The instantaneous voltages at three terminals marked X, Y and Z are given by
Vx = V0 sin ωt
Vy = V0 \((ωt+\frac{2\pi}{3})\) and
Vz = V0 sin \((ωt+\frac{4\pi}{3})\)
An ideal voltmeter is configured to read rms value of the potential difference between its terminals. It is connected between points X and Y and then between Y and Z. The reading(s) of the voltmeter will be
(A) \(V^{rms}_{xy}\) \(V_ 0 \sqrt{\frac{3}{2}}\)
(B) \(V^{rms}_{yz}\) \(V_ 0\sqrt{\frac{1}{2}}\)
(C) \(V^{rms}_{xy}\) V0
(D) independent of the choice of the two terminals