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State Newton's laws of motion - Leaving Cert Physics - Question 6 - 2009

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State Newton's laws of motion. Show that F = ma is a special case of Newton’s second law. A skateboarder with a total mass of 70 kg starts from rest at the top of ... show full transcript

Worked Solution & Example Answer:State Newton's laws of motion - Leaving Cert Physics - Question 6 - 2009

Step 1

State Newton's laws of motion.

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Answer

Newton's laws of motion can be summarized as follows:

  1. An object remains at rest or in uniform motion unless acted upon by a net external force.
  2. The force acting on an object is equal to the mass of the object multiplied by its acceleration (F = ma).
  3. For every action, there is an equal and opposite reaction.

Step 2

Show that F = ma is a special case of Newton’s second law.

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Answer

To demonstrate that F = ma is a special case of Newton's second law, we start with the definition of force as the rate of change of momentum:

F=dpdtF = \frac{dp}{dt}

Where momentum (p) is defined as:

p=mvp = mv

Taking the derivative:

dpdt=d(mv)dt\frac{dp}{dt} = \frac{d(mv)}{dt}

Assuming mass (m) is constant, this simplifies to:

F=mdvdtF = m \frac{dv}{dt}

Since acceleration (a) is defined as:

a=dvdta = \frac{dv}{dt}

We can conclude:

F=maF = ma

Thus, F = ma is indeed a special case of Newton’s second law.

Step 3

the average acceleration of the skateboarder on the ramp.

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Answer

To calculate the average acceleration (a) of the skateboarder, we use the formula:

v2=u2+2asv^2 = u^2 + 2as

Where:

  • Final velocity (v) = 12.2 m/s
  • Initial velocity (u) = 0 (starts from rest)
  • Distance (s) = 25 m

Substituting the values:

12.22=0+2a(25)12.2^2 = 0 + 2a(25)

This simplifies to:

148.84=50a148.84 = 50a

Thus,

a=148.8450=2.9768 m/s22.98 m/s2a = \frac{148.84}{50} = 2.9768\ m/s^2 \approx 2.98\ m/s^2

Step 4

the component of the skateboarder’s weight that is parallel to the ramp.

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Answer

The weight of the skateboarder (W) is given by:

W=mgW = mg

Where:

  • m = 70 kg (mass of skateboarder)
  • g = 9.8 m/s² (acceleration due to gravity)

Calculating the weight:

W=70 kg×9.8 m/s2=686 NW = 70\ kg \times 9.8\ m/s^2 = 686\ N

The component of the weight that acts parallel to the ramp is:

Wparallel=Wsin(θ)W_{parallel} = W \sin(\theta)

Substituting values:

Wparallel=686 N×sin(20°)686×0.342=234.41 NW_{parallel} = 686\ N \times \sin(20°) \approx 686 \times 0.342 = 234.41\ N

Step 5

the force of friction acting on the skateboarder on the ramp.

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Answer

The net force acting on the skateboarder on the ramp can be found using Newton's second law:

Fnet=ma=70 kg×2.98 m/s2=208.6 NF_{net} = ma = 70\ kg \times 2.98\ m/s^2 = 208.6\ N

The force of friction (F_f) is found by:

Ff=WparallelFnetF_f = W_{parallel} - F_{net}

Substituting the values:

Ff=234.41 N208.6 N=25.81 NF_f = 234.41\ N - 208.6\ N = 25.81\ N

Step 6

What is the initial centripetal force acting on him?

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Answer

The centripetal force (F_c) required to keep the skateboarder moving in a circle is given by:

Fc=mv2rF_c = \frac{mv^2}{r}

Where:

  • m = 70 kg
  • v = 10.5 m/s (speed)
  • r = 10 m (radius)

Substituting these values:

Fc=70 kg×(10.5)210=70×110.2510=771.75 NF_c = \frac{70\ kg \times (10.5)^2}{10} = \frac{70 \times 110.25}{10} = 771.75\ N

Step 7

What is the maximum height that the skateboarder can reach?

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Answer

To find the maximum height (h), we use the conservation of energy principle, where kinetic energy (KE) is converted into potential energy (PE):

KE=PEKE = PE

12mv2=mgh\frac{1}{2}mv^2 = mgh

Therefore,

12(70) times(10.5)2=70gh\frac{1}{2}(70)\ times (10.5)^2 = 70gh

Cancelling mass (m) gives:

12v2=gh\frac{1}{2}v^2 = gh

Substituting in values:

12(10.5)2=9.8h\frac{1}{2}(10.5)^2 = 9.8h

Thus:

110.2519.6=h5.63 m\frac{110.25}{19.6} = h \approx 5.63 \ m

Step 8

Sketch a velocity-time graph to illustrate his motion.

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Answer

The velocity-time graph of the skateboarder's motion would show a steady increase in velocity as he accelerates down the ramp, reaching a peak velocity of 12.2 m/s at the bottom. After that, the velocity remains constant at 10.5 m/s as he transitions into the circular ramp.

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