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7. (a) One end of a uniform ladder, of weight $W$, rests against a rough vertical wall, and the other end rests on rough horizontal ground - Leaving Cert Applied Maths - Question 7 - 2008

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7. (a) One end of a uniform ladder, of weight $W$, rests against a rough vertical wall, and the other end rests on rough horizontal ground. The coefficient of frict... show full transcript

Worked Solution & Example Answer:7. (a) One end of a uniform ladder, of weight $W$, rests against a rough vertical wall, and the other end rests on rough horizontal ground - Leaving Cert Applied Maths - Question 7 - 2008

Step 1

Find $\tan \alpha$

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Answer

To determine tanα\tan \alpha, we analyze the forces and moments acting on the ladder.

  1. Equilibrium of Forces:
    The sum of vertical forces must equal zero: R+Rt=WR + R_{t} = W
    where RR is the normal reaction at the ground and RtR_{t} is the normal reaction at the wall.

  2. Moment about Point O:
    Taking moments about the base of the ladder: R(sinα)+W(ξ(cosα))=Rt(cosα)R \cdot (\sin \alpha) + W \cdot (\frac{\xi}{(\cos \alpha)}) = R_{t} \cdot (\cos \alpha)

    Here, ξ\xi represents the distance from the wall to the point where the ladder touches the ground.

  3. Equating Moments:
    Rearranging gives us: Rtanα+12(Rt+R)=RtR \tan \alpha + \frac{1}{2}(R_{t} + R) = R_{t}
    which simplifies to:
    12Rttanα+12R=Rt\frac{1}{2} R_{t} \tan \alpha + \frac{1}{2}R = R_{t}

  4. Solving for tanα\tan \alpha:
    The final derivation leads to: tanα=74\tan \alpha = \frac{7}{4}

Step 2

Find the coefficient of friction if C is on the point of slipping

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Answer

For the scenario of rods AB and BC:

  1. Equilibrium Condition:
    As rod AB is held horizontal and rod BC is inclined, we analyze moments about point A: W+W(l2+μR(2l2))=R(2l2)W + W \left(\frac{l}{\sqrt{2}} + \mu R \left(\frac{2l}{\sqrt{2}}\right)\right) = R \left(2 \cdot \frac{l}{\sqrt{2}}\right)

  2. Moments about B:
    Write the moment equation about B: W(12)+μR(22)=W+2μRW \left(\frac{1}{\sqrt{2}}\right) + \mu R \left(\frac{2}{\sqrt{2}}\right) = W + 2 \mu R
    Solving gives: R2=W+2RR \cdot 2 = W + 2R
    On simplifying leads to: R=3W2R = \frac{3W}{2}

  3. Final Expression for the Coefficient of Friction:
    Plugging in to find μ\mu gives us: μ=23\mu = \frac{2}{3}

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