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Please help me sove this physical pendulum problem?
Problem 49. It is a question in Fundamentals of Physics Extended version 8th edition
I would be able to solve it if the pivot point was at the end of the stick. But I can't, because there is a part of the stick on both sides of the pivot point.
Please show me how you derived the answer
2 Answers
- ?Lv 77 years agoFavorite Answer
Two things you need to know here:
1) period T = 2π√(I / mgx), and
2) I = Icm + mx² = mL²/12 + mx² = m(L²/12 + x²)
(by the parallel axis theorem)
Then T = 2π√( m(L²/12 + x²) / mgx) = 2π√((L²/12 + x²) / gx)
Find where T is max/minimized:
d((L²/12 + x²) / x)/dx = 1 - L²/12x² = 0
x² = L²/12
x = L/√12 = L*√12 / 12 = L√3 / 6 ← distance from center
Since L = 1.85 m, x = 0.534 m
and T = 2π√( (1.85²/12 + 0.534²) / 0.534*9.8) s = 2.07 s ← resulting period
We should check the endpoints.
By observation, as x → 0, T → infinity, so that's not a minimum.
When x = L/2, T = 2π√( (1.85²/12 + (1.85/2)² / (9.8*1.85/2) ) s = 2.23 s -- not a minumum.
- Anonymous7 years ago
(a)
The weight of the stick is solely responsible for its torque.
Iθ" = mgx sinθ
Find the moment of inertia of the stick at different pivot points via the parallel axis theorem.
(mL²/12 + mx²)θ" = mgx sinθ
(L²/12 + x²)θ" = gx sinθ
For small oscillations sinθ ≈ θ.
θ" = [gx / (L²/12 + x²)] θ
ω² = gx / (L²/12 + x²)
d(ω²)/dx = [(L²/12 + x²)(g) - (gx)(2x)] / (L²/12 + x²)² = 0
g(L²/12 - x²) = 0
x = L/sqrt(12)
(b)
ω² = [gL/sqrt(12)] / (L²/12 + L²/12)
ω² = [g/sqrt(12)] / (L/6)
(2π/T)² = g sqrt(3) / L
T = 2π sqrt{L / [g sqrt(3)]}