Chapter 11: Rotational Dynamics & Static Equilibrium

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17 Terms

1
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Torque

  • The ability of a force F to rotate the body around an axis

    • depends on the magnitude of its tangential component Ft and the distance the Force is applied ( r )

  • Torque = τ = (F)rsin(θ)

    • r: distance from rotational axis

    • F: force

    • θ: angle between F & r

    • unit: Newton-meters Nm

  • Torque is a vector

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If r is larger, torque is…

larger

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Newton’s Law of Rotation

  • Found from Newton’s Second Law

    • Ft = mat

    • τ = Ftr = matr

    • τ = m(αr)r = (mr²)α

    • τ = Iα

  • For more than one force, we can generalize: τnet = Iα in radians

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The torque due to the tangential component of force causes…

an angular acceleration around the rotation axis

5
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If the turning tendency of the force is counterclockwise, the torque will be…

positive

<p>positive</p>
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If the turning tendency of the force is clockwise, the torque will be…

negative

<p>negative</p>
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<p>A rod is pivoted about its center. A 5-N force is applied 4 m from the pivot and another 5-N force is applied 2 m from the pivot, as shown. The magnitude of the total torque about the pivot (in N*m) is?</p>

A rod is pivoted about its center. A 5-N force is applied 4 m from the pivot and another 5-N force is applied 2 m from the pivot, as shown. The magnitude of the total torque about the pivot (in N*m) is?

  • F1 = 5 N

  • r1 = 4 m

  • F2 = 5 N

  • r2 = 2 m

  • τ1 = Frsin(theta) = (5 N)(4 m)(sin(30)) = 10

    • counterclockwise → +10

  • τ2 = Frsin(theta) = (5 N)(2 m)(sin(30)) = 5

    • counterclockwise → +5

  • τ1 + τ2 = τ = 15 N*m

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Equilibrium & Torque: Conditions

  1. The net external force must be zero at equilibrium

  • ∑F = 0

  • OR ∑Fx = 0 & ∑Fy = 0

  • translational equilibrium → no translational motion

    • no sliding, no accelerating

  • a = 0

  • v = constant or = 0

  1. The net external torque must be zero at equilibrium

  • τ = 0

  • rotational equilibrium → no rotational motion

    • no spinning, no rotating

  • α = 0

    • no angular acceleration

  • ω = constant or = 0

    • spinning at constant rate or not spinning at all

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term image
  • τ = 0

  • m = 55 kg

  • M = 75 kg

  • mpl = 12 kg

  • d = 2.0 m

  • x = ?

  • τ = 0

  • τ = Frsin(theta)

    • F = mg

    • mg *r *1

  • τmg = +mg(2.0m) - Mg(x) + n(0) - mplg(0)

    • mg → cc → positive

    • Mg → clockwise → negative

    • n → r = 0 b/c r is distance from pivot point

    • mpl → r = 0

  • τmg = +mg(2.0m) - Mg(x)

  • τmg = (55 kg)(2.0 m) - (75 kg)(x)

  • x = 15 m

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r is the distance from the…

pivot point

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<p>If we do the Lady as the pivot point…</p>

If we do the Lady as the pivot point…

  • τ = 0

  • τ = Frsin(theta)

    • F = mg

    • mg *r *1

  • τmg = mg(0m) - Mg(2+x) + n(2) - mplg(2)

    • mg → r = 0 b/c r is distance from pivot point

    • Mg → clockwise → negative; distance 2+x from pp

    • n → r = 2 b/c r is distance from pp

      • the n is positive because it is an upward acting force, counterclockwise lifing board on right

    • mpl → r = 2; clockwise → negative

  • τmg = -(75 kg)(2+x) + 2n - (12 kg)(2)

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Angular Momentum

  • rotational equivalent of linear momentum

  • L = Iω

    • kg*m²/s

    • I: Moment of Inertia

      • how spread out your mass is

    • ω: angular velocity

      • spin speed

  • τ = ΔL/Δt

  • L = (mv²)/ω

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Conservation of Angular Momentum

  • If the net external torque acting on a system is 0, the angular momentum L of the system remains constant, no matter what changes take place within the system

  • Li = Lf in an isolated system

    • rotational

    • linear: pi = pf

  • Iiωi = Ifωf

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<p>Which is faster?</p>

Which is faster?

  • Iiωi = Ifωf

    • If no external torques act

    • angular momentum remains constant

  • 1: I increases, ω must decrease

  • 2: I decreases, ω must increase

  • So, she is faster in the second position

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More condensed space typically equals…

an increased angular velocity due to conservation of angular momentum.

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Rotational Work & Power

  • a torque acting through an angular displacement does work, just as a force acting through a distance does

  • W = τΔθ

  • Power is the rate at which work is done, for rotational motion and translational motion

  • P = W/Δt = τ(Δθ/Δt) = τω

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A playground merry-go-round has a radius of 3.0 m and a rotational inertia of 600 kg × m². It is initially spinning at 0.80 rad/s when a 20-kg child crawls from the center to the rim. When the child reaches the rim, the angular velocity of the merry-go-round is what?

  • r = 3.0 m

  • I = 600 kg*m²

  • ωi = 0.80 rad/s

  • m = 20 kg

  • ωf = ?

  • Iiωi = Ifωf

  • (600 kg*m²)(0.80 rad/s) = (600 + mr²)(ωf)

  • 480 = (600 + (20 kg*3.0²))(ωf)

  • ωf = 0.62 rad/s

<ul><li><p>r = 3.0 m</p></li><li><p>I = 600 kg*m²</p></li><li><p>ω<sub>i</sub> = 0.80 rad/s</p></li><li><p>m = 20 kg</p></li><li><p>ω<sub>f </sub>= ?</p></li></ul><p></p><ul><li><p><strong>I<sub>i</sub>ω<sub>i</sub> = I<sub>f</sub>ω<sub>f</sub></strong></p></li><li><p>(600 kg*m²)(0.80 rad/s) = (600 + <strong><u>mr²</u></strong>)(ω<sub>f</sub>)</p></li><li><p>480 = (600 + (20 kg*3.0²))(ω<sub>f</sub>)</p></li><li><p>ω<sub>f </sub>= 0.62 rad/s</p></li></ul><p></p>