Second Order Circuits: Difference between revisions

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-\alpha B_1 + \omega_d B_2 =  \frac{1}{C} \left( \frac{-V_0}{R} - I_0 \right)
-\alpha B_1 + \omega_d B_2 =  \frac{1}{C} \left( \frac{-V_0}{R} - I_0 \right)
</math>
</math>
==== Characteristics ====
Voltage alternates between positive and negative values due to the two
types of energy-storage elements. It's like a mass suspended on a
spring.
The oscillation rate is fixed by <math>\omega_d</math>, which is why it
is called the '''damped radian frequency'''.
The oscillation amplitude decreases exponentially at a rate determined
by <math>\alpha</math>, so it is called the '''damping factor'''.
Notice that when <math>R \neq 0</math>, there is <math>\alpha > 0</math>
and the circuit is damped.


[[Category:Electrical Engineering]]
[[Category:Electrical Engineering]]

Revision as of 08:41, 8 March 2024

Second order circuits are circuits that have two energy storage elements, resulting in second-order differential equations.

One application of second order circuits is in timing computers. As we will see, an RLC circuit can generate a sinusoidal wave.

There are primarily two types of second order circuits:

  • Parallel RLC circuits
  • Series RLC circuits

This page will analyze them and derive some useful equations.

Series RLC Circuits

Natural Response

An unforced series RLC circuit

Consider an un-forced RLC circuit. We want to find .

First, we can use KVL and KCL

Next, we can use and substitution to get

Changing the order and moving the constants,

Moving constants away from the first term to get a second-order differential equation,

Parallel RLC Circuits

Natural Response

A parallel unforced RLC circuit

By KCL,

By differentiating once with respect to and rearranging some constants,

we get a homogeneous second-order differential equation, which has a standard solution that I will not go into detail. Briefly, it is solved by assuming since derivatives of must take the same form to cancel out to zero.

By applying the standard solution, we have

Characteristic Equation

The above simplifies to

This is the characteristic equation of the differential equation, as the root of the quadratic determines properties of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v(t)}

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle s_{1,2} = - \frac{1}{2RC} \pm \sqrt{ \left(\frac{1}{2RC}\right)^2 - \frac{1}{LC}} = - \alpha \pm \sqrt{\alpha^2 - \omega_0^2} }

where

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha = \frac{1}{2RC} }

and

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \omega_0 = \frac{1}{\sqrt{LC}} }

It can be pretty easily proven that the sum of the two roots is also a solution

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v = A_1 e^{s_1 t} + A_2 e^{s_2 t} }

Forms

Depending on the root, there are three forms:

  • Overdamped, where there are real, distinct solutions
  • Underdamped, where there are complex solutions
  • Critically damped, where the solutions are not distinct.


Overdamped

For an overdamped response, we have

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v = A_1 e^{s_1 t} + A_2 e^{s_2 t} }

The A's can be solved by substituting in Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v(0)} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle dv(0) / dt = i_C / C}

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v(0) = A_1 + A_2 }

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle dv(0)/dt = A_1 s_1 + A_2 s_2 = \frac{1}{C} \left( \frac{-V_0}{R} - I_0 \right) }

Underdamped

For an underdamped response, we have

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle s_{1,2} = - \alpha \pm j \omega_d }

where there is damped radian frequency

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \omega_d = \sqrt{w_0^2 - \alpha^2} }

From Euler's identity, the natural response comes to

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v(t) = B_1 e^{-\alpha t} \cos \omega_d t + B_2 e^{-\alpha t} \sin \omega_d t }

The rest is identical to that of overdamped:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle B_1 = V_0 }

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle -\alpha B_1 + \omega_d B_2 = \frac{1}{C} \left( \frac{-V_0}{R} - I_0 \right) }

Characteristics

Voltage alternates between positive and negative values due to the two types of energy-storage elements. It's like a mass suspended on a spring.

The oscillation rate is fixed by Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \omega_d} , which is why it is called the damped radian frequency.

The oscillation amplitude decreases exponentially at a rate determined by Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha} , so it is called the damping factor.

Notice that when Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle R \neq 0} , there is Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha > 0} and the circuit is damped.