To solve the problem, we first determine the angular acceleration α of the pulley using the relationship between torque τ and moment of inertia — τ = Iα. The tangential force F is given as a function of time t: F = (12t – 3t2) N. Since torque τ is related to the force and radius r by τ = Fr, we have: τ = (12t - 3t2) × 1.5 = 18t - 4.5t2 Nm.
Given that I = 4.5 kg m2, the angular acceleration is computed as:α = τ/I = (18t - 4.5t2)/4.5 = 4t - t2 rad/s2.
To find when the direction reverses, set the angular velocity ω to zero and integrate the expression for α: ω = ∫(4t - t2)dt = 2t2 - (t3/3).
The initial angular velocity is zero, and we solve for t when ω again becomes zero:2t2 - (t3/3) = 0.
Factor the equation:t2(2 - t/3) = 0.
Thus, solutions are t=0 or t=6. For t=0, it’s the initial condition. We use t=6. Calculate the angular displacement θ by integrating:θ = ∫ω dt = ∫(2t2 - t3/3) dt = (2t3/3) - (t4/12) |60.
Evaluate the definite integral:θ = [(2×63/3) - (64/12)] - [0] = (2×216/3) - (1296/12).
This simplifies to:θ = 144 - 108 = 36 radians.
The number of full rotations N is:N = θ/2π = 36/2π = 18/π.
This gives N = K/π, and thus K = 18. The computed value falls within the provided range of 18,18, confirming the correctness of the value.
The correct answer is 18

I = 4.5 kg m2
\(FR=Iα\)
\(α=\frac{(12t–3t^2)×1.5}{4.5}=4t−t^2\)
\(w=∫αdt=2t^2–\frac{t^3}{3} \)
w=0
\(⇒t^2(2–\frac{t}{3})0 \)
t=6 sec
\(θ=∫_{0}^{6}[2^t2–\frac{t^3}{3}]dt=[\frac{2t^3}{3}–\frac{t^4}{12}]_{0}^{6}\)
\(=[\frac{2}{3}×6^3–\frac{6^4}{12}]=36\)
\(n=\frac{36}{2π}\)
\(=\frac{18}{π}\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,



What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: