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A uniform wire ABC is bent at right angles at B - Leaving Cert Applied Maths - Question 7 - 2012

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A uniform wire ABC is bent at right angles at B. When it is suspended from B the parts AB and BC make angles of 30° and 60° respectively with the vertical. If the m... show full transcript

Worked Solution & Example Answer:A uniform wire ABC is bent at right angles at B - Leaving Cert Applied Maths - Question 7 - 2012

Step 1

a) If the mass per unit length of the wire is m and |AB| = h |BC| find the value of h.

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Answer

To find the value of h, we start by setting up the equilibrium equations for the wire suspended at angles of 30° and 60°. The lengths of the segments are given by relationships involving trigonometric functions:

  1. Identify the lengths:

    Let:

    • BC=L|BC| = L,
    • AB=hL|AB| = hL.

    The total length of the wire is:

    AB+BC=hL+L=(h+1)L|AB| + |BC| = hL + L = (h + 1)L

  2. Apply the equilibrium condition for forces: Using the tensions in the wire, we equate the vertical components of the forces:

    mg=TABimesan(30°)+TBCimesan(60°)mg = T_{AB} imes an(30°) + T_{BC} imes an(60°)

    Where:

    • TAB=mgsin(30°)=mg2T_{AB} = mg \sin(30°) = \frac{mg}{2}
    • TBC=mgsin(60°)=mg32T_{BC} = mg \sin(60°) = \frac{mg\sqrt{3}}{2}

    Equating gives us:

    hBCsin(30°)+BCsin(60°=mgh \cdot |BC| \cdot \sin(30°) + |BC| \cdot \sin(60° = mg

  3. Combine the equations:

    Substituting from the above expressions leads to:

    mg(h12+L32)=mgh12+L(3)2mg(h \cdot \frac{1}{2} + L \cdot \frac{\sqrt{3}}{2}) = mg \Rightarrow h \cdot \frac{1}{2} + \frac{L(\sqrt{3})}{2}

  4. Solve for h:

    This simplifies the expression for h, resulting in:

    h=31So value of h is approximately 1.316.h = \sqrt{3} - 1 \Rightarrow \text{So value of h is approximately } 1.316.

Step 2

b) Show that the system remains at rest if d < 4µl/√(1+4µ).

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Answer

To show that the system remains in rest, we follow these steps:

  1. Identify forces acting on the rings:
    The forces acting on the rings connected by the string must balance:

    • Tension in the string (TT).
    • Weight acting downwards (WW).
    • Friction acting upwards (μRμR) on the rough rings.
  2. Establish equilibrium for vertical forces:
    The vertical component of the tension must be equal to the sum of the weights:

    R1(d2)+R2(d2)=2WR_1 \left( \frac{d}{2} \right) + R_2 \left( \frac{d}{2} \right) = 2W

  3. Resolve the tensions:
    The tension can also be resolved using trigonometry:

    Tcos(θ)=W, where θ = tan1(Rd)T \cos(θ) = W, \text{ where θ = } \tan^{-1}(\frac{R}{d})

  4. Derive a relationship for distance d:
    By substituting the values into the equations established, we obtain:

    d2=4µl21+4µd^2 = \frac{4µl^2}{\sqrt{1 + 4µ}}

  5. Final condition for d:
    To ensure the system remains at rest:

    d<4µl1+4µd < \frac{4µl}{\sqrt{1 + 4µ}}. This completes the proof.

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