thai anal tubePrevious posts in this series:
- Electronics 101: Voltage, Current and Resistance
thai anal tubeElectronics 101 pt. 2: Kirchhoff’s Laws
- Electronics 101 pt. 4: RL and RC Circuits
If you’re unsure about how capacitors and/or inductors work, check out:
In part 4 we looked at the natural response and step response of RL and RC circuits, which means circuits with resistors together with inductors and capacitors, respectively.
This time we will take a look at , which contain both resistor(s), inductor(s) and capacitor(s), and examine their natural response and step response. We’ll not go into too much detail regarding the theory behind this material, but rather show you quite directly how to find expressions for the responses of RLC circuits.
Since this is a theory-heavy blog post, it is most suited to electrical engineering students as a supplement to other learning material. Others might find this interesting as well, especially those who are curious about how capacitors and inductors can influence a circuit.
The equations and examples in this blog post are taken from the book Electric Circuits by Nilsson and Riedel.
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We need to separate between parallel RLC circuits and series RLC circuits. Below you will find simplified theoretical circuits to illustrate different concepts in the following order:
- Natural response of a parallel RLC circuit
- Step response of a parallel RLC circuit
- Natural response of a series RLC circuit
- Step response of a series RLC circuit
We will use a couple of these in examples later in this blog post.
As opposed to RL and RC circuits, RLC circuits can be overdamped, underdamped or critically damped. The behavior of these are not the same as we talked about in this post. Here, both overdamped and critically damped circuits can overshoot the final value. However, they will not oscillate beyond that. Underdamped circuits will oscillate beyond the initial overshoot.
The combination of R, L and C values decides what kind of damping the circuit has:
The value of α (aka. the neper frequency) depends if the RLC circuit is parallel or series:
The value of ω0 (aka. the resonant radian frequency) is the same regardless of type of circuit:
Both α and ω0 have the unit of rad/s (radians per second).
What we want to do is to find an expression of either voltage or current as a function of time: x(t). There are six different equations for this, where the one you want to use is chosen based on whether you’re looking for the natural response or step response, and whether the system is overdamped, underdamped or critically damped. Each equation has a set of coefficients which need to be found. To find these coefficients you will need the initial value x(0), the initial time derivative of x dx(0)/dt and sometimes the roots of the characteristic equation. We’ll go into detail on how to do this later in this post.
- Natural response or step response?
- Find out if the circuit is overdamped, underdamped or critically damped.
- Choose the proper response equation based on 1. and 2.
- Find x(0) and dx/dt(0).
- Find the roots of the of the characteristic equation if necessary.
- Find the response equation’s coefficients using what you found in 4.
- Use the coefficients found in 6. (and the roots found in 5. if applicable) to complete the expression for the response using the equation chosen in 3.
The Characteristic Equation and Its Roots
For both parallel and series RLC circuits, the so called characteristic equation is
We need s in the overdamped response equations, and since the characteristic equation is a quadratic equation we will get two different values of s, aka. the roots of the characteristic equation. Use this equation to find the roots s1 and s2:
Natural Response Equations
In the following equations, the variable x represent either voltage or current, depending on what we want to calculate. With all natural response equations, we expect the x value to start at an initial value x(0) and converge towards zero in some way.
Overdamped Natural Response
In this scenario, the expected behavior of x(t) is a non-oscillating convergence from x(0) to zero. It might overshoot the final value.
To find the coefficients A1 and A2, you have to have two different equations. These ones are used in this specific scenario:
Note the usage of the roots s1 and s2.
Underdamped Natural Response
In this scenario, the expected behavior of x(t) is an approach from x(0) towards zero. It will dip below zero before oscillating and converging towards its final value.
aka. the damped radian frequency.
Critically Damped Natural Response
In this scenario, the expected behavior of x(t) is a similar to the overdamped scenario, except that it is on the verge of oscillating.
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These step response equations are quite similar to the natural response equations excepts they go from an initial value x(0) to a final value Xf.
Overdamped Step Response
Underdamped Step Response
Critically Damped Step Response
Let’s run through a few examples.
Overdamped Natural Response of a Parallel RLC Circuit
In this example, we’ll let
- C = 0.2 μF
- L = 50 mH
- R = 200 Ω
We need to know some initial conditions to get going. In this case we know that
- v(0) = 12 V
- iL(0) = 30 mA
Let’s double check that this is overdamped:
- α = 12500 rad/s
- ω0 = 10000 rad/s
α > ω0, thus overdamped.
Since we already know v(0), the first thing we need to do is to find dv/dt(0). We can use the following equation for this, which is a fundamental equation for capacitors:
Ohm’s law gives us iR = 60 mA. Kirchoff’s current law then gives us iC = -90 mA.
Now we have all we need: dv(0)/dt = -450 kV/s
Next, we need to find the roots. Use the equations mentioned earlier in this blog post.
- s1 = -5000 rad/s
- s2 = -20000 rad/s
Now we can dive into the coefficient equations for overdamped natural response. Use both equations to find A1 and A2.
- A1 = -14 V
- A2 = 26 V
Finally, we’re ready for the main overdamped natural response equation. Let’s plot it!
Underdamped Step Response of a Series RLC Circuit
Let’s switch all parameters and look at how it turns out.
- V = 48 V
- R = 280 Ω
- L = 0.1 H
- C = 0.4 μF
Our aim will be to find the voltage across the capacitor vc, with the + sign above the capacitor.
Let’s double check if this is underdamped or not:
- α = 1400 rad/s
- ω0 = 5000 rad/s
ω0 > α, thus underdamped.
Since no energy is stored in the circuits at t=0, we have that
- vc(0) = 0
- dvc(0)/dt = 0
We don’t need the roots for this, so we can jump directly to the coefficients:
- B’1 = -48 V
- B’2 = -14 V
After some time, no current will flow through the circuit because of the capacitor. Thus Xf = V = 48 V.
We now have everything we need for a sweet plot.
That was a lot of theory and equations, but if you took your time to go through this, this was probably what you was looking for in the first place.
We recommend that you read a proper textbook to fully understand these concepts. Electric Circuits by Nilsson and Riedel is an excellent choice.
Another source of knowledge and wisdom is this free online course where they among other things look at “time and frequency behavior of second-order circuits containing energy storage elements (capacitors and inductors)”, which is what we’ve briefly looked at here.
This blog post is only meant as a supplement to any material you already have.