Answer:
Let T be the tension in the chain,
Then,
In the vertical direction,
Tcos(θ)=mg→(1)Tcos(\theta) = mg \to (1)Tcos(θ)=mg→(1)
Where m - mass of a seat
g - acceleration of gravity
In the horizontal direction,
Tsin(θ)=mv2r→(2)Tsin(\theta) = \frac{mv^2}{r} \to (2)Tsin(θ)=rmv2→(2)
where, v - speed of a seat
According to the figure,
r=lsin(θ)+d2r = lsin(\theta) + \frac{d}{2}r=lsin(θ)+2d
r=3.45sin(42.6)+9.152=6.91mr = 3.45sin(42.6) + \frac{9.15}{2} = 6.91mr=3.45sin(42.6)+29.15=6.91m
dividing equation (2) by (1)
we can get,
tan(θ)=v2rgtan(\theta) = \frac{v^2}{rg}tan(θ)=rgv2
Therefore, the speed of a seat,
v=rgtan(θ)v = \sqrt{rgtan(\theta)}v=rgtan(θ)
v=6.91∗9.8∗tan(42.6)v = \sqrt{6.91*9.8*tan(42.6)}v=6.91∗9.8∗tan(42.6)
v=7.89ms−1v = 7.89 ms^{-1}v=7.89ms−1