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ELEC221: Tutorial 1
Mina Wahib
9/22/2015 Mina Wahib
Introduction
Text book
9/22/2015 Mina Wahib
Electric Circuits (Newest Edition) 10th Edition
by James W. Nilsson (Author), Susan Riedel (Author)
Introduction
Simple Circuit Modelling (1)
9/22/2015 Mina Wahib
 Electrical systems can be modelled by using circuit models
 Circuits are the interconnection of electrical components such as resistors, capacitors, inductors
and switches
Introduction
Simple Circuit Modelling (2)
9/22/2015 Mina Wahib
Sources Cables Electrical
Equipment
Introduction
Electrical Components
9/22/2015 Mina Wahib
Circuits Elements
Passive Active
+
-
Introduction
Circuit Variables
9/22/2015 Mina Wahib
 Current (I) : Time-rate of change of electric charge (1 Ampere = 1 Coulomb/ 1 Sec.)
𝐼 =
π‘‘π‘ž
𝑑𝑑
𝐴
 Voltage (V) : Electromotive force or potential (1 Volt = 1 Joule (N.m) / 1 Coulomb)
𝑉 =
π‘‘π‘Š
π‘‘π‘ž
𝑉
 Power (P) : Time-rate of change of energy (1 Watt = 1 Joule / 1 Sec.)
𝑃 =
π‘‘π‘Š
𝑑𝑑
= 𝐼 𝑉 π‘Šπ‘Žπ‘‘π‘‘
Introduction
Passive Sign Convention
9/22/2015 Mina Wahib
Circuit
Element
1 2+ -
𝐼
𝑉
𝑷 = 𝑰 𝑽
𝑃 > 0
Power Absorbed
𝑃 < 0
Power Supplied
Introduction
Power Balance + Passive Sign Convention
9/22/2015 Mina Wahib
-
π‘ƒπ‘Ž = 120 βˆ’10 = βˆ’1200 π‘Š
𝑃𝑏 = βˆ’ 120 9 = βˆ’1080 π‘Š
𝑃𝑐 = 10 10 = 100 π‘Š
𝑃𝑑 = βˆ’ 10 βˆ’1 = 10 π‘Š
𝑃𝑒 = βˆ’10 βˆ’9 = 90 π‘Š
𝑃𝑓 = βˆ’ βˆ’100 5 = 500 π‘Š
𝑃𝑔 = 120 4 = 480 π‘Š
π‘ƒβ„Ž = βˆ’220 βˆ’5 = 1100 π‘Š
π‘ƒπ‘Žπ‘π‘  = 2280 π‘Š 𝑃𝑠𝑒𝑝𝑝 = βˆ’2280 π‘Š 𝑃𝑛𝑒𝑑 = 0 π‘Š+ = Power Balanced !
Introduction
KVL and KCL
9/22/2015 Mina Wahib
KVL: The sum of voltage drops around a closed path must equal zero
KCL: The sum of currents leaving a node must equal zero.
βˆ’π‘‰π‘Ž + 𝑉2 + 𝑉𝑏 = 0 π‘ƒπ‘Žπ‘‘β„Ž 1
βˆ’π‘‰π‘ βˆ’ 𝑉3 + 𝑉𝑐 = 0 (π‘ƒπ‘Žπ‘‘β„Ž 2)
βˆ’π‘‰π‘Ž + 𝑉2 βˆ’ 𝑉3 + 𝑉𝑐 = 0 (π‘ƒπ‘Žπ‘‘β„Ž 3)
Introduction
KVL and KCL
9/22/2015 Mina Wahib
KVL: The sum of voltage drops around a closed path must equal zero
KCL: The sum of currents leaving a node must equal zero.
βˆ’4 + 𝑖 + 10 = 24
𝑖 = 18 𝐴
Problems
Problem 1
9/22/2015 Mina Wahib
Solution
π‘ž =
0
∞
𝑖 𝑑𝑑 =
0
∞
20π‘’βˆ’5000𝑑 𝑑𝑑 =
20π’†βˆ’πŸ“πŸŽπŸŽπŸŽπ’•
βˆ’πŸ“πŸŽπŸŽπŸŽ
∞
0
= 4000 πœ‡πΆ
Remember that’s the integration of an exponential
It’s the same exact exponential divided by the
derivative of the power of the exponential
Problems
Problem 2
9/22/2015 Mina Wahib
Solution
π‘Ž 𝑃 = 𝑉 𝐼 = 10,000π‘’βˆ’5000𝑑
20π‘’βˆ’5000𝑑
𝑃 0.001 = 0.908π‘Š
𝑏 𝑀 𝑑 =
0
∞
𝑝 𝑑 𝑑𝑑 = 20 𝐽
Remember that’s the integration of an exponential
It’s the same exact exponential divided by the
derivative of the power of the exponential
Problems
Problem 3
9/22/2015 Mina Wahib
Remember that this could be a non-constant
function (linear 1st order) as well, and in that case
multiplying it by another non-constant function
(linear 1st order) will result in a 2nd order function
Problems
Problem 3 (Cont’d)
9/22/2015 Mina Wahib
Solution
𝑀 1 =
1
2
1 100 = 50 𝐽
𝑀 6 =
1
2
1 100 βˆ’
1
2
1 100 +
1
2
1 100 βˆ’
1
2
1 100 = 0𝐽
𝑀 10 = 𝑀 6 +
1
2
1 100 = 50 𝐽
Area of the triangles under the curve
Problems
Problem 4
9/22/2015 Mina Wahib
Solution
π‘Ž 𝑝 = 0.25π‘’βˆ’3200𝑑
βˆ’ 0.5π‘’βˆ’2000𝑑
+ 0.25π‘’βˆ’800𝑑
𝑝 625 πœ‡π‘  = 42.2 π‘šπ‘Š
𝑏 𝑀 =
0
625 πœ‡π‘ 
0.25π‘’βˆ’3200𝑑
βˆ’ 0.5π‘’βˆ’2000𝑑
+ 0.25π‘’βˆ’800𝑑
𝑑𝑑
= 12.14 πœ‡π½
𝑐 𝑀 =
0
∞
0.25π‘’βˆ’3200𝑑 βˆ’ 0.5π‘’βˆ’2000𝑑 + 0.25π‘’βˆ’800𝑑 𝑑𝑑
= 140.625 πœ‡π½
Problems
Problem 5
9/22/2015 Mina Wahib
Solution
𝑖 =
π‘‘π‘ž
𝑑𝑑
= π‘‘π‘’βˆ’π›Όπ‘‘
π’…π’Š
𝒅𝒕
= 𝟎 𝒇𝒐𝒓 π’Žπ’‚π’™. 𝒄𝒖𝒓𝒓𝒆𝒏𝒕
1 βˆ’ 𝛼𝑑 π‘’βˆ’π›Όπ‘‘ = 0
∴ 𝑑 =
1
𝛼
∴ 𝑖 =
1
𝛼
π‘’βˆ’1 β‰… 10 𝐴
Problems
Problem 6
9/22/2015 Mina Wahib
Solution
π‘Ž 𝑃 = 𝑉 𝐼 = 80,000π‘‘π‘’βˆ’500𝑑
15π‘‘π‘’βˆ’500𝑑
𝑑𝑃
𝑑𝑑
= π‘’βˆ’1000𝑑 2𝑑 βˆ’ 1000𝑑2 = 0
𝑑 = 2 π‘šπ‘ π‘’π‘
𝑏 𝑃 2 π‘šπ‘ π‘’π‘ = 649.6 π‘šπ‘Š
𝒄 𝑬 𝒕𝒐𝒕𝒂𝒍 =
𝟎
∞
𝑷 𝒕 𝒅𝒕
Problems
Problem 6
9/22/2015 Mina Wahib
Solution (Cont’d)
𝑐 πΈπ‘‘π‘œπ‘‘π‘Žπ‘™
= 1200,000
0
∞
𝑑2 π‘’βˆ’1000𝑑 𝑑𝑑 = 1200,000 {(
π’†βˆ’πŸπŸŽπŸŽπŸŽπ’•
βˆ’πŸπŸŽπŸŽπŸŽ
𝒕 𝟐) βˆ’
0
∞
π’†βˆ’πŸπŸŽπŸŽπŸŽπ’•
βˆ’πŸπŸŽπŸŽπŸŽ
πŸπ’•} = 1200,000{
π‘’βˆ’1000𝑑
βˆ’10002 2𝑑 βˆ’
0
∞
π‘’βˆ’1000𝑑
βˆ’10002 2}
= 1200,000
βˆ’2
1000
0 βˆ’
1
1000 2
= 2.4 π‘šπ½
Remember that’s the integration by parts
(Integration of the simpler function X the second function as it it) – (Integration of the function I
already integrated X Derivative of the second function)
Problems
Problem 7
9/22/2015 Mina Wahib
𝑃1 = βˆ’205 π‘Š
𝑃2 = 60 π‘Š
𝑃3 = 45 π‘Š
𝑃4 = 45 π‘Š
𝑃5 = 30 π‘Š
𝑃3 =? 𝑃3 = 70 π‘Š (𝑅𝑒𝑐𝑒𝑖𝑣𝑒𝑑 π‘ƒπ‘œπ‘€π‘’π‘Ÿ)
Problems
Problem 8
9/22/2015 Mina Wahib
𝑃1 = βˆ’300 π‘Š
𝑃2 = 100 π‘Š
𝑃3 = 280 π‘Š
𝑃4 = βˆ’32 π‘Š
𝑃5 = βˆ’48 π‘Š
Problems
Problem 9
9/22/2015 Mina Wahib
π‘ƒπ‘‘π‘œπ‘‘π‘Žπ‘™ = βˆ’100 + 20𝐼0 + 36 + 24 = 0 π‘Š
𝐼0 = 2 𝐴
Problems
Problem 10
9/22/2015 Mina Wahib
π‘ƒπ‘‘π‘œπ‘‘π‘Žπ‘™ = βˆ’180 + 72 + 56 + 28 + 3𝑉0 βˆ’ 30 = 0 π‘Š
𝑉0 = 18 𝑉
Problems
Problem 11
9/22/2015 Mina Wahib
A constant current of 3 A for 4 hours is required to
charge an automotive battery. If the terminal voltage is
(𝟏𝟎 + 𝒕/𝟐 ) 𝑽, where t is in hours,
(a) How much charge is transported as a result of the
charging?
(b) How much energy is expended?
(c) How much does the charging cost? Assume
electricity costs 9 cents/kWh.
Solution
π‘Ž π‘ž =
0
𝑇
3 𝑑𝑑 = 3 𝑇 = 3 Γ— 4 Γ— 60 Γ— 60 = 43.2 𝐾𝐢
𝑏 π‘Š =
0
𝑇
𝑝 𝑑𝑑 =
0
𝑇
(3)(10 +
𝑑
2
) 𝑑𝑑
= 3 10𝑑 +
𝑑2
4
= 132 π‘Šβ„Ž
𝑐 πΆπ‘œπ‘ π‘‘ = 9
𝑐𝑒𝑛𝑑𝑠
π‘˜π‘Šβ„Ž
Γ— 0.132 π‘˜π‘Šβ„Ž = 1.188 𝐢𝑒𝑛𝑑𝑠
Problems
Problem 12
9/22/2015 Mina Wahib
Solution
π‘Ž π‘ž =
0
2
πŸ‘π’†βˆ’πŸπ’• 𝑑𝑑 = βˆ’
3
2
π‘’βˆ’4 βˆ’ 1 = 1.472 𝐢
𝑏 𝑃 = 𝑉 𝐼 = βˆ’90π‘’βˆ’4𝑑 π‘Š
𝑐 π‘Š =
0
3
βˆ’90π‘’βˆ’4𝑑 𝑑𝑑 =
90
4
π‘’βˆ’12 βˆ’ 1 = βˆ’22.49 𝐽
The current entering the positive terminal of a device is
π’Š(𝒕) = πŸ‘π’†βˆ’πŸπ’•
𝑨 and the voltage across the device is
𝒗(𝒕) = πŸ“ π’…π’Š/𝒅𝒕 𝑽.
(a) Find the charge delivered to the device between t = 0
and t = 2 s.
(b) Calculate the power absorbed.
(c) Determine the energy absorbed in 3 s.
Problems
Problem 13
9/22/2015 Mina Wahib
Solution
π‘Ž π‘ž =
0
1
10(1 βˆ’ π‘’βˆ’0.5𝑑 )𝑑𝑑 = 2.1306 𝐢
𝑏 𝑃 = 𝑣 𝑑 𝑖 𝑑 = 5π‘π‘œπ‘ π‘‘ 2𝑑 Γ— 10 1 βˆ’ π‘’βˆ’0.5𝑑
= 5 cos 2 π‘Ÿπ‘Žπ‘‘ Γ— 10 1 βˆ’ π‘’βˆ’0.5
= βˆ’8.187 π‘Š
The voltage v across a device and the current i through it
are 𝑣(𝑑) = 5 cos 2𝑑 𝑉, 𝑖(𝑑) = 10(1 βˆ’ π‘’βˆ’0.5𝑑 ) 𝐴
Calculate:
(a) The total charge in the device at t = 1 s
(b) The power consumed by the device at t = 1 s.
Problems
Problem 14
9/22/2015 Mina Wahib
Find 𝑉 using KVL and KCL
Solution:
KVL around the blue path:
βˆ’18 βˆ’ 1 6 + 2 3 + 4 4 βˆ’ 𝑉 = 0 ∴ 𝑉 = βˆ’2 𝑉
Problems
Problem 15
9/22/2015 Mina Wahib
Find 𝐼1, 𝐼2 using KVL and KCL
Solution:
KCL at a: 𝐼1 + 𝐼2 + 4 = 0
KCL at b: 𝐼2 + 𝐼3 + 4 = 6
KCL at c: 𝐼1 + 6 = 𝐼3 KVL around blue path: βˆ’12 + 3𝐼1 + 6𝐼1 + 9𝐼3 = 0 ∴ 𝐼1 = βˆ’
7
3
𝐴 , 𝐼2 = βˆ’
5
3
𝐴
Important Remarks
9/22/2015 Mina Wahib
 Don’t forget to revise the integration rules (integration by parts and the integration of other different
functions)
 Don’t forget to convert all units to the fundamental SI units (A, V, S, W….)
 Don’t forget to revise the differentiation rules (exponentials, sins, cosines…..)
 Email me whenever you have any questions at 13mmw@queensu.ca or Minawahib@Hotmail.com
Or directly come to my office at WLH506, Cubicle #9

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Tutorial_1_Mina_Wahib

  • 1. ELEC221: Tutorial 1 Mina Wahib 9/22/2015 Mina Wahib
  • 2. Introduction Text book 9/22/2015 Mina Wahib Electric Circuits (Newest Edition) 10th Edition by James W. Nilsson (Author), Susan Riedel (Author)
  • 3. Introduction Simple Circuit Modelling (1) 9/22/2015 Mina Wahib  Electrical systems can be modelled by using circuit models  Circuits are the interconnection of electrical components such as resistors, capacitors, inductors and switches
  • 4. Introduction Simple Circuit Modelling (2) 9/22/2015 Mina Wahib Sources Cables Electrical Equipment
  • 5. Introduction Electrical Components 9/22/2015 Mina Wahib Circuits Elements Passive Active + -
  • 6. Introduction Circuit Variables 9/22/2015 Mina Wahib  Current (I) : Time-rate of change of electric charge (1 Ampere = 1 Coulomb/ 1 Sec.) 𝐼 = π‘‘π‘ž 𝑑𝑑 𝐴  Voltage (V) : Electromotive force or potential (1 Volt = 1 Joule (N.m) / 1 Coulomb) 𝑉 = π‘‘π‘Š π‘‘π‘ž 𝑉  Power (P) : Time-rate of change of energy (1 Watt = 1 Joule / 1 Sec.) 𝑃 = π‘‘π‘Š 𝑑𝑑 = 𝐼 𝑉 π‘Šπ‘Žπ‘‘π‘‘
  • 7. Introduction Passive Sign Convention 9/22/2015 Mina Wahib Circuit Element 1 2+ - 𝐼 𝑉 𝑷 = 𝑰 𝑽 𝑃 > 0 Power Absorbed 𝑃 < 0 Power Supplied
  • 8. Introduction Power Balance + Passive Sign Convention 9/22/2015 Mina Wahib - π‘ƒπ‘Ž = 120 βˆ’10 = βˆ’1200 π‘Š 𝑃𝑏 = βˆ’ 120 9 = βˆ’1080 π‘Š 𝑃𝑐 = 10 10 = 100 π‘Š 𝑃𝑑 = βˆ’ 10 βˆ’1 = 10 π‘Š 𝑃𝑒 = βˆ’10 βˆ’9 = 90 π‘Š 𝑃𝑓 = βˆ’ βˆ’100 5 = 500 π‘Š 𝑃𝑔 = 120 4 = 480 π‘Š π‘ƒβ„Ž = βˆ’220 βˆ’5 = 1100 π‘Š π‘ƒπ‘Žπ‘π‘  = 2280 π‘Š 𝑃𝑠𝑒𝑝𝑝 = βˆ’2280 π‘Š 𝑃𝑛𝑒𝑑 = 0 π‘Š+ = Power Balanced !
  • 9. Introduction KVL and KCL 9/22/2015 Mina Wahib KVL: The sum of voltage drops around a closed path must equal zero KCL: The sum of currents leaving a node must equal zero. βˆ’π‘‰π‘Ž + 𝑉2 + 𝑉𝑏 = 0 π‘ƒπ‘Žπ‘‘β„Ž 1 βˆ’π‘‰π‘ βˆ’ 𝑉3 + 𝑉𝑐 = 0 (π‘ƒπ‘Žπ‘‘β„Ž 2) βˆ’π‘‰π‘Ž + 𝑉2 βˆ’ 𝑉3 + 𝑉𝑐 = 0 (π‘ƒπ‘Žπ‘‘β„Ž 3)
  • 10. Introduction KVL and KCL 9/22/2015 Mina Wahib KVL: The sum of voltage drops around a closed path must equal zero KCL: The sum of currents leaving a node must equal zero. βˆ’4 + 𝑖 + 10 = 24 𝑖 = 18 𝐴
  • 11. Problems Problem 1 9/22/2015 Mina Wahib Solution π‘ž = 0 ∞ 𝑖 𝑑𝑑 = 0 ∞ 20π‘’βˆ’5000𝑑 𝑑𝑑 = 20π’†βˆ’πŸ“πŸŽπŸŽπŸŽπ’• βˆ’πŸ“πŸŽπŸŽπŸŽ ∞ 0 = 4000 πœ‡πΆ Remember that’s the integration of an exponential It’s the same exact exponential divided by the derivative of the power of the exponential
  • 12. Problems Problem 2 9/22/2015 Mina Wahib Solution π‘Ž 𝑃 = 𝑉 𝐼 = 10,000π‘’βˆ’5000𝑑 20π‘’βˆ’5000𝑑 𝑃 0.001 = 0.908π‘Š 𝑏 𝑀 𝑑 = 0 ∞ 𝑝 𝑑 𝑑𝑑 = 20 𝐽 Remember that’s the integration of an exponential It’s the same exact exponential divided by the derivative of the power of the exponential
  • 13. Problems Problem 3 9/22/2015 Mina Wahib Remember that this could be a non-constant function (linear 1st order) as well, and in that case multiplying it by another non-constant function (linear 1st order) will result in a 2nd order function
  • 14. Problems Problem 3 (Cont’d) 9/22/2015 Mina Wahib Solution 𝑀 1 = 1 2 1 100 = 50 𝐽 𝑀 6 = 1 2 1 100 βˆ’ 1 2 1 100 + 1 2 1 100 βˆ’ 1 2 1 100 = 0𝐽 𝑀 10 = 𝑀 6 + 1 2 1 100 = 50 𝐽 Area of the triangles under the curve
  • 15. Problems Problem 4 9/22/2015 Mina Wahib Solution π‘Ž 𝑝 = 0.25π‘’βˆ’3200𝑑 βˆ’ 0.5π‘’βˆ’2000𝑑 + 0.25π‘’βˆ’800𝑑 𝑝 625 πœ‡π‘  = 42.2 π‘šπ‘Š 𝑏 𝑀 = 0 625 πœ‡π‘  0.25π‘’βˆ’3200𝑑 βˆ’ 0.5π‘’βˆ’2000𝑑 + 0.25π‘’βˆ’800𝑑 𝑑𝑑 = 12.14 πœ‡π½ 𝑐 𝑀 = 0 ∞ 0.25π‘’βˆ’3200𝑑 βˆ’ 0.5π‘’βˆ’2000𝑑 + 0.25π‘’βˆ’800𝑑 𝑑𝑑 = 140.625 πœ‡π½
  • 16. Problems Problem 5 9/22/2015 Mina Wahib Solution 𝑖 = π‘‘π‘ž 𝑑𝑑 = π‘‘π‘’βˆ’π›Όπ‘‘ π’…π’Š 𝒅𝒕 = 𝟎 𝒇𝒐𝒓 π’Žπ’‚π’™. 𝒄𝒖𝒓𝒓𝒆𝒏𝒕 1 βˆ’ 𝛼𝑑 π‘’βˆ’π›Όπ‘‘ = 0 ∴ 𝑑 = 1 𝛼 ∴ 𝑖 = 1 𝛼 π‘’βˆ’1 β‰… 10 𝐴
  • 17. Problems Problem 6 9/22/2015 Mina Wahib Solution π‘Ž 𝑃 = 𝑉 𝐼 = 80,000π‘‘π‘’βˆ’500𝑑 15π‘‘π‘’βˆ’500𝑑 𝑑𝑃 𝑑𝑑 = π‘’βˆ’1000𝑑 2𝑑 βˆ’ 1000𝑑2 = 0 𝑑 = 2 π‘šπ‘ π‘’π‘ 𝑏 𝑃 2 π‘šπ‘ π‘’π‘ = 649.6 π‘šπ‘Š 𝒄 𝑬 𝒕𝒐𝒕𝒂𝒍 = 𝟎 ∞ 𝑷 𝒕 𝒅𝒕
  • 18. Problems Problem 6 9/22/2015 Mina Wahib Solution (Cont’d) 𝑐 πΈπ‘‘π‘œπ‘‘π‘Žπ‘™ = 1200,000 0 ∞ 𝑑2 π‘’βˆ’1000𝑑 𝑑𝑑 = 1200,000 {( π’†βˆ’πŸπŸŽπŸŽπŸŽπ’• βˆ’πŸπŸŽπŸŽπŸŽ 𝒕 𝟐) βˆ’ 0 ∞ π’†βˆ’πŸπŸŽπŸŽπŸŽπ’• βˆ’πŸπŸŽπŸŽπŸŽ πŸπ’•} = 1200,000{ π‘’βˆ’1000𝑑 βˆ’10002 2𝑑 βˆ’ 0 ∞ π‘’βˆ’1000𝑑 βˆ’10002 2} = 1200,000 βˆ’2 1000 0 βˆ’ 1 1000 2 = 2.4 π‘šπ½ Remember that’s the integration by parts (Integration of the simpler function X the second function as it it) – (Integration of the function I already integrated X Derivative of the second function)
  • 19. Problems Problem 7 9/22/2015 Mina Wahib 𝑃1 = βˆ’205 π‘Š 𝑃2 = 60 π‘Š 𝑃3 = 45 π‘Š 𝑃4 = 45 π‘Š 𝑃5 = 30 π‘Š 𝑃3 =? 𝑃3 = 70 π‘Š (𝑅𝑒𝑐𝑒𝑖𝑣𝑒𝑑 π‘ƒπ‘œπ‘€π‘’π‘Ÿ)
  • 20. Problems Problem 8 9/22/2015 Mina Wahib 𝑃1 = βˆ’300 π‘Š 𝑃2 = 100 π‘Š 𝑃3 = 280 π‘Š 𝑃4 = βˆ’32 π‘Š 𝑃5 = βˆ’48 π‘Š
  • 21. Problems Problem 9 9/22/2015 Mina Wahib π‘ƒπ‘‘π‘œπ‘‘π‘Žπ‘™ = βˆ’100 + 20𝐼0 + 36 + 24 = 0 π‘Š 𝐼0 = 2 𝐴
  • 22. Problems Problem 10 9/22/2015 Mina Wahib π‘ƒπ‘‘π‘œπ‘‘π‘Žπ‘™ = βˆ’180 + 72 + 56 + 28 + 3𝑉0 βˆ’ 30 = 0 π‘Š 𝑉0 = 18 𝑉
  • 23. Problems Problem 11 9/22/2015 Mina Wahib A constant current of 3 A for 4 hours is required to charge an automotive battery. If the terminal voltage is (𝟏𝟎 + 𝒕/𝟐 ) 𝑽, where t is in hours, (a) How much charge is transported as a result of the charging? (b) How much energy is expended? (c) How much does the charging cost? Assume electricity costs 9 cents/kWh. Solution π‘Ž π‘ž = 0 𝑇 3 𝑑𝑑 = 3 𝑇 = 3 Γ— 4 Γ— 60 Γ— 60 = 43.2 𝐾𝐢 𝑏 π‘Š = 0 𝑇 𝑝 𝑑𝑑 = 0 𝑇 (3)(10 + 𝑑 2 ) 𝑑𝑑 = 3 10𝑑 + 𝑑2 4 = 132 π‘Šβ„Ž 𝑐 πΆπ‘œπ‘ π‘‘ = 9 𝑐𝑒𝑛𝑑𝑠 π‘˜π‘Šβ„Ž Γ— 0.132 π‘˜π‘Šβ„Ž = 1.188 𝐢𝑒𝑛𝑑𝑠
  • 24. Problems Problem 12 9/22/2015 Mina Wahib Solution π‘Ž π‘ž = 0 2 πŸ‘π’†βˆ’πŸπ’• 𝑑𝑑 = βˆ’ 3 2 π‘’βˆ’4 βˆ’ 1 = 1.472 𝐢 𝑏 𝑃 = 𝑉 𝐼 = βˆ’90π‘’βˆ’4𝑑 π‘Š 𝑐 π‘Š = 0 3 βˆ’90π‘’βˆ’4𝑑 𝑑𝑑 = 90 4 π‘’βˆ’12 βˆ’ 1 = βˆ’22.49 𝐽 The current entering the positive terminal of a device is π’Š(𝒕) = πŸ‘π’†βˆ’πŸπ’• 𝑨 and the voltage across the device is 𝒗(𝒕) = πŸ“ π’…π’Š/𝒅𝒕 𝑽. (a) Find the charge delivered to the device between t = 0 and t = 2 s. (b) Calculate the power absorbed. (c) Determine the energy absorbed in 3 s.
  • 25. Problems Problem 13 9/22/2015 Mina Wahib Solution π‘Ž π‘ž = 0 1 10(1 βˆ’ π‘’βˆ’0.5𝑑 )𝑑𝑑 = 2.1306 𝐢 𝑏 𝑃 = 𝑣 𝑑 𝑖 𝑑 = 5π‘π‘œπ‘ π‘‘ 2𝑑 Γ— 10 1 βˆ’ π‘’βˆ’0.5𝑑 = 5 cos 2 π‘Ÿπ‘Žπ‘‘ Γ— 10 1 βˆ’ π‘’βˆ’0.5 = βˆ’8.187 π‘Š The voltage v across a device and the current i through it are 𝑣(𝑑) = 5 cos 2𝑑 𝑉, 𝑖(𝑑) = 10(1 βˆ’ π‘’βˆ’0.5𝑑 ) 𝐴 Calculate: (a) The total charge in the device at t = 1 s (b) The power consumed by the device at t = 1 s.
  • 26. Problems Problem 14 9/22/2015 Mina Wahib Find 𝑉 using KVL and KCL Solution: KVL around the blue path: βˆ’18 βˆ’ 1 6 + 2 3 + 4 4 βˆ’ 𝑉 = 0 ∴ 𝑉 = βˆ’2 𝑉
  • 27. Problems Problem 15 9/22/2015 Mina Wahib Find 𝐼1, 𝐼2 using KVL and KCL Solution: KCL at a: 𝐼1 + 𝐼2 + 4 = 0 KCL at b: 𝐼2 + 𝐼3 + 4 = 6 KCL at c: 𝐼1 + 6 = 𝐼3 KVL around blue path: βˆ’12 + 3𝐼1 + 6𝐼1 + 9𝐼3 = 0 ∴ 𝐼1 = βˆ’ 7 3 𝐴 , 𝐼2 = βˆ’ 5 3 𝐴
  • 28. Important Remarks 9/22/2015 Mina Wahib  Don’t forget to revise the integration rules (integration by parts and the integration of other different functions)  Don’t forget to convert all units to the fundamental SI units (A, V, S, W….)  Don’t forget to revise the differentiation rules (exponentials, sins, cosines…..)  Email me whenever you have any questions at 13mmw@queensu.ca or Minawahib@Hotmail.com Or directly come to my office at WLH506, Cubicle #9