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Chapter-3: AC Circuits
 Alternating Current (AC)
 LCR circuit
 Resonance Frequency
Alternating Current (AC)
• Alternating current (AC): current that changes its magnitude
and direction periodically.
Alternating Current (AC)-Current (I)at time (t)
The current at time (t) in AC circuit can be found by the equation:
𝐼 = 𝐼𝑚𝑎𝑥 sin 2𝜋𝑓𝑡 = 𝐼𝑚𝑎𝑥 sin⁡
(𝜔𝑡)1
I: Current at time t (Ampere)
Imax: Maximum value of current (Ampere)
f: Frequency (number of cycles per second) (Hertz)
t: Time (Second)
ω: Angular frequency (rad/second)
1: use radian mode in calculations
Alternating Current (AC)-Potential Difference (ΔV) at time(t)
∆𝑉 = ∆𝑉
𝑚𝑎𝑥 sin 2𝜋𝑓𝑡 + 𝜑 = ∆𝑉
𝑚𝑎𝑥 sin⁡
(𝜔𝑡 + 𝜑)1
ΔV: Potential difference at time t (Volt)
Imax: maximum value of potential difference (Volt)
f: Frequency (number of cycles per second) (Hertz)
t: Time (Second)
ω: Angular frequency (rad/second)
φ: Phase difference (radian)2
1: use radian mode in calculations
2:Phase difference will be explained in more details in LCR circuit
Alternating Current (AC)-Potential Difference (ΔV) at time(t)
Alternating Current (AC)-Ohms Law
When an AC source is connected to passive components, ohm’s law can apply as:
∆𝑉 = 𝐼𝑧 , ∆𝑉
𝑚𝑎𝑥 = 𝐼𝑚𝑎𝑥 𝑧
z: Impedance (Ohm)
Impedance is the total current hindrance offered by the passive components in the circuit.
LCR Circuit
• LCR circuit: a circuit in which a resistor , capacitor and an inductor
are connected in series with an AC power supply.
• The current in the circuit is the same at any point.
• The total potential difference in LCR circuit is:
∆𝑉 = ∆𝑉
𝑚𝑎𝑥sin 𝜔𝑡 + 𝜑
unit of ϕ is radian
𝐼 = 𝐼𝑚𝑎𝑥 sin⁡
(𝜔𝑡)
LCR Circuit
• The impedance of the LCR circuit is:
𝑧 = 𝑅2 + 𝑋𝐿 − 𝑋𝐶
2
• The phase difference between current and voltage in LCR
circuit can also be found by:
• 𝑡𝑎𝑛𝜑 =
𝑋𝐿−𝑋𝐶
𝑅
LCR Circuit
Problem (1)
2.
3.
4.
LCR Circuit
-Resonance frequency
• if the frequency of an AC source of an LCR circuit
was increased the current increases till it reaches a
maximum value. Then if the frequency was
increase more, the current starts to drop.
• At that particular frequency where the current
peaks, the circuit is said to operate at resonance
frequency (fr).
• Note the following point when a circuit is operating
at resonance frequency is:
 XL =XC.
 z=R, which is minimum value of impedance.
 current is at maximum value.
LCR Circuit
-Resonance frequency
What happed when LCR circuit is
operating at resonance frequency?
LCR Circuit
-Resonance frequency
• The resonance frequency of a particular LCR circuit depends
only on the inductance (L) and capacitance (C) in the circuit.
𝑓𝑟 =
1
2𝜋 𝐿𝐶
fr: Resonance frequency (Hertz)
L: Inductance (Henry)
C: Capacitance (farad)
LCR Circuit
-Resonance frequency
5.
6.
7.
8.
9.
Multiple Choice Questions
Chapter-3 new format LCR pptx. Explains the L,C and R in an AC Circuit
Chapter-3 new format LCR pptx. Explains the L,C and R in an AC Circuit
Chapter-3 new format LCR pptx. Explains the L,C and R in an AC Circuit
Chapter-3 new format LCR pptx. Explains the L,C and R in an AC Circuit

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Chapter-3 new format LCR pptx. Explains the L,C and R in an AC Circuit

  • 1. Chapter-3: AC Circuits  Alternating Current (AC)  LCR circuit  Resonance Frequency
  • 2. Alternating Current (AC) • Alternating current (AC): current that changes its magnitude and direction periodically.
  • 3. Alternating Current (AC)-Current (I)at time (t) The current at time (t) in AC circuit can be found by the equation: 𝐼 = 𝐼𝑚𝑎𝑥 sin 2𝜋𝑓𝑡 = 𝐼𝑚𝑎𝑥 sin⁡ (𝜔𝑡)1 I: Current at time t (Ampere) Imax: Maximum value of current (Ampere) f: Frequency (number of cycles per second) (Hertz) t: Time (Second) ω: Angular frequency (rad/second) 1: use radian mode in calculations
  • 4. Alternating Current (AC)-Potential Difference (ΔV) at time(t) ∆𝑉 = ∆𝑉 𝑚𝑎𝑥 sin 2𝜋𝑓𝑡 + 𝜑 = ∆𝑉 𝑚𝑎𝑥 sin⁡ (𝜔𝑡 + 𝜑)1 ΔV: Potential difference at time t (Volt) Imax: maximum value of potential difference (Volt) f: Frequency (number of cycles per second) (Hertz) t: Time (Second) ω: Angular frequency (rad/second) φ: Phase difference (radian)2 1: use radian mode in calculations 2:Phase difference will be explained in more details in LCR circuit
  • 5. Alternating Current (AC)-Potential Difference (ΔV) at time(t)
  • 6. Alternating Current (AC)-Ohms Law When an AC source is connected to passive components, ohm’s law can apply as: ∆𝑉 = 𝐼𝑧 , ∆𝑉 𝑚𝑎𝑥 = 𝐼𝑚𝑎𝑥 𝑧 z: Impedance (Ohm) Impedance is the total current hindrance offered by the passive components in the circuit.
  • 7.
  • 8. LCR Circuit • LCR circuit: a circuit in which a resistor , capacitor and an inductor are connected in series with an AC power supply. • The current in the circuit is the same at any point. • The total potential difference in LCR circuit is: ∆𝑉 = ∆𝑉 𝑚𝑎𝑥sin 𝜔𝑡 + 𝜑 unit of ϕ is radian 𝐼 = 𝐼𝑚𝑎𝑥 sin⁡ (𝜔𝑡)
  • 9. LCR Circuit • The impedance of the LCR circuit is: 𝑧 = 𝑅2 + 𝑋𝐿 − 𝑋𝐶 2 • The phase difference between current and voltage in LCR circuit can also be found by: • 𝑡𝑎𝑛𝜑 = 𝑋𝐿−𝑋𝐶 𝑅
  • 11.
  • 13. 2.
  • 14. 3.
  • 15. 4.
  • 16. LCR Circuit -Resonance frequency • if the frequency of an AC source of an LCR circuit was increased the current increases till it reaches a maximum value. Then if the frequency was increase more, the current starts to drop. • At that particular frequency where the current peaks, the circuit is said to operate at resonance frequency (fr). • Note the following point when a circuit is operating at resonance frequency is:  XL =XC.  z=R, which is minimum value of impedance.  current is at maximum value.
  • 17. LCR Circuit -Resonance frequency What happed when LCR circuit is operating at resonance frequency?
  • 18. LCR Circuit -Resonance frequency • The resonance frequency of a particular LCR circuit depends only on the inductance (L) and capacitance (C) in the circuit. 𝑓𝑟 = 1 2𝜋 𝐿𝐶 fr: Resonance frequency (Hertz) L: Inductance (Henry) C: Capacitance (farad)
  • 20. 5.
  • 21. 6.
  • 22. 7.
  • 23. 8.
  • 24. 9.