Resonance in LCR Circuit | Physics Class 12 - NEET PDF Download

Intelligence agencies and police officers are capable of tapping the communication and activities of anti-social elements. Have you ever wondered how is it done? It is done through the concept of 'resonance'. The idea of resonance is also used in TV channels for clarity: a particular frequency is assigned to a channel and when this frequency is received by the receiver, the current corresponding to this frequency becomes maximum. This helps in the maximum possible separation of channels, thus increasing their clarity.

In this document, we will study the resonance conditions of LCR circuits. 

Resonance in LCR Circuit

A series LCR circuit is said to be in the resonance condition when the current through it has its maximum value.

The current amplitude I₀ for a series LCR circuit is given by

I₀ becomes zero both for ω → 0 and ω → ∞. The value of I₀ is the maximum when

 or  ⇒

Then impedance will be the minimum

Z_min = R

The circuit is purely resistive. The current and voltage are in the same phase and the current in the circuit is maximum. This condition of the LCR circuit is called the resonance condition.

Resonance in LCR Circuit

The variance of I₀ v/s ω shown in the following figure

So cosϕ=  =  = 1

V = V₀ sin (ωt)

The impedance phase of the resonance circuit,

Impedance of the circuit is minimum and heat generated in the circuit is maximum.

Q1. In the following LCR circuit find Z, i(t), V_OC, and V_OL at the resonance frequency

Solution:

 Z = Z_min = R = 2?

V_{O L} = i₀X_C = 100 volt

V_{O L} = i₀ X_L = 100 volt

Note: 

The above circuit is used as a voltage amplifier (magnification) as the peak value of voltage by the source is only 10 while we can have maximum voltage up to 100 (V_{O C}& V_{O L})

Q2. A series LCR with R = 20 ?, L = 1.5 H, and C = 35 μF is connected to a variable frequency 200 V a.c. supply. When the frequency of the supply equals the natural frequency of the circuit. What is the average power transferred to the circuit in one complete cycle?

Solution:

When the frequency of the supply equals the natural frequency of the circuit, resonance occurs.

Therefore, Z = R = 20 ohm

i_rms =

Average power transferred/cycle

P = E_rmsi_rms cos0° = 200 × 10 × 1 = 2000 watt

Sharpness of Resonance (Q - factor) 

The Q-factor of a series resonant circuit is defined as the ratio of the resonant frequency to the difference in two frequencies taken on both sides of the resonant frequency such that at each frequency, the current amplitude becomes times the value of the resonant frequency.

Mathematically Q-factor:

or 

Choke Coil 

A choke coil is simply an inductor with large inductance which is used to reduce current in a.c. circuit without much loss of energy.

Principle: A choke coil is based upon the principle that when a.c. flows through an inductor, the current lags behind the e.m.f. by a phase angle π/2.

Construction: A choke coil is an inductance. It consists of a large number of turns of insulated copper wire wound over a soft iron core. To minimize loss of electrical energy due to the production of eddy currents, a laminated iron core is used.

In practice, a low-frequency choke coil is made of insulated copper wire wound on a soft iron core, while a high-frequency choke coil has air as core materials

Working: As shown in the figure, a choke is put in series across an electrical appliance of resistance R and is connected to an a.c. source.

The average power dissipated per cycle in the circuit is

P_av = V_eff I_eff cosϕ = V_eff I_eff  .

Inductance L of the choke coil is very large so that R << wL. Then

Power factor cosϕ ≌    0  

tanϕ =

Uses: In a.c. circuit, a choke coil is used to control the current in place of a resistance. If a resistance is used to control the current, the electrical energy will be wasted in the form of heat. A choke coil decreases the current without wasting electrical energy in the form of heat.

Oscillations in LC Circuits

If a charged capacitor C is short-circuited through an inductor L, the charge and current in the circuit start oscillating simply harmonically. If the resistance of the circuit is zero, no energy is dissipated as heat. Assume an ideal situation in which energy is not radiated away from the circuit. With these idealizations resistance and no radiation, the oscillations in the circuit persist indefinitely and the energy is transferred from the capacitor's electric field to the inductor's magnetic field back and forth. The total energy associated with the circuit is constant. This is analogous to the transfer of energy in an oscillating mechanical system from potential energy to kinetic energy and back, with constant total energy. Such an analogous mechanical system is an example of spring-mass system.

Let us now derive an equation for the oscillations of charge and current in an L-C circuit. 

Refer to figure (a): The capacitor is charged to a potential difference V such that charge on capacitor q₀ = CV

Here q₀ is the maximum charge on the capacitor. At time t = 0, it is connected to an inductor through a switch S. At time t = 0, the switch S is closed.

Refer to figure (b): When the switch is closed, the capacitor starts discharging. Let at time t charge on the capacitor is q (<q₀) and since, it is further decreasing, there is a current i in the circuit in the direction shown in the figure.

The potential difference across capacitor = potential difference across inductor, or

V_b - V_a = V_c - V_d

Therefore,  Now, as the charge is decreasing, i =

or  = -

Substituting in equation (1), we get

or  = -  

This is the standard equation of simple harmonic motion

Here w =  

The general solution of equation, is

q = q₀ cos (ωt ± ϕ) 

In our case ϕ = 0 as q = q₀ at t = 0.

Thus, we can say that the charge in the circuit oscillates with angular frequency ω given by equation (3). Thus,

ln L-C oscillations, q, i and  all oscillate simply harmonically with the same angular frequency ω, but the phase difference between q and i or between i and  is that their amplitudes are q₀ q₀ω is ω² q₀ respectively. So,

q = q₀ cosωt 

i = - = q₀ω sin ωt 

and cosωt 

Potential energy in the capacitor

U_C =  =  

The potential energy in the inductor

U_L =  =  

Thus potential energy stored in the capacitor and that in the inductor also oscillates between maximum value and zero with double the frequency. All these quantities are shown in the figures that follow

Q3. A capacitor of capacitance 25 μF is charged to 300 V. It is then connected across a 10 μH inductor. The resistance of the circuit is negligible.

(a) Find the frequency of oscillation of the circuit.

(b) Find the potential difference across the capacitor and magnitude of circuit current 1.2 ms after the inductor and capacitor are connected.

(c) Find the magnetic energy and electric energy at t = 0 and t = 1.2 ms.

Solution:

(a) The frequency of oscillation of the circuit is,

f =

Substituting the given values we have,  =

(b) Charge across the capacitor at time t will be,

q = q₀ cos ωt

and i = - q₀ ωsin ωt

Here q₀ = CV₀ = (25 × 10^-6) (300) = 7.5 × 10^-3 C

Now, charge is the capacitor after t = 1.2 × 10^-3 s is,

q = (7.5 × 10^-3) cos (2p × 318.3) (1.2 × 10^-3)C

= 5.53 × 10^-3C

Therefore, P.D. across capacitors,

V =  = 221.2 volt

The magnitude of current in the circuit at

t = 1.2 × 10^-3 s is,

|i| = q₀ ω sinωt

= (7.5 × 10^-3) (2p) (318.3) sin(2p × 318.3) (1.2 × 10^-3) A = 10.13 A

(c) At t = 0: The current in the circuit is zero. Hence,U_L = 0

Charge on the capacitor is the maximum.

Hence, U_c =

or U_c =  = 1.125 J

Therefore, Total energy E = U_L + U_C = 1.125 J

At t = 1.2 ms

U_L =  = (10.13)² = 0.513 J

U_C = E - U_L = 1.125 - 0.513 = 0.612 J

Otherwise, U_C can be calculated as,

U_C =  =  = 0.612 J