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Question 6
6. (a) One end A of a light elastic string is attached to a fixed point. The other end, B, of the string is attached to a particle of mass m. The particle moves on a... show full transcript
Step 1
Answer
To prove that ω² ≤ , we start with the forces acting on the particle in circular motion.
Using the vertical balance of forces:
T ext{sin} heta = m r rac{v^2}{r}
From these equations, we can derive:
v = r imes rac{d heta}{dt} = r imes rac{d heta}{dt}, so we can write:
Step 2
Answer
From the previous part, knowing that the angular velocity ω² = , we can find θ through the elastic force in equilibrium:
Using Hooke's law, where T = k × extension, we have:
m rac{2amg}{h} = (m h ext{ + } l)
ext{cos θ} = rac{h}{l},
leading to:
$$ θ = ext{cos}^{-1}(0.8) ext{ giving } θ ≈ 36.87^ ext{o}.$
Step 3
Answer
To calculate |QR|, we assess the forces acting on the particle P suspended:
Using the equation for tension in terms of the mass and gravitational force:
T = rac{1}{2}g
k × d = rac{1}{2}g
k = rac{24.5}{g} ext{ where } g = 9.8.
Step 4
Answer
In assessing the movement of particle P, we note:
F = rac{1}{2} g - T,
Step 5
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