RL Parallel Circuit

In this Article, We will be going through the RL Parallel Circuit, We will start our Article with the Introduction of the RL Parallel Circuit, Then we will go through the Circuit Diagram of the RL Parallel Circuit where we will calculate circuit parameters and See its phasor Diagram, Then we will calculate Power and Impedance of the Parallel Circuit, At last we will conclude our Article withExample, Applications, and Some FAQs.

An RL parallel circuit is formed when a resistor and an inductor are connected in parallel and driven by the same voltage source. Unless it is powered by a current source, the parallel RL circuit is generally less interesting than the series circuit. This is mostly because this circuit does not act as a voltage input filter. After all, the output voltage (Vout) and input voltage (Vin) are equal.

Many amplifier designs include a parallel circuit on the output that is used to protect the amplifier from high-frequency capacitive loading effects. Certain amplifiers develop instability and oscillation at very high frequencies as a result of capacitance-induced phase shift. An electric circuit having resistance and self-inductance is another way to define an RL circuit. We already know that when an EMF source is applied by a constant variation in the magnetic flux, the induction process takes place. Self-inductance is the result of a device coming into contact with its own Faraday laws of induction, whereas mutual inductance is the result of Faraday’s laws of induction. A component of a circuit or device that demonstrates self-inductance is called an inductor. An RL circuit will use energy, much like an RC or RLC circuit, because a resistor is present in the optimal version of the circuit.

In the RL parallel circuit diagram, the R and L are connected in parallel. The parallel property of the circuit is defined as the division of current in branches. If we consider the heat and energy then the Resistor provides heat loss and the inductor gives the magnetic store energy. The circuit diagram is shown below.

the shown diagram is for the A.C applied source.

Where,

R is the Resistor

L is the Inductor

V_R = V_L = V_supplied (in parallel Combination)

So,

( XL = jωL )

Where,ω is the frequency of applied signal

So the Final Equation can be Written as

As we know

• The voltage in the circuit, which is shared by every element, is represented by the reference vector, which has the letter V on it. I_R is displayed across the voltage vector because the current flowing through the resistor is in phase with the voltage across it.
• The inductor current (I_L) is positioned downward and lags the voltage vector by 90 degrees. It also lags the voltage by 90 degrees.
• The total, or line current, is represented by the resultant of the vector addition of I_R and I_L. The phase difference between the applied line voltage and current is represented by the angle (φ).

we know cos(φ) is power factor

Total current (I_T) can be written as

So,as we Know the Value of ,the can be Written as

Total current

True power (W) is the power dissipated by the resistive branch, while reactive power (VARs) is the power returned to the source by the inductive branch. Together, these two types of power are referred to as VA (apparent power) in the parallel RL circuit.

Power Factor =cos(φ)=

The voltage drop across the resistor multiplied by the current passing through it yields the true power in watts.

W = V_R x I_R

The voltage drop across the inductor times the current passing through it equals the reactive power in VARs.

VARs = V_L x I_L

The applied voltage multiplied by the total current yields the apparent power in VA.

The current in each branch of a parallel RL circuit acts independently of the currents in the other branches, as is the case in all parallel circuits. Each branch’s current flow is dictated by the voltage across it as well as any resistance or inductive reactance that may be present in the branch to impede current flow.

The total resistance to the current flow in a parallel RL circuit is known as the impedance (Z). It consists of the inductive reactance (XL) provided by the inductive branch and the opposition (R) provided by the resistive branch.

In the Given Circuit Resistance and Inductor are parallel

So,Calculating the impedance Z we have,

Z=

Now Dividing the numerator and denominator by R-jX_L

Z=

We know j² =-1

Z=

For the parallel RL circuit shown in Figure, determine:

• Current flow through the R .
• Current flow through the L .
• The total line current.
• Phase between voltage and total current.

Solution:

I_R = V / R = 120 / 30 = 4 A

I_L = V / X_L = 120 / 40 = 3 A

I_T = (4² + 3²)^1/2 = 5 A

ϕ = tan^-1(I_L / I_R) = tan^-1(3/4) = 36⁰

• For providing DC power to radio-frequency amplifiers, where the DC bias current is passed through an inductor to prevent radio waves from returning to the power source.
• A single-pole filter can be formed by RL circuits.
• Inductors in RL parallel circuits play important roles in radio wave transmitters, where they are used for impedance matching, frequency tuning, and signal amplification.
• RL circuits are integral parts of resonant LC (RLC) circuits used in resonant applications.
• RL parallel circuits are used in communication systems for impedance matching, signal filtering, and amplification purposes.
• Processing of Signal.
• Inductors in RL parallel circuits are commonly used in oscillator circuits to generate periodic waveforms.
• RL circuits can be designed to magnify current or voltage signals, allowing for higher power delivery or signal amplification in various electronic systems and devices.
• Variable inductors in RL parallel circuits enable frequency tuning and adjustment in circuits
• RL parallel circuits are widely used in filtering applications to remove unwanted noise, interference, or harmonics from signals.

An RL circuit can also be defined as an electric circuit having self-inductance plus resistance. We also know that the induction process occurs when an emf source is applied through a continuous change in the magnetic flux. While mutual inductance is the outcome of Faraday’s laws of induction, self-inductance is the effect of a device comes into contact with its own Faraday laws of induction. An inductive element is a part of a circuit or apparatus that displays self-inductance. Because a resistor is a part of the ideal circuit, an RL circuit will use energy, just like an RC or RLC circuit, because the ideal version of the circuit contains a resistor.The main parts of a first-order RL circuit include one resistor and one inductor. The low power factor of the circuit is caused by the inductive load, such as a three-phase induction motor. None of the lights, transformers or welding equipment work at low leading power factor values.

What is an RL circuit’s power factor?

The ratio of actual power dissipated to apparent power is known as the power factor of an RL circuit.

Which applications are there for RL circuits?

Communication systems, radio wave transmitters, oscillator circuits, RF amplifiers, filtering circuits, variable tuned circuits, current and voltage magnification, etc. are applications for RL circuits.

Define RL circuit

An RL circuit is made up of passive parts that are coupled to one another, such as an inductor and resistor, are powered by either a voltage source or current source.

What is an RL series circuit’s time constant?

Constant in Time, τ = L/R

L stands for inductance.

R stands for resistance.