Problem + Hard 55-8
Source: Adapted from Problem 4 - RLC 2008 Problem List IV - Discipline
Electrical Circuits of the School of Engineering - UFRGS - 2008 - Prof. doctor Valner Brusamarello.
In the circuit below, the voltmeter V measure 70 volts. In addition, the voltage E
is 30° behind Vab. Determine the magnitude and phase of the voltage source E, as well as the
value and nature of X. Also determine the value of Vab , I and the voltage Vca. Make one phasor diagram of the main voltages in the circuit.
Solution of the Problem + Hard 55-8
The two impedances that are in parallel can be determined and named as follows:
ZL = 5 + j 5√3 = 10 ∠60° Ω
ZC = 5√3 - j 5 = 10 ∠-30° Ω
The voltage phase Vab was not mentioned in the problem statement. Therefore, it is appropriate to take it as a reference, making Vab = Vab ∠0°. Thus, using this reference, one can calculate the currents
IL and IC. Then:
IL = Vab ∠0° / 10 ∠60° = (Vab /10 ) ∠-60°
IC = Vab ∠0° / 10 ∠-30° = (Vab /10 ) ∠30°
From the circuit it is verified that I = IL + IC. Note that IL and IC are 90° out of phase with each other. So it is possible to use the Pythagoras theorem to calculate I. Carrying out the calculation:
I = √2 (Vab ∠0° / 10 )∠-15°
Observing the circuit very carefully and taking into account the information given in the problem statement, it is possible to
build the phase diagram of the voltages and currents of interest for the solution of the problem. This diagram is shown in figure
below.
Note that the points of interest are marked on the circuit and on the graph above. From the circuit it is possible to calculate the impedance between points a-b when solving the parallel existing between these points. Calling this impedance
Zab and carrying out the calculation, we obtain:
Zab = 6.83 + j 1.83 = 5√2 ∠15° Ω
And the existing impedance between the points c-a and calling it Zca:
Zca = 1 - j = √2 ∠-45° Ω
Thus, the voltage between these points and calling it Vca is:
Vca = Zca I = √2 ∠-45° √2 (Vab ∠0° / 10 )∠-15°
Performing the calculate:
Vca = 0.2 Vab ∠-60°
Now it is necessary to calculate the voltage Vam. Note that this voltage is across the 5 ohms resistor where current flows IL. Soon:
Vam = 5 IL = 5 (Vab /10 ) ∠-60°
Performing the calculate:
Vam = 0.5 Vab ∠-60°
Note that the two calculated voltages are in phase (-60°), as shown in the graph above. The sum of these voltages is
exactly the same as the voltmeter reading V (70 volts). Thus, one can write:
V = Vca + Vam = 70
Substituting the numerical values calculated above and considering only the voltage modules Vca and
Vam, we have:
V =Vab ( 0.2 + 0.5 ) = 70
Now you can easily calculate the value of Vab, because:
Vab = 70 / 0.7 = 100∠0° V
With this data it is possible to calculate the value of Vca as requested in the problem statement, or:
Vca = 20∠-60° V
With the value of Vab it is possible to calculate the value of I, or:
I = 10√2∠-15° A
To proceed with the solution of the problem, it was decided to reduce the circuit showing the 4 ohms resistor with the
reactance X. Note that the point n is the junction of the two components. The figure on the side shows this configuration agreeing with the graph shown above. Note that all components are in series and current I flows through them.
It is possible to calculate the voltage across the 4 ohms resistor, which is the voltage Vnc = 4 I. making up to numerical substitution and calculating, we find:
Vnc = 40√2∠-15° = 56.56∠-15° V
Looking at the graph above, note that from the point n to the voltage E, what you have is the voltage on the element
X, which will be named Vx. This voltage must be 90° behind the I
(same phase as Vnc) so that the polygon closes at point E. Thus, it is evident that the element X is a capacitor.
Right now there are two unknowns to determine: the value of E and the value of Vx. Can be determined
graphically or analytically.
Graphically, we know the value of the voltage Vnc and the angle of -15° in relation to Vab . At the point n, draw a line perpendicular to Vnc until you find the phasor E, which in turn has a -30° angle with respect to Vab. Check that Vx has the same value as
Vnc. As the two components (resistor and capacitor) are in series and carry the same current,
it is concluded that:
|R| = |X| = 4 Ω
Analytical Calculation
We will present two different ways to solve the problem analytically.
Alternative I
To find the value of E we know that Vnc = 56.56 ∠-15°. From the graph above we see that
Vnc makes an angle of 45° with the voltage phasor VEc . Then, we conclude that
|Vx| = |Vnc|. In this way, the phasor Vx closes the right triangle c-n-E. Soon,
we can easily calculate the value of VEc, because:
|VEc| = √ (Vnc2 + Vx2)
Substituting for numerical values, we have:
|VEc| = √ (56.562 + 56.562) = 80 V
Notice from the graph that VEc is in phase with Vac. So we can add the two
phasors and obtain the value of VEa = 80 + 20 = 100 V. Now we know two sides of the triangle b-a-E, that is,
Vab and VEa. And we know the angle
between them which is 120°. With that and using the law of cosines we can calculate the value of E.
E = √ (VEa2 + Vab2 - 2 VEa Vab cos 120°)
ubstituting for numerical values, we have:
E = √ (1002 + 1002 - 2 x 100 x 100 cos 120°)
Performing the calculate, we have:
E = 173.2 ∠-30° V
Note that we added the angle of E, as the problem statement states that E is lagging by 30° in
with respect to Vab and we define at the beginning of the problem solution
Vab = Vab∠ 0°.
Alternativae II
For an analytical calculation, you must work with the line equation. Remembering that the reduced equation of the line is given by y = a x + b, and that a = tan φ, where φ is the angle that the line makes with the reference line (in this case, Vab). For the voltage Vnc, it is known that the angle is -15°. Consequently a = tan (-15°) = - 0.268. And to find the equation of the line, you must know a point on the line. Using the point n, xn and yn are calculated as follows:
xn = Vab + Vca cos (-60°) + Vnc cos (-15°) = 164.64
yn = Vca sen (-60°) + Vnc sen (-15°) = -32
Ready. Knowing a point on the line and its angular coefficient, it is possible to determine the equation using the relationship below:
y - yn = a (x - xn ) ⓵
Substituting for numeric values and performing the calculation:
y = - 0.268 x + 12.12
As it is known that Vx is perpendicular to Vnc, the next step is to find the equation of the line perpendicular to the Vnc passing through the point (xn , yn ) . So that two lines are perpendicular, their angular coefficients must obey the relation ap = - (1 / a). So, it is determined that
the value of the angular coefficient of the perpendicular line is ap = 3.73. Returning to the relationship
⓵, find the equation of the line perpendicular to Vnc, or:
yp = 3.73 xp - 646.33 ⓶
To determine the values of E and Vx, you must know the equation of the line E. like this line
passes through the origin, just know its angular coefficient , or aE = tan (-30°) = - 0.577. So the equation is:
yE = - 0.577 xE ⓷
Now that you know the equation of the two lines of interest, you must determine the point where they intersect. Then,
subtracting ⓷ from ⓶ and remembering that in point of intersection yE = yp and xE = xp, you get
0 = 4.307 xE - 646.33
From this relation one obtains the point of intersection of E and Vx. Like this:
xE = 150 and yE = - 86.6
For the calculation of yE, the equation ⓷ was used. With these data, one can calculate the length of the phasor E. As it passes through the origin, then:
|E| = √ [1502 + (- 86.6)2]
Thus, the phasor E is:
E = 173.2 ∠-30° volts
Finally, an analytical calculation of X can be carried out, remembering that Vx = 56.56 ∠-105°. Soon
X = Vx / I = 56.56 ∠-105° / 14.14∠-15°
Carrying out the calculation, we find:
X = 4∠-90° = -j4 Ω
Note that, analytically, it follows that X is a capacitor.