A particle at the periphery of a rotating object will have both radial and tangential acceleration. Let's calculate both accelerations step by step.
The tangential acceleration \( a_t \) is given by:
\(a_t = R \alpha = 0.5 \times 2 = 1 \, \text{m/s}^2\)
The angular velocity \( \omega \) is calculated using the formula:
\(\omega = \omega_0 + \alpha t\)
Substitute the values:
\(\omega = 0 + 2 \times 2 = 4 \, \text{rad/sec}\)
The centripetal acceleration \( a_c \) is given by:
\(a_c = \omega^2 R = (4)^2 \times 0.5 = 16 \times 0.5 = 8 \, \text{m/s}^2\)
The total acceleration \( a_{\text{total}} \) is the vector sum of tangential and centripetal accelerations, calculated as:
\(a_{\text{total}} = \sqrt{a_t^2 + a_c^2} = \sqrt{1^2 + 8^2} \approx 8 \, \text{m/s}^2\)
The total acceleration of the particle is approximately \( 8 \, \text{m/s}^2 \).
The maximum speed of a boat in still water is 27 km/h. Now this boat is moving downstream in a river flowing at 9 km/h. A man in the boat throws a ball vertically upwards with speed of 10 m/s. Range of the ball as observed by an observer at rest on the river bank is _________ cm. (Take \( g = 10 \, {m/s}^2 \)).
A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec: 