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0.2.1 State one function of a flywheel - AQA - A-Level Physics - Question 2 - 2018 - Paper 6

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0.2.1 State one function of a flywheel. 0.2.2 A student does an experiment to determine the frictional torque acting at the bearings of a steel flywheel. The flywhe... show full transcript

Worked Solution & Example Answer:0.2.1 State one function of a flywheel - AQA - A-Level Physics - Question 2 - 2018 - Paper 6

Step 1

State one function of a flywheel.

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Answer

One function of a flywheel is to smooth out fluctuations in rotational speed.

Step 2

Show that the frictional torque is about $7 \times 10^{-4} \text{ N m}$.

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Answer

To find the frictional torque, we can use the change in gravitational potential energy and equate it to the work done against the torque.

  1. Calculate the decrease in potential energy:

    ΔPE=mgh=(0.020 kg)(9.81 m/s2)(0.075 m)(1cos(3.00))\Delta PE = mgh = (0.020 \text{ kg})(9.81 \text{ m/s}^2)(0.075 \text{ m}) (1 - \cos(3.00)) where h is the vertical drop of the magnet. Since the angle moved is 3.00 radians, the height change can be calculated using the radius:

    h=0.075(1cos(3.00 rad))h = 0.075(1 - \cos(3.00 \text{ rad}))

  2. The work done is equal to the torque (τ\tau) times the angle moved in radians:

    W=τθW = \tau \cdot \theta

  3. Setting the loss in potential energy equal to the work done:

    ΔPE=τθ\Delta PE = \tau \cdot \theta

  4. Rearranging gives:

    τ=ΔPEθ7×104 N m\tau = \frac{\Delta PE}{\theta} \approx 7 \times 10^{-4} \text{ N m}

Step 3

Determine the moment of inertia of the flywheel about its axis of rotation.

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Answer

We can determine the moment of inertia (II) using the relationship involving torque and angular deceleration:

  1. The angular displacement (θ\theta) is given in rotations, so convert to radians:

    θ=73 rotations×2π rad/rotation=459.7 rad\theta = 73 \text{ rotations} \times 2\pi \text{ rad/rotation} = 459.7 \text{ rad}

  2. Calculate the average angular speed (ω\omega):

    ωavg=ωi+ωf2=25.0+02=12.5 rad/s\omega_{avg} = \frac{\omega_i + \omega_f}{2} = \frac{25.0 + 0}{2} = 12.5 \text{ rad/s}

  3. Use the formula for angular deceleration (α\alpha) as follows:

    α=ΔωΔt\alpha = \frac{\Delta \omega}{\Delta t}

    Where Δω\Delta \omega is the change in angular speed and Δt\Delta t is the time taken. Since the time is not provided, we need to assume a constant torque and calculate using the average speed.

  4. Finally apply the relationship between torque, moment of inertia, and angular acceleration:

    τ=Iα\tau = I \cdot \alpha

  5. From this expression, rearranging gives:

    I=ταI = \frac{\tau}{\alpha}

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