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In this Physics tutorial, you will learn:

- What is a RLC circuit?
- Why oscillations in a RLC circuit are damped?
- What is the equation of oscillations in a RLC circuit?
- What is angular frequency of damped oscillations? How does it differ from the angular frequency of undamped oscillations?
- How to find the energy in a damped RLC circuits at any instant?
- What are forced oscillations? What do they cause in an electric circuit?
- How to calculate the AC current and emf caused by forced oscillations in a circuit at any instant?
- What is resistive/capacitive/inductive load?
- How to cope with AC circuits containing a single resistor/capacitor/inductor?
- What are phasor diagrams? Why do we use them?

x(t) = A_{0} ∙ e^(-γ ∙ t) cos〖(ω ∙ t+φ)〗

On the other hand, in sustainable SHM, the amplitude of oscillations does not change with time. The envelope shows a horizontal function of the type x(t) = A0." In the next paragraph, we will see that a RLC circuit without a sustainable energy supply from outside, represents a system of damped oscillations because the energy of system decreases with time. This occurs because part of the total energy of the system converts into thermal energy and is therefore dissipated in the form of heat from the resistor to the environment. This brings a continuous decrease in the total energy of the system. Equation of the Damped Oscillations in a RLC Circuit In the previous tutorial, we have explained that the total electromagnetic energy in a LC circuit is W_tot = W_m+W_e = (L ∙ i^{2})/2+Q^{2}/2C

When a resistor is added in this circuit, the total electromagnetic energy will decrease at a rate of (dW_tot)/dt = -i^{2} ∙ R

because some of the energy in the system turns into thermal energy of resistor and is dissipated in the environment in the form of heat energy. The negative sign in the equation means that the total energy of the system decreases. Differentiating the above equation with time, we obtain (dW_tot)/dt = L ∙ i ∙ di/dt+Q/C ∙ dQ/dt = -i^{2} ∙ R

Since i = dQ/dt, and di/dt = d2Q/dt2 we obtain L ∙ dQ/dt ∙ (d^{2} Q)/(dt^{2} )+Q/C ∙ dQ/dt = -R ∙ (dQ/dt)^{2} L ∙ dQ/dt ∙ (d^{2} Q)/(dt^{2} )+R ∙ (dQ/dt)^{2}+Q/C ∙ dQ/dt = 0

Simplifying both sides of the last equation by dQ/dt, we obtain L ∙ (d^{2} Q)/(dt^{2} )+R ∙ dQ/dt+1/C ∙ Q = 0

This is the differential equation for the damped oscillations in a RLC circuit. The charge decay in such a circuit is calculated through an expression, which is a combination of exponential and sinusoidal equation, as occurs in all types of damped oscillations. Thus, the charge left in a RLC circuit after a given time t of operation is found by: Q(t) = Q_{0} ∙ e^(-(R ∙ t)/2L) ∙ cos(ω^' ∙ t+φ)

where ω^' = √(ω^{2}-(R/2L)^{2} )

is the angular frequency of damped oscillations and ω = 1/√(L ∙ C)

is the angular frequency of undamped oscillations. In addition, you can see that the amplitude also contains an exponential decaying term e^(-(R ∙ t)/2L). This means the amplitude of every successive oscillation is smaller than the previous one as the power of Euler's Number e here is negative. Example: The potential difference between the plates of a 5μF capacitor connected in an alternating 50Hz RLC circuit shown in the figure is 20V and the resistance of resistor in the circuit has a value of 0.25Ω. Calculate: a) The initial charge stored in the capacitor b) The charge stored in the circuit 0.4 s after the switch turns on Take the initial phase as zero. Solution a) The initial charge stored in the capacitor is Q_{0} = C ∙ ∆V = (5 × 10^{-6} F) ∙ (20V) = 10^{-4} C

b) First we must find the inductance and then calculate the charge stored in the circuit at the given time. Thus, since the circuit has a frequency of 50Hz, we have ω = 2π ∙ f = 2π ∙ 50Hz = 100π rad/s

Hence, giving that ω = 1/√(L ∙ C)

or ω^{2} = 1/LC

we obtain for the inductance L of the inductor: L = 1/(ω^{2} ∙ C) = 1/((100π)^{2} ∙ (10^{-4} ) ) = 1/(10^{4} ∙ π^{2} ∙ 10^{-4} ) = 1/π^{2} = 1/(3.14)^{2} = 0.1 H

The charge stored in the capacitor after 20s therefore is Q(t) = Q_{0} ∙ e^(-(R ∙ t)/2L) ∙ cos(ω^' ∙ t+φ) Q(t) = Q_{0} ∙ e^(-(R ∙ t)/2L) ∙ cos(√(ω^{2}-(R/2L)^{2} ) ∙ t) Q(20) = (10^{-4} ) ∙ e^(-(0.25 ∙ 0.4)/(2 ∙ 0.1)) ∙ cos(√((100π)^{2}-(0.25/(2 ∙ 0.1))^{2} ) ∙ 0.4) Q(20) = (10^{-4} ) ∙ e^{-5} ∙ cos(√((100π)^{2}-(1.2)^{2} ) ∙ 0.4) = (10^{-4} ) ∙ e^{-5} ∙ cos(100π ∙ 0.4) = (10^{-4} ) ∙ e^{-5} ∙ cos(40π) = (10^{-4} ) ∙ e^{-5} ∙ 1 = 10^{-4} ∙ 6.7 × 10^{-2} = 6.7 × 10^{-6} C

From the above results, we draw the following conclusions: 1- For small values of resistance, ω' ≈ ω, so we can neglect the (R/2L)2 factor and focus only on the value of ω. 2- In absence of an external source, the charge in the circuits drops very fast (in only 0.4 s it has dropped about 15 times, from 10-4C to 6.7 × 10-6 C). This means that if the emf source is not active, the RLC circuit discharges almost immediately due to the electromagnetic-to-heat energy conversion, which takes place in the resistor. We can use a similar approach when calculating the energy decay in a RLC circuit operating without an external energy supply. For this, we observe what happens to the electric energy in the capacitor. Since W_e = Q^{2}/2C

we can write this expression as a function of time, i.e. W_e (t) = [Q(t)]^{2}/2C = [Q_{0} ∙ e^(-(R ∙ t)/2L) ∙ cos(ω^' ∙ t+φ) ]^{2}/2C = (Q_{0}^{2})/2C ∙ e^(-(R ∙ t)/L) ∙ cos^{2}(ω^' ∙ t+φ)

This means the energy of the electric field in a RLC circuit oscillates in a cos2 fashion while the amplitude decreases exponentially with time. Example: A 50Hz RLC circuit contains a 10Ω resistor, a 0.4H inductor and a 2nF capacitor connected in series. The capacitor initially stores a charge of 5μC. Calculate: a) The initial electric energy stored in the capacitor plates b) The energy left in the capacitor plates 2 s after the switch turns OFF. Take the initial phase equal to zero. Solution Clues: R = 10 Ω L = 0.4 H C = 2nF = 2 × 10-9 F Q0 = 5μC = 5 × 10-6 C f = 50 Hz a) We initial = ? b) W(2) = ? a) The initial electric energy stored in the capacitor plates is W_(e (initial) ) = (Q_{0}^{2})/2C = (5 × 10^{-6} C)^{2}/(2 ∙ (2 × 10^{-9} F) ) = 6.25 × 10^{-3} J

b) The energy left in the capacitor plates after 2 s of supply interruption is W_e (t) = (Q_{0}^{2})/2C ∙ e^(-(R ∙ t)/L) ∙ cos^{2}(ω^' ∙ t+φ) W_e (t) = (Q_{0}^{2})/2C ∙ e^(-(R ∙ t)/L) ∙ cos^{2}(├ √(ω^{2}-(R/2L)^{2} ) ∙ t┤) W_e (2) = (6.25 × 10^{-3} J) ∙ e^(-(10 ∙ 2)/0.4) ∙ cos^{2}(├ √((2 ∙ π ∙ 50)^{2}-(10/(2 ∙ 0.4))^{2} ) ∙ 2┤) = (6.25 × 10^{-3} J) ∙ e^(-50) ∙ cos^{2}(├ √(98596-156.25) ∙ 2┤) = (6.25 × 10^{-3} J) ∙ e^(-50) ∙ cos^{2}(├ √98439.75 ∙ 2┤) = (6.25 × 10^{-3} J) ∙ e^(-50) ∙ cos^{2}(├ 627.5 rad┤) (6.25 × 10^{-3} J) ∙ (〖1.93 × 10〗^(-22) ) ∙ (0.6833)^{2} = 5.63 × 10^(-25) J

This value is very small, close to zero. Hence, we say the flow of energy through a RLC circuit, practically stops immediately after the switch turns off. Again, here you can see how necessary a sustainable external source such as a battery or an AC power supply is, in order to maintain constant the electricity flow through a RLC circuit. Forced Oscillations. Alternating Current and Emf in a RLC Circuit caused by Forced Oscillations As stated in the previous paragraph, a RLC circuit needs an external sustainable source of emf to make it operate for a long time at steady values. This is made possible by connecting the circuit to an AC power supply, which on the other hand is supplied by an AC generator. An AC generator consists on a current-carrying loop placed inside an external magnetic field, as discussed in the tutorial 16.3 "Magnetic Force on a Current-Carrying Wire. Ampere's Force." Such a system produces forced oscillations in the circuit, which makes it operate for a long time with constant periodic values. A simplified version of an AC generator is shown in the figure below. A conducting loop is placed inside an external magnetic field. The slip rings are used to create the contact with multiple coils. Each ring is connected to one end of the loop and to the rest of the circuit through metal brushes. As a result, the rings slip against the metal brush and are free to rotate. This brings an induced current i in the circuit. As the conducting loop of the generator is forced to rotate in the external magnetic field B, an emf is induced in the loop. The equation of this induced emf is ε(t) = ε_max ∙ sin〖ω_{d} ∙ t〗

where εmax is the amplitude of the induced emf in the generator (usually the amplitude is the initial induced emf), while ωd is called the "driving angular frequency" because it drives an induced current in the circuit, the equation of which is given by i(t) = i_max ∙ sin(ω_{d} ∙ t-φ)

where imax is the amplitude of the driven current in the circuit. The induced current may not be in phase with the induced emf, so the inclusion in the formula of the initial phase φ is necessary. In addition, we may express the driven angular frequency as ω_{d} = 2π ∙ f_{d}

where fd is the driven frequency of the induced current. Thus, in circuits with no or very small resistance, the induced current (and emf) oscillate at angular frequency ω = 1/√(L ∙ C)

which is known as the "natural angular frequency". Such oscillations are known as free oscillations. On the other hand, when a resistor is present is the circuit, the oscillations are known as damped (when no external source is present) or forced (when an external source is needed to keep the values of the induced current and emf constant). The following rule is true for the forced oscillations: "The induced current and emf in a circuit always occur according the angular frequency of the forced oscillations, regardless the value of the natural angular frequency." Resistive, Inductive and Capacitive Load To make the understanding of a RLC circuit more digestible, we will discuss separately three simple circuits, each of them containing only an external emf and one of the three circuit components: resistor, capacitor or inductor, which produce a load in the circuit. Let's start with the circuit that produces the resistive load. a) Resistive Load Let's consider a circuit containing only an alternating emf source and a resistor as shown in the figure. From the Law of Energy Conservation, we have ε-∆V_R = 0

where ΔVR is the potential difference across the resistor. We can write this equation as ∆V_R (t) = ε_max ∙ sin〖ω_{d} ∙ t〗

When neglecting the resistance of conducting wire, we obtain i_R (t) = (ε(t))/R = ε_max/R ∙ sin〖ω_{d} ∙ t〗

Moreover, we have for the current in the circuit: i_R (t) = i(t) = i_max ∙ sin〖〖(ω〗_{d} ∙ t-φ)〗

Giving that in this type of circuit the current is in phase with the potential difference, we have φ = 0. The graph below shows one cycle of induced current and potential difference in an AC circuit containing a resistive load: To make the graph plotting easier, we use arrows similar to vectors even though neither current nor voltage are vectors. Such diagrams are known as phasor diagrams. The angle formed by the arrows and the horizontal (time) axis gives the ωt term. A phasor diagram pertaining the above graph is shown below: Example: The voltage of an AC generator is given by the equation ΔV(t) = 90 sin ωt and the frequency of generator is 60 Hz. Calculate: a) The maximum current produced by the generator if it is connected to a 30 Ω resistor b) The potential difference in the circuit at t = 2.504 s. Solution a) From the equation of voltage, we notice than the maximum voltage (potential difference) in the circuit is 90 V. In addition, we obtain for the maximum current flowing through the circuit: i_max = (∆V_max)/R = (90 V)/(30 Ω) = 3A

b) The potential difference at t = 2.504 s (giving that ω = 2πf and f = 60 Hz), is ΔV(2.504) = 90 ∙ sin(2π ∙ 60 ∙ 2.504) = 90 ∙ sin(2π ∙ 60 ∙ 2.504) = 90 ∙ sin300.48π = 90 ∙ sin0.48π = 90V ∙ 0.998 = 89.82 V

b) Capacitive Load Now, let's consider a circuit supplied by an AC source, which contains only a capacitor C as shown in the figure. Using a similar approach as we did when dealing with the resistive load, we obtain for the potential difference at any instant across the capacitor: ∆V_{c} (t) = 〖∆V〗_(C(max)) ∙ sin〖ω_{d} ∙ t〗

From the definition of capacitance, we have for the charge stored in the capacitor at any instant t: Q_{c} (t) = C ∙ ∆V_{c} (t) = C ∙ 〖∆V〗_(C(max)) ∙ sin〖ω_{d} ∙ t〗

and for the current at any instant t: i_{c} (t) = (dQ_{c})/dt = 〖ω_{d} ∙ ∆V〗_(C(max)) ∙ cos〖ω_{d} ∙ t〗

The quantity X_{c} = 1/(ω_{d} ∙ C)

is called capacitive reactance of capacitor. It has the unit of resistance (Ohm). From experiments, it results that current leads by one quarter of a cycle the voltage in such a circuit. If we replace the cos ωd ∙ t term with a phase-shifted sine expression of +π/2 rad, we obtain cos〖ω_{d} ∙ t〗 = sin(ω_{d} ∙ t+π/2)

Hence, we obtain for the current in the circuit: i_{c} (t) = 〖∆V〗_(C(max))/X_{c} ∙ sin(ω_{d} ∙ t+π/2)

In addition, we have for the maximum potential difference in the circuit 〖∆V〗_(C(max)) = i_(C(max)) ∙ X_{c}

Since there is a shift in phase by one quarter of a period (π/2 = 2π/4 = T/4), the graphs of potential difference and current versus time for one complete cycle are: The corresponding phasor diagram for this circuit is The current is π/2 (a quarter of a cycle) in advantage to potential difference. Therefore, we say: "the current leads the voltage by π/2". Remark! The capacitive reactance behaves as an AC resistance. As the frequency of current approaches zero, the capacitive reactance raises to infinity and as a result, the circuit behaves as a DC circuit. However, the current flow in this way (in one direction only) is prevented from the high resistance between the plates of capacitor (at the gap between the plates), which does not allow the current to flow between the plates and to close therefore the cycle. Example: A circuit containing a 60 Hz AC power source that oscillates according the equation ΔVC(t) = 50 ∙ sin ωd ∙ t and a 20 μF capacitor as shown in the figure. Calculate: a) The capacitive reactance in the circuit b) The maximum current flowing in the circuit c) The value of voltage and current in the circuit at t = 1.406 s. Solution a) From the clues, it is clear that ΔVC(max) = 50 V, C = 20μF = 2 × 10-5 F and f = 60 Hz. Thus, for capacitive reactance, we have X_{c} = 1/(ω_{d} ∙ C) = 1/(2π ∙ f ∙ C) = 1/(2 ∙ 3.14 ∙ (60 Hz) ∙ (2 × 10^{-5} F) ) = 132.7Ω

b) The maximum current flowing through the circuit is given by 〖∆V〗_(C(max)) = i_(C(max)) ∙ X_{c}

Thus, i_{c}(max) = 〖∆V〗_{c}(max) /X_{c} = (50 V)/132.7Ω = 0.38 A

c) The value of voltage in the circuit at t = 1.406 s is ∆V_{c} (t) = 〖∆V〗_(C(max)) ∙ sin〖ω_{d} ∙ t〗 ∆V_{c} (1.406) = 50 ∙ sin(2π ∙ 60 ∙ 1.406) = 50 ∙ sin(168.72π) = 50 ∙ sin(0.72π) = 50V ∙ 0.77 = 38.5 V

As for the current at t = 1.406 s, we have i_{c} (t) = i_(C(max)) ∙ sin(ω_{d} ∙ t+π/2) i_{c} (1.406) = 0.38 ∙ sin(168.72π+π/2) = 0.38 ∙ sin(169.22π) = 0.38 ∙ sin(1.22π) = 0.38A ∙ (-0.64) = -0.24 A

The negative sign shows direction; it means the current actually is flowing in the opposite direction to the initial current at t = 0. c) Inductive Load The reasoning is the same even when we have a circuit in which there is only an AC source and an inductor as shown in the figure. The potential difference across the inductor is ∆V_L (t) = ∆V_(L(max)) ∙ sin〖ω_{d} ∙ t〗

From Faraday's Law, we have ∆V_L = L (di_L)/dt

Thus, combining the above equations, we obtain (di_L)/dt = (∆V_L)/L = (∆V_(L(max)))/L ∙ sin〖ω_{d} ∙ t〗

Or di_L = (∆V_(L(max)))/L ∙ sin(ω_{d} ∙ t)dt

The current flowing at any instant in the circuit is obtained through integration techniques. Thus, i_L (t) = ∫▒〖di_L 〗 = (∆V_(L(max)))/L ∙ ∫▒〖sin(ω_{d} ∙ t)dt〗 = (∆V_(L(max)))/L ∙ (-1/ω_{d} ) ∙ cos(ω_{d} ∙ t) = -((∆V_(L(max)))/(ω_{d} ∙ L)) ∙ cos(ω_{d} ∙ t)

The quantity X_L = ω_{d} ∙ L

is called inductive reactance and is measured in Ohms, similarly to capacitive reactance discussed in the previous paragraph. Using the trigonometric identity -cos(ω_{d} ∙ t) = sin(ω_{d} ∙ t-π/2)

we obtain for the current flowing in a circuit containing an inductive load: i_L (t) = ((∆V_(L(max)))/(ω_{d} ∙ L)) ∙ sin(ω_{d} ∙ t-π/2)

From this equation, we can see that for a purely inductive load, the current is delayed (is out of phase) by π/2 (a quarter of a cycle) to the potential difference. Therefore, we obtain the graph below: Again, we use the phasor concept to simplify the understanding of the above graph. The phasor diagram that corresponds the above graph is shown below: Example: A 0.2 H inductor is connected to an AC source of voltage ΔVC(t) = 40 ∙ sin(100 π ∙ t). a) Calculate the inductive reactance of the circuit b) Write the equation of current in the circuit as a function of time c) Calculate the current and voltage in the circuit at t = 4.961 s. Solution a) From the clues, we have ΔVL(max) = 40 V and L = 0.2 H. In addition, we have ω_{d} = 2πf = 100π

so, f = 50 Hz. The inductive reactance in the circuit is X_L = ω_{d} ∙ L = 100π ∙ 0.2 = 20π Ω = 20 ∙ 3.14 Ω = 62.8 Ω

b) Since the inductive reactance is like a resistance in the circuit, we obtain for the maximum current flowing through the circuit (applying the Ohm's Law): i_(L(max)) = (ΔV_(L(max)))/X_L = 40V/62.8Ω = 0.64A

Therefore, the equation of current in the circuit is i_L (t) = ((∆V_(L(max)))/(ω_{d} ∙ L)) ∙ sin(ω_{d} ∙ t-π/2) = 40/(100π ∙ 0.2) ∙ sin(100π ∙ t-π/2) = 2/π ∙ sin(100π ∙ t-π/2) = 0.64 ∙ sin(100π ∙ t-π/2)

c) The current at t = 4.961s is i_L (4.961) = 0.64 ∙ sin(100π ∙ 4.961-π/2) = 0.64 ∙ sin(100π ∙ 4.961-π/2) = 0.64 ∙ sin(496.1π-π/2) = 0.64 ∙ sin(495.6π) = 0.64 ∙ sin(1.6π) = 0.64A ∙ (-0.95) = 0.61A

and the voltage in the circuit at t = 4.961s is ∆V_L (t) = ∆V_(L(max)) ∙ sin(ω_{d} ∙ t) ∆V_L (4.961) = ∆V_(L(max)) ∙ sin(ω_{d} ∙ t) = 40 ∙ sin(100π ∙ 4.961) = 40 ∙ sin(496.1π) = 40 ∙ sin(0.1π) = 40V ∙ 0.31 = 12.4V

Summary A RLC circuit is a circuit that contains at least a resistor, a capacitor and an inductor. The simplest RLC circuit is the series RLC circuit. The differential equation for the damped oscillations in a RLC circuit, is L ∙ (d^{2} Q)/(dt^{2} )+R ∙ dQ/dt+1/C ∙ Q = 0

The charge decay in such a circuit is calculated through an expression, which is a combination of exponential and sinusoidal equation, as occurs in all types of damped oscillations. Thus, the charge left in a RLC circuit after a given time t of operation is found by: Q(t) = Q_{0} ∙ e^(-(R ∙ t)/2L) ∙ cos(ω^' ∙ t+φ)

where ω^' = √(ω^{2}-(R/2L)^{2} )

is the angular frequency of damped oscillations and ω = 1/√(L ∙ C)

is the angular frequency of undamped oscillations. The equation for the energy decay in a damped oscillation system of electricity is W_e (t) = = (Q_{0}^{2})/2C ∙ e^(-(R ∙ t)/L) ∙ cos^{2}(ω^' ∙ t+φ)

This means the energy of the electric field in a RLC circuit oscillates in a cos2 fashion while the amplitude decreases exponentially with time. A RLC circuit needs an external sustainable source of emf to make it operate for a long time at steady values. This is made possible by connecting the circuit to an AC power supply, which on the other hand is supplied by an AC generator. Such a system produces forced oscillations in the circuit, which makes it operate for a long time with constant periodic values. The equation of this induced emf in an AC generator is ε(t) = ε_max ∙ sin〖ω_{d} ∙ t〗

where εmax is the amplitude of the induced emf in the generator (usually the amplitude is the initial induced emf), while ωd is called the "driving angular frequency" because it drives an induced current in the circuit, the equation of which is given by i(t) = i_max ∙ sin(ω_{d} ∙ t-φ)

in circuits with no or very small resistance, the induced current (and emf) oscillate at angular frequency ω = 1/√(L ∙ C)

which is known as the "natural angular frequency". Such oscillations are known as free oscillations. On the other hand, when a resistor is present is the circuit, the oscillations are known as damped (when no external source is present) or forced (when an external source is needed to keep the values of the induced current and emf constant). The following rule is true for the forced oscillations: "The induced current and emf in a circuit always occur according the angular frequency of the forced oscillations, regardless the value of the natural angular frequency." The resistive load as a function of time in a circuit containing only an AC power source and a resistor is ∆V_R (t) = ε_max ∙ sin〖ω_{d} ∙ t〗

and the current in this circuit as a function of time is i_R (t) = i(t) = i_max ∙ sin〖〖(ω〗_{d} ∙ t-φ)〗

Giving that in this type of circuit the current is in phase with the potential difference, we have the initial phase φ = 0. When considering a circuit supplied by an AC source, which contains only a capacitor C, we have for the potential difference at any instant across the capacitor: ∆V_{c} (t) = 〖∆V〗_(C(max)) ∙ sin〖ω_{d} ∙ t〗

and for the current at any instant t: i_{c} (t) = (dQ_{c})/dt = 〖ω_{d} ∙ ∆V〗_(C(max)) ∙ cos〖ω_{d} ∙ t〗

The quantity X_{c} = 1/(ω_{d} ∙ C)

is called capacitive reactance of capacitor. It has the unit of resistance (Ohm). From experiments, it results that current leads by one quarter of a cycle the voltage in such a circuit. If we replace the cos ωd ∙ t term with a phase-shifted sine expression of +π/2 rad, we obtain cos〖ω_{d} ∙ t〗 = sin(ω_{d} ∙ t+π/2)

Hence, we obtain for the current in the circuit: i_{c} (t) = 〖∆V〗_(C(max))/X_{c} ∙ sin(ω_{d} ∙ t+π/2)

In addition, we have for the maximum potential difference in the circuit 〖∆V〗_(C(max)) = i_(C(max)) ∙ X_{c}

The current is π/2 (a quarter of a cycle) in advantage to potential difference. Therefore, we say: "the current leads the voltage by π/2". Similarly, in a circuit containing only an AC power source and an inductor, the potential difference across the inductor is ∆V_L (t) = ∆V_(L(max)) ∙ sin(ω_{d} ∙ t) = -((∆V_(L(max)))/(ω_{d} ∙ L)) ∙ cos(ω_{d} ∙ t)

The quantity X_L = ω_{d} ∙ L

is called inductive reactance and is measured in Ohms, similarly to capacitive reactance. The current flowing in a circuit containing an inductive load is i_L (t) = ((∆V_(L(max)))/(ω_{d} ∙ L)) ∙ sin(ω_{d} ∙ t-π/2)

From this equation, we can see that for a purely inductive load, the current is delayed (is out of phase) by π/2 (a quarter of a cycle) to the potential difference. To make the graph plotting easier and its understanding more digestible, we use arrows similar to vectors even though neither current nor voltage are vectors. Such diagrams are known as phasor diagrams. The angle formed by the arrows and the horizontal (time) axis gives the ωt term. **1)** The initial potential difference between the plates of a 2μF capacitor connected in an alternating 60Hz RLC circuit shown in the figure is 12V and the resistance of resistor in the circuit has a value of 0.5Ω.

At a certain instant, the source is removed from the circuit. In such conditions, calculate the time elapsed until the maximum charge stored in the capacitor plates becomes half of the maximum charge stored in the plates before the source was removed from the circuit.

Take the initial phase as zero and ω' ≈ ω. Use a logarithmic approach and write the answer to the nearest whole number.

- 0s
- 1s
- 10s
- 11s

**Correct Answer: A**

**2)** The initial values of a RLC circuit operating at 60 Hz are shown in the figure. What is the energy stored in the capacitor plates 0.1 s after the power source is removed from the circuit? For simplicity, take ω' ≈ ω and φ = 0.

- 0.135 J
- 0.292 J
- 1.771 J
- 2.16 J

**Correct Answer: B**

**3)** In which of the circuits below the resistance is the lowest at the initial instant of circuits operation? Take the maximum current flowing through all circuits as 0.5A and the maximum voltage across every operating device as 12V. Consider any individual reactance as a resistance of the circuit itself. All circuits are operating at the same frequency f = 50 Hz.

- Circuit I
- Circuit II
- Circuit III
- Circuits II and III

**Correct Answer: A**

We hope you found this Physics tutorial "Introduction to RLC Circuits" useful. If you thought the guide useful, it would be great if you could spare the time to rate this tutorial and/or share on social media, this helps us identify popular tutorials and calculators and expand our free learning resources to support our users around the world have free access to expand their knowledge of physics and other disciplines. In our next tutorial, we expand your insight and knowledge of Magnetism with our Physics tutorial on The Series RLC Circuit .

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- Frequency Of Oscillations In A Lc Circuit Calculator
- Impedance Calculator
- Induced Emf As A Motional Emf Calculator
- Inductive Reactance Calculator
- Lorentz Force Calculator
- Magnetic Dipole Moment Calculator
- Magnetic Field At Centre Of A Current Carrying Loop Calculator
- Magnetic Field In Terms Of Electric Field Change Calculator
- Magnetic Field Inside A Long Stretched Current Carrying Wire Calculator
- Magnetic Field Inside A Solenoid Calculator
- Magnetic Field Inside A Toroid Calculator
- Magnetic Field Produced Around A Long Current Carrying Wire
- Magnetic Flux Calculator
- Magnetic Force Acting On A Moving Charge Inside A Uniform Magnetic Field Calculator
- Magnetic Force Between Two Parallel Current Carrying Wires Calculator
- Magnetic Potential Energy Stored In An Inductor Calculator
- Output Current In A Transformer Calculator
- Phase Constant In A Rlc Circuit Calculator
- Power Factor In A Rlc Circuit Calculator
- Power Induced On A Metal Bar Moving Inside A Magnetic Field Due To An Applied Force Calculator
- Radius Of Trajectory And Period Of A Charge Moving Inside A Uniform Magnetic Field Calculator
- Self Induced Emf Calculator
- Self Inductance Calculator
- Torque Produced By A Rectangular Coil Inside A Uniform Magnetic Field Calculator
- Work Done On A Magnetic Dipole Calculator

You may also find the following Physics calculators useful.

- Lande G Factor Calculator
- Force Of Magnetic Field Calculator
- J Pole Antenna Calculator
- Liquid Phase Coefficient Calculator
- Average Velocity Calculator
- Gas Pressure Calculator
- Output Current In A Transformer Calculator
- Orbit Pericenter Distance Calculator
- Conical Pendulum Calculator
- Ideal Gas Law Calculator
- Ramsauer Townsend Effect Calculator
- Radius Of Trajectory And Period Of A Charge Moving Inside A Uniform Magnetic Field Calculator
- Hall Electrical Conductivity Calculator
- Convective Heat Transfer Calculator
- D Exponent Calculator
- Helical Spring Axial Deflection Calculator
- Orbital Velocity Calculator
- Density Of Sand Calculator
- Power And Efficiency Calculator
- Power Factor In A Rlc Circuit Calculator