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During the discus event, Ashton swings a discus of mass 2.0 kg in uniform circular motion - Leaving Cert Physics - Question 6 - 2018

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During the discus event, Ashton swings a discus of mass 2.0 kg in uniform circular motion. The radius of orbit of the discus is 1.2 m and the discus has a velocity o... show full transcript

Worked Solution & Example Answer:During the discus event, Ashton swings a discus of mass 2.0 kg in uniform circular motion - Leaving Cert Physics - Question 6 - 2018

Step 1

(i) Derive an expression to show the relationship between the radius, velocity and angular velocity of an object moving in uniform circular motion.

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Answer

In uniform circular motion, the relationship between the radius (r), tangential velocity (v), and angular velocity (ω) is given by:

ω=vrω = \frac{v}{r}

This expression shows that angular velocity is the ratio of linear velocity to radius. Thus, angular velocity increases with an increase in velocity or a decrease in radius.

Step 2

(ii) Calculate the angular velocity of the discus immediately prior to its release.

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Answer

Using the formula derived in part (i):

ω=vr=20.4 m s11.2 m=17 rad s1ω = \frac{v}{r} = \frac{20.4 \text{ m s}^{-1}}{1.2 \text{ m}} = 17 \text{ rad s}^{-1}

Therefore, the angular velocity is 17 rad s⁻¹.

Step 3

(iii) Calculate the centripetal force acting on the discus just before Ashton releases it.

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Answer

The centripetal force (F) can be calculated using the formula:

F=mv2rF = m \frac{v^2}{r}

Substituting the given values:

F=2.0extkg×(20.4extms1)21.2extm=693.6extNF = 2.0 ext{ kg} \times \frac{(20.4 ext{ m s}^{-1})^2}{1.2 ext{ m}} = 693.6 ext{ N}

Thus, the centripetal force acting on the discus just before release is 693.6 N towards the centre.

Step 4

(i) his velocity in the horizontal direction.

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Answer

To find the horizontal component of the velocity ( v_h), we use:

vh=vcos(θ)v_h = v \cos(\theta)

Substituting the known values:

vh=10.9 m s1cos(43)7.97 m s1v_h = 10.9 \text{ m s}^{-1} \cos(43^\circ) \approx 7.97 \text{ m s}^{-1}

Step 5

(ii) the length of the jump.

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Answer

The length of the jump (s) can be calculated using:

s=vt=(vh)(t)=(7.97 m s1)(1.03 s)8.21extms = vt = (v_h)(t) = (7.97 \text{ m s}^{-1})(1.03 \text{ s}) \approx 8.21 ext{ m}

Step 6

(i) State the principle of conservation of energy.

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Answer

The principle of conservation of energy states that energy cannot be created or destroyed; it can only be transformed from one form to another.

Step 7

(ii) What is meant by the centre of gravity of a body?

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Answer

The centre of gravity of a body is the point at which the weight of that body acts, assuming uniform gravitational field conditions.

Step 8

(iii) what is the maximum height above the ground to which he can raise his centre of gravity?

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Answer

Using the conservation of energy principles, the maximum height can be calculated as follows:

mgh=gain in potential energy=loss in kinetic energymg h = \text{gain in potential energy} = \text{loss in kinetic energy}

Substituting the relevant values, we set the potential energy gain equal to the kinetic energy lost:

After solving the equations, the maximum height reached by Ashton's centre of gravity is:

h=4.26+0.98=5.24extmh = 4.26 + 0.98 = 5.24 ext{ m}

Step 9

(iv) Draw a diagram to show any forces acting on Ashton when he is at his highest point.

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Answer

Draw a free-body diagram showing forces acting on Ashton at his highest point:

  • Weight acting downward due to gravity
  • Any additional supporting force, if applicable Label the downward force as 'Weight', pointing towards the ground.

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