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A particle of mass 5 kg is suspended from a fixed point by a light elastic string - Leaving Cert Applied Maths - Question 6 - 2014

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A particle of mass 5 kg is suspended from a fixed point by a light elastic string. The mass is set vibrating vertically with simple harmonic motion, making 4 oscilla... show full transcript

Worked Solution & Example Answer:A particle of mass 5 kg is suspended from a fixed point by a light elastic string - Leaving Cert Applied Maths - Question 6 - 2014

Step 1

(i) Find the constant of elasticity of the string.

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Answer

To find the elastic constant of the string, we start with the formula for the angular frequency of simple harmonic motion:

ω=2πf\omega = 2\pi f

Where:

  • ( f = 4 ) oscillations per second.

Substituting for ( \omega ):

ω=2π×4=8π\omega = 2\pi \times 4 = 8\pi

The formula for angular frequency in terms of the elastic constant ( k ) and mass ( m ) is:

ω=km\omega = \sqrt{\frac{k}{m}}

Here, substituting ( m = 5 , \text{kg} ):

8π=k58\pi = \sqrt{\frac{k}{5}}

Squaring both sides gives:

(8π)2=k5k=5(8π)2(8\pi)^2 = \frac{k}{5} \Rightarrow k = 5(8\pi)^2

Calculating ( k ):

k=5×64π23158.27N/mk = 5 \times 64\pi^2 ≈ 3158.27 \, \text{N/m}

Thus, the constant of elasticity is approximately 3158.27 N/m.

Step 2

(ii) Find the force required to stretch the string through 1.5 cm from its natural length.

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Answer

The force required to stretch the string can be calculated using Hooke's Law:

F=kxF = kx

Where:

  • ( k ≈ 3158.27 , \text{N/m} )
  • ( x = 1.5 , \text{cm} = 0.015 , \text{m} )

Substituting these values:

F=3158.27×0.01547.37NF = 3158.27 \times 0.015 ≈ 47.37 \, \text{N}

Thus, the force required to stretch the string through 1.5 cm is approximately 47.37 N.

Step 3

(i) If cos α = \( \frac{1}{4} \) find, in terms of d, the speed of the particle at the moment that the string touches the peg.

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Answer

Using the principle of conservation of energy, the total mechanical energy at the initial height will equal the total mechanical energy when the string touches the peg:

Initial potential energy:

PEinitial=mgh=mg(2dh)PE_initial = mgh = mg(2d - h)

Where ( h = 2d \cos(α) ). Substitute ( cos(α) = \frac{1}{4} ):

h=2d(14)=d2h = 2d(\frac{1}{4}) = \frac{d}{2}

Now substituting for height:

PEinitial=mg(2dd2)=mg(4dd2)=mg(3d2)PE_initial = mg(2d - \frac{d}{2}) = mg(\frac{4d - d}{2}) = mg(\frac{3d}{2})

At the point just before touching:

KE+PE=PEinitialKE + PE = PE_initial

So,

12mv2+mgd2=mg3d2\frac{1}{2}mv^2 + mg \frac{d}{2} = mg \frac{3d}{2}

Solving for ( v ):

v2=2g3d2gd2=3gdgd=2gdv^2 = 2g \frac{3d}{2} - g \frac{d}{2} = 3gd - gd = 2gd

Thus,

v=2gd4.233dv = \sqrt{2gd} ≈ 4.233 \sqrt{d}

Step 4

(ii) Find, in terms of m, the tension in the string when the particle reaches the same height as the peg.

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Answer

At the moment the particle reaches the same height as the peg, applying the forces:

Using the tension formula:

T=mgcos(45°)+mv2dT = mg \cos(45°) + \frac{mv^2}{d}

Since ( v^2 = 2g \frac{d}{2} - g \frac{d}{2} = gd ):

v2=gdv^2 = gd

Now substituting:

T=mgcos(45°)+m(2gd)dT = mg \cos(45°) + \frac{m(2gd)}{d}

So,

v2=2gd2gdv^2 = 2gd - \sqrt{2}gd

After simplifying:

T=mg12+mg=mg(12+1)T = mg \frac{1}{\sqrt{2}} + mg = mg \left(\frac{1}{\sqrt{2}} + 1\right)

This simplifies to yield:

T4.06NT ≈ 4.06 \, \text{N}

Thus, the tension in the string when the particle reaches the same height as the peg is approximately 4.06 N.

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