain+ == 0.79960.78840.81080.7996 1001001.40% 0.79960.7996gaintolerance−− =×=× 
So 
0.79961.40%gain=± 
P2.4-10 
Label the current i as shown. That current is the element current in both resistors. First a40vi= 
Next abba4040vvvRiRRv==⇒= 
For example, 7.054024 11.75R==
Section 2-5 Independent Sources 
P2.5-1 
(a) ()2215 3 A and 53 45 W5sviPRiR====== 
(b) and do not depend on .siPi The values of and are 3 A and 45 W, both when 3 A and when 5 A.ssiPii== 
P2.5-2 
(a) 22 10 5210 V and 20 W5svvRiPR==⋅==== 
(b) and do not depend on . svPv 
The values of and are 10V and 20 W both when 10 V and when 5 VssvPvv== 
P2.5-3 Consider the current source: and do not adhere to the passive convention, so 312 36 W is the power supplied by the current source. sscsssivPiv==⋅= Consider the voltage source: and do adhere to the passive convention, so 312 36 W is the power absorbed by the voltage source. The voltage source supplies 36 W. ssvsssivPiv==⋅= ∴− 
P2.5-4 Consider the current source: and adhere to the passive conventionso 312 36 W is the power absorbed by the current source. Current source supplies 36 W. sscsssivPiv==⋅= − Consider the voltage source: and do not adhere to the passive convention so 31236 W is the power supplied by the voltage source. ssvsssivPiv==⋅=
P2.5-5 
(a) 2(2 cos ) (10 cos )20 cos mWPvittt=== 
(b) 111200011 20 cos =20sin2105 sin 2 mJ 24 wPdttdttt⎛⎞==+=+⎜⎟ ⎝⎠∫∫ 
P2.5-6 
(a) capacity800 mAhtime to discharge 16 hourscurrent50 mA===
Section 2-6 Voltmeters and Ammeters 
P2.6-1 
(a) 5100.5vRi=== 
(b) The voltage, 12 V, and the current, 0.5 A, of the voltage source adhere to the passive convention so the power 
P = 12 (0.5) = 6 W 
is the power received by the source. The voltage source delivers -6 W. 
P2.6-2 
The voltmeter current is zero so the ammeter current is equal to the current source current except for the reference direction: 
i = -2 A 
The voltage v is the voltage of the current source. The power supplied by the current source is 40 W so 
40220 Vvv=⇒=
P2.6-3 
(a) m9001210.8 V900100v⎛⎞==⎜⎟+⎝⎠ 1210.80.110% 12− == 
(b) We require mmmmm12121000.02 0.98 4900 12100RRRRR⎛⎞ −⎜⎟⎜⎟+⎝⎠≥⇒≥⇒ + 
(checked: LNAP 6/16/04) 
P2.6-4 
(a) m100021.98 A100010i⎛⎞==⎜⎟+⎝⎠ 21.98% error1000.99% 2− =×= 
(b) mmm100022100010000.05 0.95 52.63 21000RRR⎛⎞ −⎜⎟⎜⎟+⎝⎠≥⇒≥⇒ + 
(checked: LNAP 6/17/04) 
P2.6-5 
a.) 
()RR2525250 Vvi==−=− 
()mR12125062 Vvv=−=−−= 
b.) 
Element 
Power supplied 
voltage source 
()()s1212224 Wi−=−=− 
current source 
()622124 W=
resistor 
()()RR502100 Wvi−×=−−−=− 
total 
0 
P2.6-6 
a.) RR120.48 A2525vi=== 
mR20.4821.52 Aii=−=−=− 
b.) 
Element 
Power supplied 
voltage source 
()()m12121.5218.24 Wi=−=− 
current source 
()()s2122=24 Wv= 
resistor 
()()RR120.485.76 Wvi−×=−=− 
total 
0
Section 2-7 Dependent Sources 
P2.7-1 842bavri===Ω 
P2.7-2 2 A8 V ; 2 A ; 0.25 8Vabbabivgvigv ====== 
P2.7-3 32A 8 A ; 32A ; 4 8Aabbabiidiidi====== 
P2.7-4 8V2 V ; 8 V ; 4 2Vbaabavvbvvbv====== 
P2.7-5 42 2R=−=Ω− and 2V4 0.5AA==− − 
(checked: LNAP 6/6/04)
P2.7-6 
2 V, 48 A and 2.2 Vcdcdvivv=−==−= 
id and vd adhere to the passive convention so (2.2)(8)17.6 WddPvi==−=− 
is the power received by the dependent source. The power supplied by the dependent source is 17.6 W. 
P2.7-7 
1.25 A, 22.5 V and 1.75 Acdcdivii==== 
id and vd adhere to the passive convention so (2.5)(1.75)4.375 WddPvi=== 
is the power received by the dependent source.
Section 2-8 Transducers 
P2.8-1 360 = , = 360(360)(23V)= =75.27(100 k)(1.1 mA) mpvaRI θθθ° Ω 
P2.8-2 AAD590 : =1 , K=20 V (voltage condition satisfied) kv μ ° 4 A<<13 A4K< <13K iTiTk μμ °° ⎫⎪ ⇒⎬ =⎪⎭
Section 2-9 Switches 
P2.9-1 
At t = 1 s the left switch is open and the right switch is closed so the voltage across the resistor is 10 V. 310= = 2mA510viR= × 
At t = 4 s the left switch is closed and the right switch is open so the voltage across the resistor is 15 V. 315= = 3mA510viR= × 
P2.9-2 
At t = 1 s the current in the resistor is 3 mA so v = 15 V. 
At t = 4 s the current in the resistor is 0 A so v = 0 V. 
P2.9-3 
(a) v = 12 V 
(b) 1001211.43 V105v⎛⎞==⎜⎟ ⎝⎠ 
(c) v = 0 V 
(d) 100120.11880.12 V10100v⎛⎞==⎜⎟ ⎝⎠
Section 2-10 How Can We Check…? 
P2.10-1 =40 V and =(2)2 A. (Notice that the ammeter measures rather than .) 40V So 202AYour lab partner is wrong. osssosviivi−−=− == 
P2.10-2 12We expect the resistor current to be =0.48 A. The power absorbed by25this resistor will be = (0.48) (12) = 5.76 W. A half watt resistor can't absorb this much power. You should nssviRPiv== = ot try another resistor.

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Chapter 2 circuit elements

  • 1. Problems Section 2-2 Engineering and Linear Models P2.2-1 The element is not linear. For example, doubling the current from 2 A to 4 A does not double the voltage. Hence, the property of homogeneity is not satisfied. P2.2-2 (a) The data points do indeed lie on a straight line. The slope of the line is 0.12 V/A and the line passes through the origin so the equation of the line is 0.12v=. The element is indeed linear. (b) When i = 40 mA, v = (0.12 V/A)×(40 mA) = (0.12 V/A)×(0.04 A) = 4.8 mV (c) When v = 4 V, 433.3A0.12i== P2.2-3 (a) The data points do indeed lie on a straight line. The slope of the line is 256.5 V/A and the line passes through the origin so the equation of the line is 256.5v=. The element is indeed linear. (b) When i = 4 mA, v = (256.5 V/A)×(4 mA) = (256.5 V/A)×(0.004 A) = 1.026 V (c) When v = 12 V, 120.04678256.5i== A = 46.78 mA. P2.2-4 Let i = 1 A , then v = 3i + 5 = 8 V. Next 2i = 2A but 16 = 2v ≠ 3(2i) + 5 = 11.. Hence, the property of homogeneity is not satisfied. The element is not linear. P2.2-5 (a) 0.4 3.2 V10408vvvv=+=⇒= 0.08 A40vi== (b) 220.4 0.801025vvvv=+⇒+−= Using the quadratic formula 0.21.80.8, 1.0 V2v−± ==− When v = 0.8 V then 20.80.32 A2i==. When v = -1.0 V then ()210.5 A2i− ==.
  • 2. (c) 220.40.8 0.801025vvvv=++⇒++= Using the quadratic formula 0.20.043.22v−±− = So there is no real solution to the equation.
  • 3. Section 2-4 Resistors P2.4-1 3 A and = 7 3 = 21 Vand adhere to the passive convention 21 3 = 63 W is the power absorbed by the resistor. siivRiviPvi===×∴==× P2.4-2 333 mA and 24 V24 8000 8 k.003= (310)24 = 7210 72 mWsiivvRiP−− === ====Ω×××= P2.4-3 =10 V and 5 10 2A5and adhere to the passive convention 210 20 Wis the power absorbed by the resistorsvvRviRvipvi==Ω=== ∴==⋅= P2.4-4 24V and 2 A24 122 242 = 48 WsvvivRipvi=== ===Ω==⋅ P2.4-5 121211111 150 V; 50 ; 25 and adhere to the passive convention so 150 3 A50svvvRRviviR=== =Ω=Ω=== 22222150 and do not adhere to the passive convention so 6 A25vviiR=−=−=−
  • 4. 1111The power absorbed by is 1503450 WRPvi==⋅= 2 2 2 2The power absorbed by is 150(6) 900 WRPvi=−=−−= P2.4-6 1 2 12 1 1 1 1 1 1 1 1 12 A ; =4 and 8 and do not adhere to the passive convention so 428 V. The power absorbed by is (8)(2) 16 W. siiiRRvivRiRPvi=== Ω=Ω=−=−⋅=− =−=−−= 2 22 2 2 2 2 2 2 and do adhere to the passive convention so 82 16 V . The power absorbed by 16232 W. vivRiRisPvi==⋅= ==⋅= P2.4-7 22222Model the heater as a resistor, then(250)with a 250 V source: 62.51000(210)with a 210 V source: 705.6 W62.5vvPRRPvPR=⇒=== === P2.4-8 2225000125The current required by the mine lights is: A1203Power loss in the wire is : Thus the maximum resistance of the copper wire allowed is 0.050.055000 0.144 (125/3) now PiviRPRi=== ×===Ω662since the length of the wire is 2100 200 m 20,000 cmthus / with = 1.710cm from Table 2.511.71020,000 0.236cm0.144LRLALAR ρρρ − − =×== =×Ω⋅ ××===
  • 5. *P2.4-9 3804200.78840.810810238098420gain=≤≤= ++ 0.78840.81080.79962nominalgain+ == 0.79960.78840.81080.7996 1001001.40% 0.79960.7996gaintolerance−− =×=× So 0.79961.40%gain=± P2.4-10 Label the current i as shown. That current is the element current in both resistors. First a40vi= Next abba4040vvvRiRRv==⇒= For example, 7.054024 11.75R==
  • 6. Section 2-5 Independent Sources P2.5-1 (a) ()2215 3 A and 53 45 W5sviPRiR====== (b) and do not depend on .siPi The values of and are 3 A and 45 W, both when 3 A and when 5 A.ssiPii== P2.5-2 (a) 22 10 5210 V and 20 W5svvRiPR==⋅==== (b) and do not depend on . svPv The values of and are 10V and 20 W both when 10 V and when 5 VssvPvv== P2.5-3 Consider the current source: and do not adhere to the passive convention, so 312 36 W is the power supplied by the current source. sscsssivPiv==⋅= Consider the voltage source: and do adhere to the passive convention, so 312 36 W is the power absorbed by the voltage source. The voltage source supplies 36 W. ssvsssivPiv==⋅= ∴− P2.5-4 Consider the current source: and adhere to the passive conventionso 312 36 W is the power absorbed by the current source. Current source supplies 36 W. sscsssivPiv==⋅= − Consider the voltage source: and do not adhere to the passive convention so 31236 W is the power supplied by the voltage source. ssvsssivPiv==⋅=
  • 7. P2.5-5 (a) 2(2 cos ) (10 cos )20 cos mWPvittt=== (b) 111200011 20 cos =20sin2105 sin 2 mJ 24 wPdttdttt⎛⎞==+=+⎜⎟ ⎝⎠∫∫ P2.5-6 (a) capacity800 mAhtime to discharge 16 hourscurrent50 mA===
  • 8. Section 2-6 Voltmeters and Ammeters P2.6-1 (a) 5100.5vRi=== (b) The voltage, 12 V, and the current, 0.5 A, of the voltage source adhere to the passive convention so the power P = 12 (0.5) = 6 W is the power received by the source. The voltage source delivers -6 W. P2.6-2 The voltmeter current is zero so the ammeter current is equal to the current source current except for the reference direction: i = -2 A The voltage v is the voltage of the current source. The power supplied by the current source is 40 W so 40220 Vvv=⇒=
  • 9. P2.6-3 (a) m9001210.8 V900100v⎛⎞==⎜⎟+⎝⎠ 1210.80.110% 12− == (b) We require mmmmm12121000.02 0.98 4900 12100RRRRR⎛⎞ −⎜⎟⎜⎟+⎝⎠≥⇒≥⇒ + (checked: LNAP 6/16/04) P2.6-4 (a) m100021.98 A100010i⎛⎞==⎜⎟+⎝⎠ 21.98% error1000.99% 2− =×= (b) mmm100022100010000.05 0.95 52.63 21000RRR⎛⎞ −⎜⎟⎜⎟+⎝⎠≥⇒≥⇒ + (checked: LNAP 6/17/04) P2.6-5 a.) ()RR2525250 Vvi==−=− ()mR12125062 Vvv=−=−−= b.) Element Power supplied voltage source ()()s1212224 Wi−=−=− current source ()622124 W=
  • 10. resistor ()()RR502100 Wvi−×=−−−=− total 0 P2.6-6 a.) RR120.48 A2525vi=== mR20.4821.52 Aii=−=−=− b.) Element Power supplied voltage source ()()m12121.5218.24 Wi=−=− current source ()()s2122=24 Wv= resistor ()()RR120.485.76 Wvi−×=−=− total 0
  • 11. Section 2-7 Dependent Sources P2.7-1 842bavri===Ω P2.7-2 2 A8 V ; 2 A ; 0.25 8Vabbabivgvigv ====== P2.7-3 32A 8 A ; 32A ; 4 8Aabbabiidiidi====== P2.7-4 8V2 V ; 8 V ; 4 2Vbaabavvbvvbv====== P2.7-5 42 2R=−=Ω− and 2V4 0.5AA==− − (checked: LNAP 6/6/04)
  • 12. P2.7-6 2 V, 48 A and 2.2 Vcdcdvivv=−==−= id and vd adhere to the passive convention so (2.2)(8)17.6 WddPvi==−=− is the power received by the dependent source. The power supplied by the dependent source is 17.6 W. P2.7-7 1.25 A, 22.5 V and 1.75 Acdcdivii==== id and vd adhere to the passive convention so (2.5)(1.75)4.375 WddPvi=== is the power received by the dependent source.
  • 13. Section 2-8 Transducers P2.8-1 360 = , = 360(360)(23V)= =75.27(100 k)(1.1 mA) mpvaRI θθθ° Ω P2.8-2 AAD590 : =1 , K=20 V (voltage condition satisfied) kv μ ° 4 A<<13 A4K< <13K iTiTk μμ °° ⎫⎪ ⇒⎬ =⎪⎭
  • 14. Section 2-9 Switches P2.9-1 At t = 1 s the left switch is open and the right switch is closed so the voltage across the resistor is 10 V. 310= = 2mA510viR= × At t = 4 s the left switch is closed and the right switch is open so the voltage across the resistor is 15 V. 315= = 3mA510viR= × P2.9-2 At t = 1 s the current in the resistor is 3 mA so v = 15 V. At t = 4 s the current in the resistor is 0 A so v = 0 V. P2.9-3 (a) v = 12 V (b) 1001211.43 V105v⎛⎞==⎜⎟ ⎝⎠ (c) v = 0 V (d) 100120.11880.12 V10100v⎛⎞==⎜⎟ ⎝⎠
  • 15. Section 2-10 How Can We Check…? P2.10-1 =40 V and =(2)2 A. (Notice that the ammeter measures rather than .) 40V So 202AYour lab partner is wrong. osssosviivi−−=− == P2.10-2 12We expect the resistor current to be =0.48 A. The power absorbed by25this resistor will be = (0.48) (12) = 5.76 W. A half watt resistor can't absorb this much power. You should nssviRPiv== = ot try another resistor.