Our dialogue factors:- What is an RL Circuit, There are principal kinds of RL circuits, Working Principle of RL Circuits, Series RL Circuit, RL Parallel Circuit, Applications of RL Circuits , Summary.
What is an RL Circuit: -
An RL circuit is an electric-powered circuit that consists
of a resistor (R) and an inductor (L) linked to a voltage or current supply. It
is referred to as an "RL" circuit because it consists of both a
resistive and an inductive element.
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RL CIRCUIT |
There are two major styles of RL circuits: -
Series RL Circuit: Resistor and inductor linked end to give
up (in collection).
Parallel RL Circuit: a resistor and an inductor connected to the same voltage source (in parallel).
Symbols:
R = Resistance (Ohms, Ω)
L = Inductance (Henrys, H)
V = Voltage (Volts, V)
I = Current (Amperes, A)
Working Principle of RL Circuits: -
The inductor inside the circuit resists modifications in
current using a returned EMF (electromotive force). When
current flows through the circuit, the inductor stores power in the
shape of a magnetic field.
When the power delivery is suddenly turned on or off, the
inductor tries to hold the present current by either absorbing or releasing
energy. This results in a time delay inside modern-day, attaining its maximum or
0 cost.
This time-established conduct makes RL circuits useful in
timing programs and temporary response analysis.
Series RL Circuit: -
In a series RL circuit, the resistor and inductor are linked in a single route, and the same current flows through each component.
The above LR collection circuit is connected across a steady
voltage supply (the battery) and a transfer. Assume that the switch, S, is open
till it's miles closed at a time t = zero and then stays completely closed,
generating a “step reaction” kind of voltage to enter. The contemporary, I begins
to go with the flow through the circuit but no longer thrusts upward swiftly to
its maximum value of Imax as determined by the ratio of V/R (Ohm's Law).
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SERIES RL CIRCUIT |
This restricting element is due to the presence of the self-induced
emf within the inductor as a result of the growth of magnetic flux (Lenz’s
Law). After a time, the voltage supply neutralises the effect of the self-triggered
EMF, the present-day drift becomes constant, and the brought-about cutting-edge
and field are decreased to zero.
We can use Kirchhoff’s Voltage Law (KVL) to define the man or woman voltage drops that exist across the circuit, after which, with a bit of luck, use it to provide us an expression for the flow of contemporary.
Kirchhoff's Voltage Law (KVL) Equation:
When a DC voltage source is implemented in an RL chain circuit, the voltage equation turns into:
V = IR + L(dI/dt)
Where:
- V is the supply voltage
- IR is the voltage drop across the resistor
- L(dI/dt) is the voltage across the inductor
Time Constant (τ):
The time constant (τ) of a sequence RL circuit is given
by:
τ = L / R
It represents the time required for the present day to
attain about 63.2% of its final cost after a sudden exchange.
RL Parallel Circuit: -
An RL parallel circuit is formed while a resistor and an
inductor are connected in parallel and driven with the aid of an identical
voltage supply. Unless it is powered by way of a modern source, the parallel RL
circuit is generally less exciting than the series circuit. This is frequently
due to the fact that this circuit does not act as a voltage entry filter. After all,
the output voltage (Vout) and enter voltage (Vin) are equal.
Many amplifier designs encompass a parallel circuit at the
output, which is used to defend the amplifier from excessive-frequency
capacitive loading consequences. Certain amplifiers develop instability and
oscillation at very high frequencies as a result of capacitance-induced section
shift. An electric-powered circuit having resistance and self-inductance is
another way to define an RL circuit. We already realize that when an EMF source
is implemented through a consistent variation inside the magnetic flux, the
induction technique takes place. Self-inductance is the result of a device
getting into contact with its personal Faraday laws of induction, whereas
mutual inductance is the result of Faraday's laws of induction. A factor of a
circuit or tool that demonstrates self-inductance is known as an inductor. An
RL circuit will use energy, just like an RC or RLC circuit, because a resistor
is gift within the most suitable model of the circuit.
Circuit Diagram of RL Parallel Circuit: -
In the RL parallel circuit diagram, the R and L are
connected in parallel. The parallel assets of the circuit are described as the
division of cutting-edge in branches. If we recall the warmth and strength,
then the resistor gives warmth loss, and the inductor gives the magnetic saving
of energy. The circuit diagram is shown below.

Where,
- R is the Resistor
- L is the inductor
- V is the voltage.
- I=IR+IL
- IR = V/R
Applications of RL Circuits: -
Common Applications:
- Filters: Used in excessive-pass and band-skip filters in signal processing.
- Inductive Loads: Modelling the behaviour of inductive devices like motors and transformers.
- Transient Suppression: Protect circuits from voltage spikes.
- Timers and Delays: Create time delays in relay and control systems.
- Current Control: Limit inrush cutting-edge in power materials.
- AC Analysis: Analyse alternating contemporary conduct and impedance.
Summary: -
Parameter |
Series RL
Circuit |
Parallel
RL Circuit |
Components |
R and L in
series |
R and L in
parallel |
Time Constant
(τ) |
L / R |
L / R
(applies to individual branches) |
Behavior with
DC |
Current grows
exponentially |
Voltage is the same
across branches |
Behavior with
AC |
Inductive
reactance opposes current |
Phase
difference in current paths |
Application
Examples |
Filters,
delays, motor modeling |
AC filtering,
signal mixing |
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