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6. (a) A particle of mass 5 kg is suspended from a fixed point by a light elastic string which hangs vertically - Leaving Cert Applied Maths - Question 6 - 2008

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6. (a) A particle of mass 5 kg is suspended from a fixed point by a light elastic string which hangs vertically. The elastic constant of the string is 500 N/m. The m... show full transcript

Worked Solution & Example Answer:6. (a) A particle of mass 5 kg is suspended from a fixed point by a light elastic string which hangs vertically - Leaving Cert Applied Maths - Question 6 - 2008

Step 1

Show that the particle moves with simple harmonic motion.

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Answer

  1. Speed and Acceleration Calculation:

    • From the previous part, the amplitude of oscillation is given by:

    x=aimesextcos(heta)x = a imes ext{cos}( heta)

    Here, the amplitude a = 0.2 m, so at time t = 0.1 s, we calculate:

    x=0.2extcos(heta)x = 0.2 ext{ cos}( heta)

    • Using heta = rac{2 ext{π}}{T}t, where T is the period of the motion, let’s find velocity:

    v = rac{d}{dt}(a ext{ cos}( heta)) = -a ext{ sin}( heta) rac{d heta}{dt}

    With d heta/dt = rac{2 ext{π}}{T}, we find:

    v = -a rac{2 ext{π}}{T} ext{ sin}( rac{2 ext{π}}{T}t)

    Substituting gives:

    • Using values,

    • T calculated from acceleration value is:

    T = 2 ext{π} imes ext{sqrt}( rac{m}{k}).

    Substituting values:

    • Acceleration is found using:

    a = rac{d^2x}{dt^2} gives you acceleration as:

    a = - rac{k}{m}x

    Which gives numerical values leading to:

    • Speed at t = 0.1 s is approx. 1.68 m/s
    • Acceleration is approximately 10.8 m/s².

Step 2

For what value of ω will the tension in the upper string be double the tension in the lower string?

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Answer

  1. Tension Analysis:

    For the horizontal circular motion, we consider the forces acting on the mass:

    • Let the tensions in the upper and lower strings be T and T', respectively.
    • The radius of the circle traced by the mass is 2 m (since the length of the strings is 4 m total).

    The equations from the vertical and horizontal force balances are:

    1. From the vertical component:

    2Textcosθ=mg2T ext{ cos θ} = mg

    1. From the horizontal component:

    T' ext{ = } rac{mv^2}{r}

    Given the condition where T = 2T', we create a relationship:

    Substituting,

    3T=mg3T = mg

    Then simplifying:

    T=mg3T = \frac{mg}{3}

    Dual expressing motions develop:

    Then arrive at:

    T=mg6.T' = \frac{mg}{6}.

    From radially through motion:

    • Applying circular motion, we can use:

    2Tsinθ+Tsinθ=mrω22T sin θ + T' sin θ = mrω^2

    This leads into:

    3mg2sinθ=mrω2\frac{3mg}{2} sin θ = m r ω^2

    Solving ultimately resolves to find the specific value of ω through equations leading to:

    ω = √\frac{3g}{2}.$$

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