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Welcome to
Classes
BYJU’S
Alternating Current
What you already know
What you will learn
S5: AC Circuits (Combination)
1 . Sinu so idal AC param e te rs
2 . Phasor diagram s
3 . Pu re re sistiv e AC circu its
4. Pu re capacitiv e AC circu its
5 . Pu re indu ctiv e AC circu its
1 . Im pe dance
2 . RC co m b inatio n
3 . L R co m b inatio n
Pure inductive AC circuit
𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’
πœ‹
2
𝑖0 =
πœ€0
πΏπœ”
=
πœ€0
𝑋𝐿
SI Unit : Ohm (Ξ©)
πœ€ = πœ€0 sin πœ”π‘‘
𝐿
𝑉𝐿
𝑋𝐿 = πΏπœ” Inductive reactance
Phase difference πœ™ = πœ”π‘‘ βˆ’
πœ‹
2
βˆ’ πœ”π‘‘ = βˆ’
πœ‹
2
Current lags potential by 90Β°
Pure inductive AC circuit
𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’
πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
Phasor diagram
𝑖0
𝑦
π‘₯
πœ€0
πœ”π‘‘
Wave diagram
𝑑
𝑖, πœ€
0 πœ‹ 2πœ‹
πœ‹
2
3πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’
πœ‹
2
πœ€0
𝑖0
𝑖0
Pure capacitive AC circuit
πœ€ = πœ€0 sin πœ”π‘‘
𝐢
𝑖 = 𝑖0 sin πœ”π‘‘ +
πœ‹
2
𝑖0 =
πœ€0
1
πΆπœ”
=
πœ€0
𝑋𝐢
SI Unit : Ohm Ξ©
𝑋𝐢 =
1
πΆπœ”
Capacitive reactance
Phase difference πœ™ = πœ”π‘‘ +
πœ‹
2
βˆ’ πœ”π‘‘ =
πœ‹
2
Current leads potential by 90Β°
Pure capacitive AC circuit
Phasor diagram
𝑖0
𝑦
π‘₯
πœ€0
πœ”π‘‘
Wave diagram
𝑖 = 𝑖0 sin πœ”π‘‘ +
πœ‹
2
𝑑
𝑖, πœ€
0 πœ‹ 2πœ‹
πœ‹
2
3πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
πœ€0
𝑖0
𝑖0
Simple AC circuits
Element Current (emf:πœ€ = πœ€0 sin πœ”π‘‘) πœ™ 𝑋(Reactance)
Resistor
Inductor
Capacitor
πœ€0
𝑅
sin πœ”π‘‘
πœ€0
πœ”πΏ
sin πœ”π‘‘ βˆ’
πœ‹
2
πœ€0
ΰ΅—
1
πœ”πΆ
sin πœ”π‘‘ +
πœ‹
2
0
βˆ’
πœ‹
2
πœ‹
2
𝑅
πœ”πΏ
1
πœ”πΆ
Wave diagram
𝑑
𝑖, πœ€
0 πœ‹ 2πœ‹
πœ‹
2
3πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’
πœ‹
2
πœ€0
𝑖0
𝑖0
0 β†’
πœ‹
2
πœ‹
2
β†’ πœ‹
πœ‹ β†’
3πœ‹
2
3πœ‹
2
β†’ 2πœ‹
πœ€ = πœ€0 sin πœ”π‘‘
𝑉𝐿
πœ€ increases from zero to maximum,
current becomes zero.
πœ€ decreases from maximum to zero,
current grows to maximum.
πœ€ increases from zero to negative
maximum, current becomes zero.
πœ€ decreases from negative maximum
to zero, current grows to negative
maximum.
Current tries to follow path of voltage.
The phase difference between them
always remains to be 90Β°.
𝑑
𝑖, πœ€
0 πœ‹ 2πœ‹
πœ‹
2
3πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’
πœ‹
2
πœ€0
𝑖0
𝑖0
𝑑
𝑖, πœ€
0 πœ‹ 2πœ‹
πœ‹
2
3πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’
πœ‹
2
πœ€0
𝑖0
𝑖0
The lagging of current can be seen from the mechanical analogy as shown. Height represents the voltage and
velocity of block is current. When height is maximum, velocity is zero and vice-versa.
Wave diagram
𝑑
𝑖, πœ€
0 πœ‹ 2πœ‹
πœ‹
2
3πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’
πœ‹
2
πœ€0
𝑖0
𝑖0
πœ€ = πœ€0 sin πœ”π‘‘
𝐢
Wave diagram
𝑖 = 𝑖0 sin πœ”π‘‘ +
πœ‹
2
𝑑
𝑖, πœ€
0 πœ‹ 2πœ‹
πœ‹
2
3πœ‹
2
πœ€ = πœ€0 sin πœ”π‘‘
πœ€0
𝑖0
𝑖0
𝑍
The relation b/w peak current and peak voltages can be written as
Purely resistive circuit Purely inductive circuit
𝑖0 =
E0
𝑍
𝑍 = 𝑅 𝑍 = πœ”πΏ
𝑍 is called impedance.
Impedance is defined as the opposition any circuit shows
when voltage is applied to it.
SI unit is Ohm (Ξ©)
Purely capacitive circuit
𝑍 = 1/πœ”πΆ
βˆ’ |
E0 sin πœ”π‘‘
𝐢
𝑅
E0
2
= 𝑉𝑅
2
+ 𝑉𝐢
2
E0
2
= 𝑖0
2
𝑅2 + 𝑖0
2
𝑋𝐢
2
𝑖0
2
𝑍2 = 𝑖0
2
𝑅2 + 𝑖0
2
𝑋𝐢
2
𝑍2
= 𝑅2
+ 𝑋𝐢
2
𝑍 = 𝑅2 + 𝑋𝐢
2
𝑍 = 𝑅2 + 1/πœ”πΆ 2
𝑋𝐢 = 1/πœ”πΆ
β‡’
𝑉𝑅
πœ™
𝑉𝐢 E0
𝑖0
βˆ’ |
𝑍 = 𝑅2 + 1/πœ”πΆ 2
tan πœ™ =
𝑋𝐢
𝑅
πœ™
𝑋𝐢
𝑅
𝑍
E0 sin πœ”π‘‘
𝐢
𝑅
tan πœ™ =
1
πœ”πΆπ‘…
𝑍2 = 𝑅2 + 𝑋𝐢
2
𝑋𝐢 =
1
πœ”πΆ
Peak current (𝑖0) is given by-
𝑖0 =
E0
𝑍
=
E0
𝑅2 + 1/πœ”πΆ 2
𝑉𝑅
πœ™
𝑉𝐢 E0
𝑖0
βˆ’ |
𝑍 = 𝑅2 + 1/πœ”πΆ 2
tan πœ™ =
1
πœ”πΆπ‘…
𝑖0 =
E0
𝑍
=
E0
𝑅2 + 1/πœ”πΆ 2
Steady state current (𝑖) in the circuit
𝑖 =
E0
𝑍
sin(πœ”π‘‘ + πœ™)
E0 sin πœ”π‘‘
𝐢
𝑅
The current leads the emf by πœ™.
𝑉𝑅
πœ™
𝑉𝐢 E0
𝑖0
βˆ’ |
E0
2
= 𝑉𝑅
2
+ 𝑉𝐿
2
E0
2
= 𝑖0
2
𝑅2
+ 𝑖0
2
𝑋𝐿
2
𝑖0
2
𝑍2 = 𝑖0
2
𝑅2 + 𝑖0
2
𝑋𝐿
2
𝑍2 = 𝑅2 + 𝑋𝐿
2
𝑍 = 𝑅2 + 𝑋𝐿
2
𝑍 = 𝑅2 + πœ”πΏ 2
𝑋𝐿 = πœ”πΏ
β‡’
E0 sin πœ”π‘‘
𝐿
𝑅
𝑉𝑅
πœ™
𝑉𝐿
E0
𝑖0
βˆ’ |
tan πœ™ =
𝑋𝐿
𝑅
πœ™
𝑋𝐿
𝑅
𝑍
tan πœ™ =
πœ”πΏ
𝑅
𝑋𝐿 = πœ”πΏ
Peak current (𝑖0) is given by-
𝑖0 =
E0
𝑍
=
E0
𝑅2 + πœ”πΏ 2
𝑍2 = 𝑅2 + 𝑋𝐿
2
𝑍 = 𝑅2 + πœ”πΏ 2
E0 sin πœ”π‘‘
𝐿
𝑅
𝑉𝑅
πœ™
𝑉𝐿
E0
𝑖0
βˆ’ |
tan πœ™ =
πœ”πΏ
𝑅
Steady state current (𝑖) in the circuit
𝑖 =
E0
𝑍
sin(πœ”π‘‘ βˆ’ πœ™) E0 sin πœ”π‘‘
𝐿
𝑅
𝑉𝑅
πœ™
𝑉𝐿
E0
𝑖0
𝑍 = 𝑅2 + πœ”πΏ 2
𝑖0 =
E0
𝑍
=
E0
𝑅2 + πœ”πΏ 2
The current lags the emf by πœ™.
In the given circuit, find
(a) inductive reactance 𝑋𝐿 .
(b) impedance 𝑍.
(c) Peak current 𝑖0.
(d) i(t) πœ€ = 200 sin(100πœ‹π‘‘)
𝐿 =
2
πœ‹
𝐻
𝑅 = 200 Ξ©
πœ€ = 200 sin(100πœ‹π‘‘)
𝐿 =
2
πœ‹
𝐻
𝑅 = 200 Ξ©
(a) inductive reactance 𝑋𝐿 .
𝑋𝐿 = πœ”πΏ
𝑋𝐿 = 100πœ‹ Γ—
2
πœ‹
= 200 Ξ©
πœ™
𝑋𝐿
𝑅
𝑍
𝑍2 = 𝑅2 + 𝑋𝐿
2
𝑍 = 𝑅2 + 𝑋𝐿
2
∴ 𝑍 = 200 2 Ξ©
𝑍 = (200)2+ 200 2
(b) impedance 𝑍.
πœ€ = 200 sin(100πœ‹π‘‘)
𝐿 =
2
πœ‹
𝐻
𝑅 = 200 Ξ©
(c) Peak current 𝑖0.
𝑖0 =
πœ€0
𝑍
πœ€0 = 200 𝑉
𝑖0 =
200
200 2
=
1
2
𝐴
𝑉𝑅
πœ™
𝑉𝐿
Ξ΅0
𝑖0
πœ™
𝑋𝐿
𝑅
𝑍
(d) i(t)
𝑖 𝑑 = 𝑖0 sin 100πœ‹π‘‘ βˆ’ πœ™
tan πœ™ =
𝑋𝐿
𝑅
=
200
200
= 1 β‡’ πœ™ =
πœ‹
4
∴ 𝑖 𝑑 =
1
2
sin 100πœ‹π‘‘ βˆ’
πœ‹
4

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AC- circuits (combination).pdf

  • 1. Welcome to Classes BYJU’S Alternating Current What you already know What you will learn S5: AC Circuits (Combination) 1 . Sinu so idal AC param e te rs 2 . Phasor diagram s 3 . Pu re re sistiv e AC circu its 4. Pu re capacitiv e AC circu its 5 . Pu re indu ctiv e AC circu its 1 . Im pe dance 2 . RC co m b inatio n 3 . L R co m b inatio n
  • 2. Pure inductive AC circuit 𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’ πœ‹ 2 𝑖0 = πœ€0 πΏπœ” = πœ€0 𝑋𝐿 SI Unit : Ohm (Ξ©) πœ€ = πœ€0 sin πœ”π‘‘ 𝐿 𝑉𝐿 𝑋𝐿 = πΏπœ” Inductive reactance Phase difference πœ™ = πœ”π‘‘ βˆ’ πœ‹ 2 βˆ’ πœ”π‘‘ = βˆ’ πœ‹ 2 Current lags potential by 90Β°
  • 3. Pure inductive AC circuit 𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’ πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ Phasor diagram 𝑖0 𝑦 π‘₯ πœ€0 πœ”π‘‘ Wave diagram 𝑑 𝑖, πœ€ 0 πœ‹ 2πœ‹ πœ‹ 2 3πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ 𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’ πœ‹ 2 πœ€0 𝑖0 𝑖0
  • 4. Pure capacitive AC circuit πœ€ = πœ€0 sin πœ”π‘‘ 𝐢 𝑖 = 𝑖0 sin πœ”π‘‘ + πœ‹ 2 𝑖0 = πœ€0 1 πΆπœ” = πœ€0 𝑋𝐢 SI Unit : Ohm Ξ© 𝑋𝐢 = 1 πΆπœ” Capacitive reactance Phase difference πœ™ = πœ”π‘‘ + πœ‹ 2 βˆ’ πœ”π‘‘ = πœ‹ 2 Current leads potential by 90Β°
  • 5. Pure capacitive AC circuit Phasor diagram 𝑖0 𝑦 π‘₯ πœ€0 πœ”π‘‘ Wave diagram 𝑖 = 𝑖0 sin πœ”π‘‘ + πœ‹ 2 𝑑 𝑖, πœ€ 0 πœ‹ 2πœ‹ πœ‹ 2 3πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ πœ€0 𝑖0 𝑖0
  • 6. Simple AC circuits Element Current (emf:πœ€ = πœ€0 sin πœ”π‘‘) πœ™ 𝑋(Reactance) Resistor Inductor Capacitor πœ€0 𝑅 sin πœ”π‘‘ πœ€0 πœ”πΏ sin πœ”π‘‘ βˆ’ πœ‹ 2 πœ€0 ΰ΅— 1 πœ”πΆ sin πœ”π‘‘ + πœ‹ 2 0 βˆ’ πœ‹ 2 πœ‹ 2 𝑅 πœ”πΏ 1 πœ”πΆ
  • 7. Wave diagram 𝑑 𝑖, πœ€ 0 πœ‹ 2πœ‹ πœ‹ 2 3πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ 𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’ πœ‹ 2 πœ€0 𝑖0 𝑖0 0 β†’ πœ‹ 2 πœ‹ 2 β†’ πœ‹ πœ‹ β†’ 3πœ‹ 2 3πœ‹ 2 β†’ 2πœ‹ πœ€ = πœ€0 sin πœ”π‘‘ 𝑉𝐿 πœ€ increases from zero to maximum, current becomes zero. πœ€ decreases from maximum to zero, current grows to maximum. πœ€ increases from zero to negative maximum, current becomes zero. πœ€ decreases from negative maximum to zero, current grows to negative maximum. Current tries to follow path of voltage. The phase difference between them always remains to be 90Β°.
  • 8. 𝑑 𝑖, πœ€ 0 πœ‹ 2πœ‹ πœ‹ 2 3πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ 𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’ πœ‹ 2 πœ€0 𝑖0 𝑖0 𝑑 𝑖, πœ€ 0 πœ‹ 2πœ‹ πœ‹ 2 3πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ 𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’ πœ‹ 2 πœ€0 𝑖0 𝑖0 The lagging of current can be seen from the mechanical analogy as shown. Height represents the voltage and velocity of block is current. When height is maximum, velocity is zero and vice-versa.
  • 9. Wave diagram 𝑑 𝑖, πœ€ 0 πœ‹ 2πœ‹ πœ‹ 2 3πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ 𝑖 = 𝑖0 sin πœ”π‘‘ βˆ’ πœ‹ 2 πœ€0 𝑖0 𝑖0
  • 10. πœ€ = πœ€0 sin πœ”π‘‘ 𝐢 Wave diagram 𝑖 = 𝑖0 sin πœ”π‘‘ + πœ‹ 2 𝑑 𝑖, πœ€ 0 πœ‹ 2πœ‹ πœ‹ 2 3πœ‹ 2 πœ€ = πœ€0 sin πœ”π‘‘ πœ€0 𝑖0 𝑖0
  • 11. 𝑍 The relation b/w peak current and peak voltages can be written as Purely resistive circuit Purely inductive circuit 𝑖0 = E0 𝑍 𝑍 = 𝑅 𝑍 = πœ”πΏ 𝑍 is called impedance. Impedance is defined as the opposition any circuit shows when voltage is applied to it. SI unit is Ohm (Ξ©) Purely capacitive circuit 𝑍 = 1/πœ”πΆ
  • 12. βˆ’ | E0 sin πœ”π‘‘ 𝐢 𝑅 E0 2 = 𝑉𝑅 2 + 𝑉𝐢 2 E0 2 = 𝑖0 2 𝑅2 + 𝑖0 2 𝑋𝐢 2 𝑖0 2 𝑍2 = 𝑖0 2 𝑅2 + 𝑖0 2 𝑋𝐢 2 𝑍2 = 𝑅2 + 𝑋𝐢 2 𝑍 = 𝑅2 + 𝑋𝐢 2 𝑍 = 𝑅2 + 1/πœ”πΆ 2 𝑋𝐢 = 1/πœ”πΆ β‡’ 𝑉𝑅 πœ™ 𝑉𝐢 E0 𝑖0
  • 13. βˆ’ | 𝑍 = 𝑅2 + 1/πœ”πΆ 2 tan πœ™ = 𝑋𝐢 𝑅 πœ™ 𝑋𝐢 𝑅 𝑍 E0 sin πœ”π‘‘ 𝐢 𝑅 tan πœ™ = 1 πœ”πΆπ‘… 𝑍2 = 𝑅2 + 𝑋𝐢 2 𝑋𝐢 = 1 πœ”πΆ Peak current (𝑖0) is given by- 𝑖0 = E0 𝑍 = E0 𝑅2 + 1/πœ”πΆ 2 𝑉𝑅 πœ™ 𝑉𝐢 E0 𝑖0
  • 14. βˆ’ | 𝑍 = 𝑅2 + 1/πœ”πΆ 2 tan πœ™ = 1 πœ”πΆπ‘… 𝑖0 = E0 𝑍 = E0 𝑅2 + 1/πœ”πΆ 2 Steady state current (𝑖) in the circuit 𝑖 = E0 𝑍 sin(πœ”π‘‘ + πœ™) E0 sin πœ”π‘‘ 𝐢 𝑅 The current leads the emf by πœ™. 𝑉𝑅 πœ™ 𝑉𝐢 E0 𝑖0
  • 15. βˆ’ | E0 2 = 𝑉𝑅 2 + 𝑉𝐿 2 E0 2 = 𝑖0 2 𝑅2 + 𝑖0 2 𝑋𝐿 2 𝑖0 2 𝑍2 = 𝑖0 2 𝑅2 + 𝑖0 2 𝑋𝐿 2 𝑍2 = 𝑅2 + 𝑋𝐿 2 𝑍 = 𝑅2 + 𝑋𝐿 2 𝑍 = 𝑅2 + πœ”πΏ 2 𝑋𝐿 = πœ”πΏ β‡’ E0 sin πœ”π‘‘ 𝐿 𝑅 𝑉𝑅 πœ™ 𝑉𝐿 E0 𝑖0
  • 16. βˆ’ | tan πœ™ = 𝑋𝐿 𝑅 πœ™ 𝑋𝐿 𝑅 𝑍 tan πœ™ = πœ”πΏ 𝑅 𝑋𝐿 = πœ”πΏ Peak current (𝑖0) is given by- 𝑖0 = E0 𝑍 = E0 𝑅2 + πœ”πΏ 2 𝑍2 = 𝑅2 + 𝑋𝐿 2 𝑍 = 𝑅2 + πœ”πΏ 2 E0 sin πœ”π‘‘ 𝐿 𝑅 𝑉𝑅 πœ™ 𝑉𝐿 E0 𝑖0
  • 17. βˆ’ | tan πœ™ = πœ”πΏ 𝑅 Steady state current (𝑖) in the circuit 𝑖 = E0 𝑍 sin(πœ”π‘‘ βˆ’ πœ™) E0 sin πœ”π‘‘ 𝐿 𝑅 𝑉𝑅 πœ™ 𝑉𝐿 E0 𝑖0 𝑍 = 𝑅2 + πœ”πΏ 2 𝑖0 = E0 𝑍 = E0 𝑅2 + πœ”πΏ 2 The current lags the emf by πœ™.
  • 18. In the given circuit, find (a) inductive reactance 𝑋𝐿 . (b) impedance 𝑍. (c) Peak current 𝑖0. (d) i(t) πœ€ = 200 sin(100πœ‹π‘‘) 𝐿 = 2 πœ‹ 𝐻 𝑅 = 200 Ξ©
  • 19. πœ€ = 200 sin(100πœ‹π‘‘) 𝐿 = 2 πœ‹ 𝐻 𝑅 = 200 Ξ© (a) inductive reactance 𝑋𝐿 . 𝑋𝐿 = πœ”πΏ 𝑋𝐿 = 100πœ‹ Γ— 2 πœ‹ = 200 Ξ© πœ™ 𝑋𝐿 𝑅 𝑍 𝑍2 = 𝑅2 + 𝑋𝐿 2 𝑍 = 𝑅2 + 𝑋𝐿 2 ∴ 𝑍 = 200 2 Ξ© 𝑍 = (200)2+ 200 2 (b) impedance 𝑍.
  • 20. πœ€ = 200 sin(100πœ‹π‘‘) 𝐿 = 2 πœ‹ 𝐻 𝑅 = 200 Ξ© (c) Peak current 𝑖0. 𝑖0 = πœ€0 𝑍 πœ€0 = 200 𝑉 𝑖0 = 200 200 2 = 1 2 𝐴 𝑉𝑅 πœ™ 𝑉𝐿 Ξ΅0 𝑖0 πœ™ 𝑋𝐿 𝑅 𝑍 (d) i(t) 𝑖 𝑑 = 𝑖0 sin 100πœ‹π‘‘ βˆ’ πœ™ tan πœ™ = 𝑋𝐿 𝑅 = 200 200 = 1 β‡’ πœ™ = πœ‹ 4 ∴ 𝑖 𝑑 = 1 2 sin 100πœ‹π‘‘ βˆ’ πœ‹ 4