To perform a transient analysis of an RL (Resistor-Inductor) circuit with a step input using Laplace transforms, you'll follow these steps:
Step 1: Obtain the circuit differential equation:
Start by writing down the governing differential equation for the RL circuit. For a series RL circuit, the differential equation is derived from Kirchhoff's voltage law:
(
)
=
(
)
+
⋅
(
)
v(t)=L
dt
di(t)
+R⋅i(t)
where:
(
)
v(t) is the input voltage (step input in this case, v(t) = V for t ≥ 0)
(
)
i(t) is the current flowing through the inductor
L is the inductance of the inductor
R is the resistance of the resistor
Step 2: Take the Laplace transform of the differential equation:
Apply the Laplace transform to both sides of the equation. The Laplace transform of
(
)
v(t) with respect to
t is denoted as
(
)
V(s), and the Laplace transform of
(
)
i(t) with respect to
t is denoted as
(
)
I(s). The Laplace transform of
(
)
dt
di(t)
is
(
)
−
(
0
)
sI(s)−i(0), where
(
0
)
i(0) is the initial condition of the current (current at t = 0+).
After taking the Laplace transform and applying the initial condition
(
0
)
i(0), the equation becomes:
(
)
=
⋅
(
(
)
−
(
0
)
)
+
⋅
(
)
V(s)=L⋅(sI(s)−i(0))+R⋅I(s)
Step 3: Solve for
(
)
I(s):
Rearrange the equation to solve for
(
)
I(s):
(
)
=
(
)
+
(
0
)
⋅
+
I(s)=
sL+R
V(s)+i(0)⋅s
Step 4: Perform inverse Laplace transform:
Now, you need to take the inverse Laplace transform of
(
)
I(s) to get the time-domain current
(
)
i(t). The inverse Laplace transform of
(
)
I(s) can be found using tables or software tools like MATLAB or Wolfram Alpha.
The inverse Laplace transform of
(
)
+
(
0
)
⋅
+
sL+R
V(s)+i(0)⋅s
is denoted as
(
)
i(t).
Step 5: Include initial conditions:
Finally, include the initial condition
(
0
)
i(0) to obtain the complete time-domain current
(
)
i(t).
In summary, follow these steps to perform transient analysis of an RL circuit with a step input using Laplace transforms:
Write the differential equation for the circuit.
Take the Laplace transform of the equation.
Solve for
(
)
I(s) in terms of
(
)
V(s) and
(
0
)
i(0).
Perform the inverse Laplace transform to get
(
)
i(t).
Include the initial condition
(
0
)
i(0) to get the complete time-domain current
(
)
i(t).