d) The voltages \( V_{1} \) and \( V_{2} \) are represented by waveforms as follows \( V_{1}=9 \sin (\omega t) \) \( V_{2}=2 \cos (\omega t) \) If \( V_{3} \) is the sum of \( V_{1} \) and \( V_{2} \) such that \( V_{3}=V_{1}+V_{2} \) Find the expression of \( V_{3} \) in sine form \( V_{3}=R \sin (\omega t+\alpha) \) where \( \alpha \) is expressed in radians. Both figures to two decimal places. \( V_{3}=\square \sin (\omega t+\square) \) rks red s. submit part
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To find \( V_{3} \), we first need to combine \( V_{1} \) and \( V_{2} \). Rewrite \( V_{2} \) in sine form. This can be done using the identity \( \cos(\theta) = \sin\left(\theta + \frac{\pi}{2}\right) \). Substituting, we get: \[ V_{2} = 2 \cos(\omega t) = 2 \sin\left(\omega t + \frac{\pi}{2}\right) \] Now we can express \( V_{3} \): \[ V_{3} = V_{1} + V_{2} = 9 \sin(\omega t) + 2 \sin\left(\omega t + \frac{\pi}{2}\right) \] We can use the sine addition formula or phasor method to combine these two sine waves. The amplitude \( R \) and phase \( \alpha \) can be calculated as follows: 1. Convert the sine functions to their rectangular forms: \[ 9 \sin(\omega t) = 9j + 0 \] \[ 2 \cos(\omega t) = 2(0) + 2j \] 2. Now, add the phasors: \[ Z = 9 + 2j \] 3. The magnitude \( R \) can be found using Pythagorean theorem: \[ R = \sqrt{9^2 + 2^2} = \sqrt{81 + 4} = \sqrt{85} \approx 9.22 \] 4. The angle \( \alpha \) is calculated using: \[ \alpha = \tan^{-1}\left(\frac{2}{9}\right) \approx 0.2187 \, \text{radians} \] Therefore, the final expression for \( V_{3} \) in sine form is: \[ V_{3} = 9.22 \sin\left(\omega t + 0.22\right) \] So, \( V_{3} = 9.22 \sin(\omega t + 0.22) \).