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IBDP Physics HL Paper 1B- Data-Based Question- New Syllabus

Question

A flywheel consists of a solid disk of mass \(5.00\,\text{kg}\) mounted on a light radial axle of negligible mass. The disk has radius \(R = 6.00\,\text{cm}\) and the axle has radius \(r = 1.20\,\text{cm}\).
A thin string is wrapped around the axle and pulled vertically by an electric motor, producing a tension force \(T\). The diagram shows the forces acting on the flywheel, where \(W\) is the weight and \(N\) is the normal reaction from the support.
The moment of inertia of the flywheel about its axis is given by \( I = \frac{1}{2}MR^2 \).
Initially, the flywheel is at rest. At time \(t=0\), the motor is switched on and the torque \(\Gamma\) applied by the string varies with time as shown.
At \(t = 5.00\,\text{s}\), the string becomes fully unwound and disconnects from the flywheel, which continues to rotate.
(a) State the torque provided by the force \(W\) about the axis of the flywheel. [1]
(b)(i) Identify the physical quantity represented by the area under the torque–time graph. [1]
(b)(ii) Show that the angular velocity of the flywheel at \(t = 5.00\,\text{s}\) is \(200\,\text{rad s}^{-1}\). [2]
(b)(iii) Calculate the maximum tension in the string.
(c)(i) The flywheel is in translational equilibrium. Distinguish between translational equilibrium and rotational equilibrium.
(c)(ii) At \(t = 5.00\,\text{s}\), the flywheel rotates with angular velocity \(200\,\text{rad s}^{-1}\). The support bearings exert a constant frictional torque. The flywheel comes to rest after \(8.00 \times 10^3\) revolutions. Calculate the magnitude of the frictional torque. [3]
▶️ Answer/Explanation

(a)
The line of action of the weight passes through the axis of rotation, so it produces no turning effect.
\( \boxed{0\,\text{N m}} \)

(b)(i)
The area under a torque–time graph represents the change in angular momentum (angular impulse).

(b)(ii)
Area under the graph \(= \Delta L = 1.80\,\text{kg m}^2\text{s}^{-1}\).
Using \( \Delta L = I\omega \):
\( 1.80 = \left(\frac{1}{2} \times 5.00 \times 0.060^2\right)\omega \)
\( \omega = 200\,\text{rad s}^{-1} \).

(b)(iii)
Maximum torque \( \Gamma_{\max} = Tr \).
\( T = \dfrac{0.40}{0.012} = 33.3\,\text{N} \).

(c)(i)
Translational equilibrium occurs when the resultant force on a body is zero.
Rotational equilibrium occurs when the resultant torque on a body is zero.

(c)(ii)
The angular displacement before stopping is \( \theta = 2\pi \times 8000 \).
Using \( 0 = \omega^2 + 2\alpha\theta \):
\( \alpha = -0.398\,\text{rad s}^{-2} \).
Frictional torque: \( \tau = I\alpha = 0.398 \times \left(\frac{1}{2} \times 5.00 \times 0.060^2\right) \).
\( \boxed{3.58 \times 10^{-3}\,\text{N m}} \).

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