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Dwade
Lv 4
Dwade asked in Science & MathematicsPhysics · 7 years ago

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

Attachment image

2 Answers

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  • ?
    Lv 7
    7 years ago
    Favorite 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.

  • Anonymous
    7 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)]}

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