Problema 24-5
Source:
Adapted from Question 1 of the PUCRS II Electrical Circuits Test - 2019.
a) Determine the value of vc (t) for t > 0 knowing that the circuit is in steady state when the switch is in the position shown in
Figure 24-05.1 for t < 0 .
b) Graph the system response. Making R = 5 Ω, redo the graph and compare with the previous one.
Solution of the Problem 24-5
Item a
Note that for t < 0 we have two independent circuits in steady state. In this way, we can calculate
vc (0+) = 5 V and
iL (0+) = 20/10 = 2 A. We can also calculate the value of iR (0+) = (20 - 5)/10 = 1.5 A and, applying LKC to node a, we can determine the value of
ic (0+) = 1.5 - 2 = - 0.5 A. These are the initial conditions of the problem.
Note that in Figure 24-05.2, we have a parallel RLC circuit that is perfectly possible to be solved by applying the theory already studied.
Then, with the values provided by the problem, we can calculate the operating frequency of the circuit using eq. 24 - 06 and, we find:
ωo2 = 1 / L C = 1/ (2 x (1/20)) = 10 rad2/s2
We easily conclude that:
ωo = √10 rad/s
Now let's calculate the value of α of a parallel RLC circuit. Using eq. 24-05, we have:
α = 1/ (2 R C ) = 1 rad/s
Note that in this case, α < ωo, confirming an underdamped response. Therefore, the two roots of the characteristic equation are complex and the equation for vc (t) will be in the form of eq. 24-14 plus vf = 0. For clarity, below we repeat the equation.
eq. 24-14
Now we need to calculate the value of ωd, which is given by eq. 24-13. Then:
ωd = √ (10 - 1) = 3 rad/s
So the system response is:
vc (t ) = e- t ( B1 cos (3 t) + B2 sen (3 t) )
At this point it is necessary to discover the values of B1 and B2. To do this, we will use the initial conditions of the problem. Therefore, as we know that vc (0+) = 5 V and t = 0, substituting into the equation above we found that:
B1 = 5
And to calculate the value of B2, we will use the initial condition ic (0+ ) = 1.5 - 2 = - 0.5 A. Since ic is related to the first derivative of vc, then deriving
vc we find the relationship below:
dv(0
+) / dt =
i
c(0
+) / C =
- α B
1 + ω
d B
2
Therefore, performing numerical substitution, we find:
- 0,5/ (1/20) = - 5 + 3 B2
Solving this equation, we find the value of B2, or:
B2 = - 5/3
And now we can write the solution equation of the system, or:
vc (t ) = e- t ( 5 cos (3 t) - (5/3) sen (3 t) ) V
Item b
Note that, in Figure 24-05.3, the graph in blue represents the answer to the problem solved in item a. When we make R = 5 Ω, the system response is represented by the curve in red. In this case, we have α = 2 rad/s.
As α represents the damping factor of the circuit, observe that the response tends to steady state more quickly. So, when we decrease the value of R, we increase the value of α, making the circuit more stable, that is, less oscillating. There is a value of R where the circuit stops being underdamped and becomes critically damped. This fact happens when R = √10. Check!!!