Angular speed ($\omega$) = $\frac{\text{Angular displacement}}{\text{time}}$
For the second hand: $\omega_1 = \frac{2\pi}{60}$ rad/s x1 = ω1 × 60 = 2π rad
For the minute hand: $\omega_2 = \frac{2\pi}{3600}$ rad/s x2 = ω2 × 60 = $\frac{2\pi}{60}$ rad
For the hour hand:
$\omega_3 = \frac{2\pi}{3600 \times 12}$ rad/s
x3 = ω3 × 60 = $\frac{2\pi}{720}$ rad
Thus, $\frac{\omega_1}{x_1} = \frac{\omega_2}{x_2} = \frac{\omega_3}{x_3} = \frac{1}{60} = k$
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is:
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is:

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The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.