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Figure 3 shows the basic principle of operation of a hand-operated salad spinner used to dry washed salads - AQA - A-Level Physics - Question 2 - 2017 - Paper 6

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Figure 3 shows the basic principle of operation of a hand-operated salad spinner used to dry washed salads. When handle A is turned the basket and its contents spin... show full transcript

Worked Solution & Example Answer:Figure 3 shows the basic principle of operation of a hand-operated salad spinner used to dry washed salads - AQA - A-Level Physics - Question 2 - 2017 - Paper 6

Step 1

Calculate the input torque.

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Answer

The input torque ( au) can be calculated using the formula:

τ=F×r\tau = F \times r

where:

  • F is the force applied (6.0 N)
  • r is the radius (36 mm = 0.036 m)

Substituting the values:

τ=6.0×0.036=0.216 N m\tau = 6.0 \times 0.036 = 0.216 \text{ N m}

Thus, the input torque is 0.216 N m.

Step 2

Deduce whether it is possible for the torque on gear C to be greater than that on gear B.

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Answer

Given that gear C rotates four times for every one revolution of gear B, the torque on gear C cannot exceed the torque on gear B if there are no losses. The torque relationship can be described as:

TC=4×TBT_C = 4 \times T_B

However, for the system to function within the limits of mechanical advantage, the power output cannot exceed the power input, hence the torque on gear C cannot be greater than on gear B.

Step 3

Calculate the moment of inertia of the basket about its axis of rotation.

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Answer

The moment of inertia (I) can be calculated using the formula for torque:

τ=Iα\tau = I \alpha

Given:

  • Torque on gear C (\tau) = 0.054 N m
  • Angular acceleration (\alpha) can be found from angular speed: [ \alpha = \frac{\Delta \omega}{\Delta t} = \frac{76 , \text{rad s}^{-1}}{2.1 \text{s}} \approx 36.19 , \text{rad s}^{-2}] Thus:
\Rightarrow I = \frac{0.054}{36.19} \approx 0.00149 \text{ kg m}^2$$.

Step 4

Explain with reference to angular impulse why a great force is put on the gear teeth.

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Answer

Angular Impulse relates to the change of angular momentum and is defined by:

J=ΔL=IΔωJ = \Delta L = I \cdot \Delta \omega

where:

  • J is the angular impulse
  • \Delta L is the change in angular momentum
  • I is the moment of inertia
  • \Delta \omega is the change in angular velocity.

A large force applied quickly changes the angular velocity, resulting in a high angular impulse that can exceed the limits of the gear teeth. The rapid deceleration necessitates a greater input force, potentially leading to damage of the plastic gear teeth due to stress beyond the material's tolerance.

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