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
\(θ=∫_{0}^{6}[2^t2–\frac{t^3}{3}]dt=[\frac{2t^3}{3}–\frac{t^4}{12}]_{0}^{6}\)
\(=[\frac{2}{3}×6^3–\frac{6^4}{12}]=36\)
\(n=\frac{36}{2π}\)
\(=\frac{18}{π}\)
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

Two point charges 2q and q are placed at vertex A and centre of face CDEF of the cube as shown in figure. The electric flux passing through the cube is : 
Suppose there is a uniform circular disc of mass M kg and radius r m shown in figure. The shaded regions are cut out from the disc. The moment of inertia of the remainder about the axis A of the disc is given by $\frac{x{256} Mr^2$. The value of x is ___.

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: