Solveeit Logo

Question

Question: The value of current in the circuit shown are $I_1 = 2 \sin wt$ A and $I_2 = 4 \sin (wt + \frac{\pi}...

The value of current in the circuit shown are I1=2sinwtI_1 = 2 \sin wt A and I2=4sin(wt+π3)I_2 = 4 \sin (wt + \frac{\pi}{3}) A. The current supplied by the source is 2αsin(wt+θ)2\sqrt{\alpha} \sin(wt + \theta) A, where tanθ=β2\tan \theta = \frac{\sqrt{\beta}}{2}. Find α+β\alpha + \beta

Answer

10

Explanation

Solution

The problem involves finding the sum of two sinusoidal currents in parallel branches to determine the total current supplied by the source. We will use the phasor method for adding AC currents.

Given currents are:

  1. I1=2sinwtI_1 = 2 \sin wt A
  2. I2=4sin(wt+π3)I_2 = 4 \sin (wt + \frac{\pi}{3}) A

The total current supplied by the source is I=I1+I2I = I_1 + I_2. We can represent these currents as phasors: I1I_1 has an amplitude I1m=2I_{1m} = 2 A and a phase angle ϕ1=0\phi_1 = 0 radians. In rectangular form: I1=2cos0+j2sin0=2+j0I_1 = 2 \cos 0^\circ + j 2 \sin 0^\circ = 2 + j0

I2I_2 has an amplitude I2m=4I_{2m} = 4 A and a phase angle ϕ2=π3\phi_2 = \frac{\pi}{3} radians (or 6060^\circ). In rectangular form: I2=4cos60+j4sin60I_2 = 4 \cos 60^\circ + j 4 \sin 60^\circ We know cos60=12\cos 60^\circ = \frac{1}{2} and sin60=32\sin 60^\circ = \frac{\sqrt{3}}{2}. I2=4(12)+j4(32)=2+j23I_2 = 4 \left(\frac{1}{2}\right) + j 4 \left(\frac{\sqrt{3}}{2}\right) = 2 + j 2\sqrt{3}

Now, add the currents in rectangular form to find the total current II: I=I1+I2=(2+j0)+(2+j23)I = I_1 + I_2 = (2 + j0) + (2 + j 2\sqrt{3}) I=(2+2)+j(0+23)I = (2+2) + j (0 + 2\sqrt{3}) I=4+j23I = 4 + j 2\sqrt{3}

To express the total current in the form Imsin(wt+θ)I_m \sin(wt + \theta), we need to convert II from rectangular form (X+jYX + jY) to polar form (ImθI_m \angle \theta). The amplitude ImI_m is the magnitude of the complex number: Im=X2+Y2I_m = \sqrt{X^2 + Y^2} Im=42+(23)2I_m = \sqrt{4^2 + (2\sqrt{3})^2} Im=16+(4×3)I_m = \sqrt{16 + (4 \times 3)} Im=16+12I_m = \sqrt{16 + 12} Im=28I_m = \sqrt{28} Im=4×7=27I_m = \sqrt{4 \times 7} = 2\sqrt{7} A

The phase angle θ\theta is given by: tanθ=YX\tan \theta = \frac{Y}{X} tanθ=234\tan \theta = \frac{2\sqrt{3}}{4} tanθ=32\tan \theta = \frac{\sqrt{3}}{2}

So, the total current is I=27sin(wt+θ)I = 2\sqrt{7} \sin(wt + \theta) A, where tanθ=32\tan \theta = \frac{\sqrt{3}}{2}.

The problem states that the current supplied by the source is 2αsin(wt+θ)2\sqrt{\alpha} \sin(wt + \theta) A, where tanθ=β2\tan \theta = \frac{\sqrt{\beta}}{2}.

By comparing the amplitude expressions: 2α=272\sqrt{\alpha} = 2\sqrt{7} α=7\sqrt{\alpha} = \sqrt{7} α=7\alpha = 7

By comparing the expressions for tanθ\tan \theta: β2=32\frac{\sqrt{\beta}}{2} = \frac{\sqrt{3}}{2} β=3\sqrt{\beta} = \sqrt{3} β=3\beta = 3

Finally, we need to find α+β\alpha + \beta: α+β=7+3=10\alpha + \beta = 7 + 3 = 10