What is a parallel RLC circuit? An RLC circuit is an electrical circuit consisting of a resistor Ran inductor Land a capacitor Cconnected in series or in parallel. The name of the circuit is derived from the letters that are used to denote the constituent components of this circuitwhere the sequence of the components may vary from RLC.
See Full Answer. What is acceptor and Rejector circuit? A series resonance circuit is also known as an Acceptor Circuit because at resonance, the impedance of the circuit is at its minimum so easily accepts the current whose frequency is equal to its resonant frequency or we can say that it functions mainly at resonance.
Capacitive reactance symbol XC is a measure of a capacitor's opposition to AC alternating current. Like resistance it is measured in ohms, but reactance is more complex than resistance because its value depends on the frequency f of the signal passing through the capacitor.
The resonance of a parallel RLC circuit is a bit more involved than the series resonance. The resonant frequency can be defined in three different ways, which converge on the same expression as the series resonant frequency if the resistance of the circuit is small. Impedance definition. Phase definition. The most prominent feature of the frequency response of a resonant circuit is a sharp resonant peak in its amplitude characteristics.
Because impedance is minimum and current is maximum, series resonance circuits are also called Acceptor Circuits. What is a parallel resonant circuit? Parallel Resonance. Why a series resonant circuit is called an acceptor circuit? What is the difference between a series and a parallel circuit? In a series circuitthe current through each of the components is the same, and the voltage across the circuit is the sum of the voltages across each component.
In a parallel circuitthe voltage across each of the components is the same, and the total current is the sum of the currents through each component. What is series resonant circuit? The resonance of a series RLC circuit occurs when the inductive and capacitive reactances are equal in magnitude but cancel each other because they are degrees apart in phase.
The sharp minimum in impedance which occurs is useful in tuning applications.Take this series-parallel circuit for example:. The first order of business, as usual, is to determine values of impedance Z for all components based on the frequency of the AC power source. To do this, we need to first determine values of reactance X for all inductors and capacitorsthen convert reactance X and resistance R figures into proper impedance Z form:.
Being a series-parallel combination circuit, we must reduce it to a total impedance in more than one step. The first step is to combine L and C 2 as a series combination of impedances, by adding their impedances together.
Then, that impedance will be combined in parallel with the impedance of the resistorto arrive at another combination of impedances. Finally, that quantity will be added to the impedance of C 1 to arrive at the total impedance. In order that our table may follow all these steps, it will be necessary to add additional columns to it so that each step may be represented. Adding more columns horizontally to the table shown above would be impractical for formatting reasons, so I will place a new row of columns underneath, each column designated by its respective component combination:.
This time, there is no avoidance of the reciprocal formula: the required figures can arrive at no other way! This gives us one table with four columns and another table with three columns.
Now that we know the total impedance At this point we ask ourselves the question: are there any components or component combinations which share either the total voltage or the total current? That last step was merely a precaution. In a problem with as many steps, as this one has, there is much opportunity for error.
Occasional cross-checks like that one can save a person a lot of work and unnecessary frustration by identifying problems prior to the final step of the problem. In this case, the resistor R and the combination of the inductor and the second capacitor L—C 2 share the same voltage, because those sets of impedances are in parallel with each other. Therefore, we can transfer the voltage figure just solved into the columns for R and L—C 2 :. Another quick double-check of our work at this point would be to see if the current figures for L—C 2 and R add up to the total current.
Since the L and C 2 are connected in series, and since we know the current through their series combination impedance, we can distribute that current figure to the L and C 2 columns following the rule of series circuits whereby series components share the same current:. With one last step actually, two calculationswe can complete our analysis table for this circuit.
As you can see, these figures do concur with our hand-calculated figures in the circuit analysis table.In simple reactive circuits with little or no resistance, the effects of radically altered impedance will manifest at the resonance frequency predicted by the equation given earlier.
In a parallel tank LC circuit, this means infinite impedance at resonance. In a series LC circuit, it means zero impedance at resonance:. However, as soon as significant levels of resistance are introduced into most LC circuits, this simple calculation for resonance becomes invalid. According to our simple equation above, the resonant frequency should be Resistance in series with L produces minimum current at Resistance in series with C shifts minimum current from calculated Switching our attention to series LC circuits, we experiment with placing significant resistances in parallel with either L or C.
The results are shown in the figure below. Series LC resonant circuit with resistance in parallel with L. Series resonant circuit with resistance in parallel with L shifts maximum current from And finally, a series LC circuit with the significant resistance in parallel with the capacitor The shifted resonance is shown below.
Series LC resonant circuit with resistance in parallel with C. Resistance in parallel with C in series resonant circuit shifts current maximum from calculated The tendency for added resistance to skew the point at which impedance reaches a maximum or minimum in an LC circuit is called antiresonance. The astute observer will notice a pattern between the four SPICE examples given above, in terms of how resistance affects the resonant peak of a circuit:.
Again, this illustrates the complementary nature of capacitors and inductors : how resistance in series with one creates an antiresonance effect equivalent to resistance in parallel with the other.
Antiresonance is an effect that resonant circuit designers must be aware of. It should suffice the beginning student of electronics to understand that the effect exists, and what its general tendencies are.
Added resistance in an LC circuit is no academic matter. While it is possible to manufacture capacitors with negligible unwanted resistances, inductors are typically plagued with substantial amounts of resistance due to the long lengths of wire used in their construction.
Thus, inductors not only have resistance, but changing, frequency-dependent resistance at that. Since iron is a conductor of electricity as well as a conductor of magnetic flux, changing flux produced by alternating current through the coil will tend to induce electric currents in the core itself eddy currents. This effect can be thought of as though the iron core of the transformer were a sort of secondary transformer coil powering a resistive load: the less-than-perfect conductivity of the iron metal.
This effects can be minimized with laminated cores, good core design high-grade materials, but never completely eliminated. So long as all components are connected in series with each other, the resonant frequency of the circuit will be unaffected by the resistance.Second-order RLC circuits have a resistor, inductor, and capacitor connected serially or in parallel.
To analyze a second-order parallel circuit, you follow the same process for analyzing an RLC series circuit. Here is an example RLC parallel circuit. The left diagram shows an input i N with initial inductor current I 0 and capacitor voltage V 0.
The top-right diagram shows the input current source i N set equal to zero, which lets you solve for the zero-input response. The bottom-right diagram shows the initial conditions I 0 and V 0 set equal to zero, which lets you obtain the zero-state response. With duality, you substitute every electrical term in an equation with its dual, or counterpart, and get another correct equation.
For example, voltage and current are dual variables. KCL says the sum of the incoming currents equals the sum of the outgoing currents at a node. Next, put the resistor current and capacitor current in terms of the inductor current.
The current i L t is the inductor current, and L is the inductance. This constraint means a changing current generates an inductor voltage. Parallel devices have the same voltage v t. Substitute the values of i R t and i C t into the KCL equation to give you the device currents in terms of the inductor current:.
The RLC parallel circuit is described by a second-order differential equation, so the circuit is a second-order circuit. The unknown is the inductor current i L t. Compare the preceding equation with this second-order equation derived from the RLC series:. The two differential equations have the same form.
The unknown solution for the parallel RLC circuit is the inductor current, and the unknown for the series RLC circuit is the capacitor voltage.
These unknowns are dual variables.03 Parallel \u0026 Series, Resistor, Inductor, Capacitor = RLC circuit
With dualityyou can replace every electrical term in an equation with its dual and get another correct equation. If you use the following substitution of variables in the differential equation for the RLC series circuit, you get the differential equation for the RLC parallel circuit.
For a parallel circuit, you have a second-order and homogeneous differential equation given in terms of the inductor current:. The zero-input responses of the inductor responses resemble the form shown here, which describes the capacitor voltage. When you have k 1 and k 2you have the zero-input response i ZI t. The solution gives you. You can find the constants c 1 and c 2 by using the results found in the RLC series circuit, which are given as. Apply duality to the preceding equation by replacing the voltage, current, and inductance with their duals current, voltage, and capacitance to get c 1 and c 2 for the RLC parallel circuit:.
After you plug in the dual variables, finding the constants c 1 and c 2 is easy. Zero-state response means zero initial conditions. The second-order differential equation becomes the following, where i L t is the inductor current:. Adding the homogeneous solution to the particular solution for a step input IAu t gives you the zero-state response i ZS t :. You now apply duality through a simple substitution of terms in order to get C 1 and C 2 for the RLC parallel circuit:.
You finally add up the zero-input response i ZI t and the zero-state response i ZS t to get the total response i L t :. The solution resembles the results for the RLC series circuit.The series behavior of the three elementary components of electronics has been detailed in our previous article Series RLC Circuit Analysis. In this tutorial, another association known as the parallel RLC circuit is presented. To conclude these two articles about RLC circuits, alternative configurations are presented in the last section.
The parallel RLC circuit consists of a resistor, capacitor, and inductor which share the same voltage at their terminals:. Since the voltage remains unchanged, the input and output for a parallel configuration are instead considered to be the current. In other terms, the total admittance of the circuit is the sum of the admittances of each component. The total impedance is therefore given by Equation 1 after taking the norm of the admittance:.
Fast analysis of the impedance can reveal the behavior of the parallel RLC circuit. It is clearly evidenced by this figure that around the resonance frequency, the impedance of the circuit peaks, which leads to a decrease of the current output around this same frequency.
The following Figure shows the steps involved in a cycle called resonance :. Many things must be commented in Figure 3. First of all, the red and green arrows represent respectively the electric field across the capacitor and the magnetic field across the inductor.
The arrows indicate the direction of the fields, a fully charged component is represented with many arrows while a discharged component has none.
The numbers represent the steps of the cycle, the next step after number 8 is step number 1. As highlighted in this series of figures, the resonance phenomenon is due to mutual charges and discharges occurring between the capacitor and the inductor. However, an AC source can force the circuit to maintain this exchange of current between the inductor and capacitor. Another way to understand that is through the concept of reactance. We remind that the reactances of a capacitor X C and an inductor X L are given by:.
This phenomenon can be seen in steps 2 and 4 or steps 6 and 8 in Figure 3. A representation of this architecture is given in Figure 4 below:. An interesting concept called duality enables us to directly find the behavior of a new circuit from the knowledge of another.We recommend downloading the newest version of Flash here, but we support all versions 10 and above.
If that doesn't help, please let us know. Unable to load video. Please check your Internet connection and reload this page. If the problem continues, please let us know and we'll try to help. An unexpected error occurred. A resistor is an electrical component that dissipates energy, usually in the form of heat. In contrast, a capacitor stores energy in an electric field, and an inductor stores energy in a magnetic field.
When resistors, capacitors and inductors are connected together, the circuits display time and frequency dependent responses useful for AC signal processing, radios, electrical filters and many other applications.
This video will illustrate the behaviors of a resistor-capacitor and a resistor-inductor circuit, and show the oscillation in an inductor-capacitor circuit with little resistive energy loss. Let's learn how current and voltage behave in circuits involving resistors, inductors and capacitors.
First, let's talk about a circuit of a resistor in series with a capacitor, called an RC circuit. When the switch is closed, the output of the voltage source is applied across both components and current starts flowing. As, the capacitor is initially uncharged, it has zero voltage across its terminals. Hence, all of the voltage source's output appears across the resistor and the current is at its maximum value.
If we look at the plot of voltage and current against time, initially VR equals source voltage the voltage across the capacitor 'VC' is zero and the current is at its max. As the current charges the capacitor, 'VC' increases. In response, VR decreases and therefore the current also goes down, in accordance with Ohm's Law. Eventually the resistor voltage is zero and the current flow stops.
A similar analysis is possible for an RL circuit consisting of a resistor in series with an inductor. At the instant the switch closes, the sudden flow of charge creates a magnetic field in the inductor, and its voltage 'VL' is equal to the source's voltage.
Consequently, the initial VR is zero and thus the initial current is also zero. Now, to monitor the changes, let's look at the voltage and current graphs like before. Over time as the inductor voltage decreases, the voltage across the resistor increases and therefore the current also increases. Ultimately, the inductor voltage is zero, all of the voltage source output is across the resistor, and the current is at its maximum value.
The decay of current and voltage transients in RC and RL circuits is caused by energy dissipation in the resistor. In contrast, an LC circuit, which has a capacitor connected to an inductor, ideally has no resistance or energy loss, and exhibits very different behavior. If the capacitor in this circuit is charged to voltage V and then connected to the inductor, electrical energy stored in the capacitor is transferred to the inductor and converted to magnetic energy.This parallel RLC circuit impedance calculator determines the impedance and the phase difference angle of a resistor, an inductor, and a capacitor connected in parallel for a given frequency of a sinusoidal signal.
The angular frequency is also determined. This example shows a high, near-resonance impedance of about ,99 ohms. If you want to check the impedance at almost exact resonance, enter The circuit is slightly inductive and the inductive reactance is less than the capacitive one. If you enter slightly higher frequency Enter the resistance, capacitance, inductance, and frequency values, select the units and click or tap the Calculate button.
Resonance RLC Series Circuit
Try to enter zero or infinitely large values to see how this circuit behaves. Infinite frequency is not supported. To enter the Infinity value, just type inf in the input box.
C is the capacitance in farads F. To calculate, enter the resistance, the inductance, the capacitance, and the frequency, select the units of measurements and the result for the RLC impedance will be shown in ohms and for the phase difference in degrees. The Q factor, C and L reactance, and the resonant frequency will also be calculated. Click or tap Calculate at the resonant frequency to see what will happen at resonance.
Like a pure parallel LC circuitthe RLC circuit can resonate at a resonant frequency and the resistor increases the decay of the oscillations at this frequency. The resonance occurs at the frequency at which the impedance of the circuit is at its maximum, that is, if there is no reactance in the circuit.
In other words, if the impedance is purely resistive or real. This phenomenon occurs when the reactances of the inductor and the capacitor are equal and because of their opposite signs, they cancel each other the canceling can be observed on the right phasor diagram below.
The calculator defines the resonant frequency of the RLC circuit and you can enter this frequency or the value slightly above or below it to view what will happen with other calculated values at resonance.
The calculator also defines the Q factor of the RLC circuit, a parameter, which is used to characterize resonance circuits and not only electrical but mechanical resonators as well. Damped and lossy RLC circuits with low resistance have a low Q factor and are wide-band, while circuits with low resistance have a high Q factor. For a parallel RLC circuit, the Q factor can be calculated using the formula above.
In the parallel RLC circuit, the applied voltage is the same for the resistor, the inductor, and the capacitor, but the individual currents in all branches of the circuit are different. The phasor diagram shows the V T voltage of the ideal voltage source. Because there is a resistance, the resistor current vector appears in phase with the applied voltage.
The vector sum of the two opposing vectors can be pointed downwards or upwards depending on the current flowing through the inductance and capacitance.