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The fly-press shown in Figure 1 is used by a jeweller to punch shapes out of a thin metal sheet - AQA - A-Level Physics - Question 1 - 2019 - Paper 6

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The fly-press shown in Figure 1 is used by a jeweller to punch shapes out of a thin metal sheet. The frame holds a screw and punch. Two arms are attached to the scr... show full transcript

Worked Solution & Example Answer:The fly-press shown in Figure 1 is used by a jeweller to punch shapes out of a thin metal sheet - AQA - A-Level Physics - Question 1 - 2019 - Paper 6

Step 1

Calculate the moment of inertia of the rotating parts about the axis of rotation.

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Answer

The rotational kinetic energy (KE) is given by the formula:

KE=12Iω2KE = \frac{1}{2} I \omega^2

Where:

  • (I) is the moment of inertia
  • (\omega) is the angular velocity in radians per second.

First, we convert the angular speed:

ω=2.9 rev s1×2π rad=2.9×2×3.14 rad s1=18.224 rad s1\omega = 2.9 \text{ rev s}^{-1} \times 2\pi \text{ rad} = 2.9 \times 2 \times 3.14 \text{ rad s}^{-1} = 18.224 \text{ rad s}^{-1}

Now substituting into the kinetic energy formula:

10.3=12I(18.224)210.3 = \frac{1}{2} I (18.224)^2

Solving for (I):

I=10.3×2(18.224)20.0614kg m2I = \frac{10.3 \times 2}{(18.224)^2} \approx 0.0614 \, \text{kg m}^2

Step 2

Explain why the moment of inertia of the screw, punch and arms about the axis of rotation is much smaller than the moment of inertia of the steel balls about the same axis.

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Answer

The moment of inertia depends on the distribution of mass relative to the axis of rotation. The screw, punch, and arms have their mass concentrated closer to the axis of rotation, leading to a lower moment of inertia. In contrast, the steel balls are further away from this axis, resulting in a higher moment of inertia. Thus, the more mass is distributed away from the axis, the larger the moment of inertia.

Step 3

Determine the angular deceleration.

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Answer

We can use the kinematic equation for angular motion:

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

Where:

  • (\Delta \omega = 0 - 2.9{ rev s}^{-1} = -2.9{ rev s}^{-1})
  • (\Delta t = 89 ms = 0.089 s)

Converting (\Delta \omega) to radians:

Δω=2.9×2π=18.224 rad s1\Delta \omega = -2.9 \times 2\pi = -18.224 \text{ rad s}^{-1}

Now substituting into the equation:

α=18.2240.089204.77rad s2\alpha = \frac{-18.224}{0.089} \approx -204.77 \, \text{rad s}^{-2}

Step 4

Determine the angle turned through by the rotating parts.

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Answer

Using the formula for angular displacement:

θ=ωt+12αt2\theta = \omega t + \frac{1}{2} \alpha t^2

Substituting the known values:

  • Initial angular velocity, (\omega = 18.224 , \text{rad s}^{-1})
  • Time, (t = 0.089 , s)
  • Angular acceleration, (\alpha = -204.77 , \text{rad s}^{-2})

We have:

θ=18.224×0.089+12×(204.77)×(0.089)2\theta = 18.224 \times 0.089 + \frac{1}{2} \times (-204.77) \times (0.089)^2

Calculating that gives:

θ1.6230.80450.8185extrad\theta \approx 1.623 - 0.8045 \approx 0.8185 \, ext{rad}

Step 5

Deduce which of these would produce the greater increase in stored energy.

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Answer

The stored energy (E) in the system is related to the moment of inertia and angular velocity:

E=12Iω2E = \frac{1}{2} I \omega^2

If we increase (y) by 15% without changing (R), it will result in a decrease of torque producing less energy than increasing (R) by 15% without changing (y). This is because the effective distance from the axis increases significantly when increasing the radius, thus leading to a greater increase in stored energy. Therefore, increasing (R) by 15% will produce the greater increase in stored energy.

Step 6

Which of the following is the SI unit for angular impulse?

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Answer

The SI unit for angular impulse is N s. Thus, the correct option is:

  • N s

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