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 \( 8 \, \text{m/s}^2 \).
A cylindrical tube \(AB\) of length \(l\), closed at both ends, contains an ideal gas of \(1\) mol having molecular weight \(M\). The tube is rotated in a horizontal plane with constant angular velocity \(\omega\) about an axis perpendicular to \(AB\) and passing through the edge at end \(A\), as shown in the figure. If \(P_A\) and \(P_B\) are the pressures at \(A\) and \(B\) respectively, then (consider the temperature to be same at all points in the tube) 
As shown in the figure, radius of gyration about the axis shown in \(\sqrt{n}\) cm for a solid sphere. Find 'n'. 
When rod becomes horizontal find its angular velocity. It is pivoted at point A as shown. 
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The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.