Rigid Body Mechanics

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शिक्षकों के लिए: Rigid Body Mechanics (Physics, HL) के लिए इस्तेमाल के लिए तैयार लेसन स्लाइड्स, रिवीज़न नोट्स — इन्हें अपने लेसन में इस्तेमाल करें, या टॉपिक को एक इंटरैक्टिव क्लास एक्टिविटी की तरह चलाएं जिसे आपके शिक्षार्थी लाइव गेम की तरह खेलें।

लेसन नोट्स

Torque & Couples

  • A moment is the turning effect of a force around a pivot: Moment = Force × perpendicular distance from the pivot (N m).
  • For a non-perpendicular force, resolve the force or use τ = Fr sin θ, where θ is the angle between the force and the line from the pivot.
  • A couple is a pair of equal and opposite coplanar forces that produce rotation only; the forces are equal in magnitude, opposite in direction, and perpendicular to the distance between them.
  • The moment of a couple is Force × perpendicular distance between the lines of action; it does not depend on a pivot.
  • A couple produces zero resultant force (no linear acceleration) but a net torque causing angular acceleration.
  • For a couple on a wheel of radius r, the net torque is τ = 2Fr sin θ; when θ = 90°, τ = 2Fr.
  • Torque is maximum when the force is applied perpendicular to the lever arm (θ = 90°); at θ = 0° or 180°, torque is zero.

Rotational Equilibrium

  • A body is in rotational equilibrium if the resultant torque acting on it is zero; it remains at rest or rotates with constant angular velocity.
  • The condition for rotational equilibrium is: sum of clockwise torques = sum of anticlockwise torques (principle of moments).
  • A resultant (unbalanced) torque causes angular acceleration; the direction of angular acceleration is the same as the net torque direction.
  • When solving equilibrium problems, you can take torques about any point; choose a point that simplifies the calculation (e.g. where unknown forces act).
  • For a beam balanced on a pivot, the weight acts at the centre of mass; torques are calculated using τ = Fr for perpendicular forces.

Angular Displacement, Velocity & Acceleration

  • Angular displacement Δθ is the change in angle through which a body rotates, measured in radians.
  • Linear displacement is related to angular displacement by s = rΔθ.
  • Angular velocity ω is the rate of change of angular displacement: ω = Δθ / Δt, measured in rad s⁻¹.
  • Linear speed is related to angular speed by v = rω; also ω = 2πf = 2π/T and v = 2πfr.
  • Angular acceleration α is the rate of change of angular velocity: α = Δω / Δt, measured in rad s⁻².
  • Linear acceleration is related to angular acceleration by a = rα.
  • Graphs: angular displacement is the area under the angular velocity–time graph; angular velocity is the gradient of the angular displacement–time graph and the area under the angular acceleration–time graph; angular acceleration is the gradient of the angular velocity–time graph.

Angular Acceleration Formula (Rotational Kinematics)

  • The linear kinematic equations can be rewritten for uniform angular acceleration:
  • ωf = ωi + αt
  • Δθ = ωi t + ½ αt²
  • ωf² = ωi² + 2αΔθ
  • Δθ = (ωi + ωf) t / 2
  • These equations are used when angular acceleration is constant; identify the known and unknown quantities to select the appropriate equation.
  • When converting from RPM to rad s⁻¹, use ω = 2π × (RPM / 60).

Moment of Inertia

  • Moment of inertia I is the resistance of a body to a change in rotational motion; it depends on the mass distribution about the axis of rotation.
  • Moment of inertia is measured in kg m².
  • For a point mass, I = mr², where r is the distance from the axis of rotation.
  • The total moment of inertia of a system is the sum of the moments of inertia of its parts: Itotal = Σ mr².
  • The moment of inertia of a rigid body depends on its shape, density, and orientation relative to the axis of rotation.
  • Common moments of inertia (given in exams): solid cylinder/disc I = ½MR², solid sphere I = ⅖mr², hollow sphere I = ⅔mr², thin rod about centre I = 1/12 mL².
  • You are not expected to memorise moments of inertia of different shapes; they will be provided where needed.

Newton’s Second Law for Rotation

  • Newton’s second law for rotation: τ = Iα, where τ is torque (N m), I is moment of inertia (kg m²), and α is angular acceleration (rad s⁻²).
  • This is the rotational analogue of F = ma.
  • Torque is the rotational equivalent of force; moment of inertia is the rotational equivalent of mass.
  • For a point mass, I = mr² and α = a/r, leading to τ = Iα.
  • In problems with a hanging mass and pulley, apply F = ma to the linear motion and τ = Iα to the rotation, linking linear and angular acceleration by a = rα.

Angular Momentum

  • Angular momentum L is the rotational equivalent of linear momentum: L = Iω, measured in kg m² rad s⁻¹ (or kg m² s⁻¹).
  • For a point mass, L = mvr, where r is the perpendicular distance from the axis of rotation.
  • Conservation of angular momentum: the total angular momentum of a system remains constant unless acted upon by a net resultant torque.
  • For a constant total angular momentum: Iiωi = Ifωf.
  • Examples: an ice skater spinning faster when arms are pulled in (I decreases, ω increases); a diver tucking; a collapsing star increasing its rotation rate.
  • Objects travelling in straight lines can have angular momentum about a point not on their line of motion.

Conservation of momentum

Conservation of momentum

Angular Impulse

  • Angular impulse is the change in angular momentum produced by a torque acting over a time interval: ΔL = τΔt.
  • Angular impulse is measured in kg m² s⁻¹ or N m s.
  • The equation requires a constant resultant torque; if torque varies, use an average value.
  • A small torque acting for a long time can produce the same angular impulse as a large torque acting for a short time.
  • On a torque–time graph, the area under the graph equals the angular impulse or change in angular momentum.
  • For a changing torque, ΔL = I(ωf − ωi) can be used with the area under the graph.

Rotational Kinetic Energy

  • A rotating body has rotational kinetic energy: Ek = ½Iω² (or Ek = L² / 2I).
  • For an object rolling without slipping, total kinetic energy is the sum of translational and rotational kinetic energy: Ektotal = ½mv² + ½Iω².
  • Rolling without slipping requires friction; the point of contact has zero velocity, the centre of mass has velocity v = ωr, and the top point has velocity 2v.
  • When an object rolls down a slope, gravitational potential energy is converted into both translational and rotational kinetic energy: mgΔh = ½mv² + ½Iω².
  • Using v = ωr and the moment of inertia, the total kinetic energy can be expressed in terms of ω or v; for a solid sphere, mgΔh = 7/10 mω²r².
  • If an object slides (slips) without rolling, there is no rotational kinetic energy and angular velocity is zero.

स्लाइड्स

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प्रैक्टिस सवाल

फ्री प्रीव्यू — 61 में से 8 सवाल। सभी देखने के लिए साइन अप करें।
  1. 1.Which of the following best defines the moment of a force about a pivot?

    Easy
    • AThe product of the force and the perpendicular distance from the pivot to the line of action of the force
    • BThe product of the force and the distance from the pivot to the point of application of the force
    • CThe force divided by the perpendicular distance from the pivot
    • DThe product of the force and the time for which it acts
  2. 2.Which pair of forces acts as a couple?

    Easy
    • ATwo forces equal in magnitude, opposite in direction, and perpendicular to the distance between them
    • BTwo forces equal in magnitude and in the same direction, separated by a distance
    • CTwo forces of different magnitudes acting in opposite directions
    • DTwo forces equal in magnitude and opposite in direction, but not perpendicular to the distance between them
  3. 3.A force of 50 N is applied at an angle of 30° to a spanner of length 0.20 m. What is the torque produced?

    Medium
    • A5.0 N m
    • B8.7 N m
    • C10 N m
    • D0.50 N m
  4. 4.A uniform beam is pivoted at its centre. Two forces act on it: a 10 N force downwards at 0.30 m to the left of the pivot, and a 15 N force downwards at 0.20 m to the right of the pivot. What is the resultant torque on the beam?

    Medium
    • A0 N m, the beam is in rotational equilibrium
    • B1.0 N m clockwise
    • C1.0 N m anticlockwise
    • D6.0 N m clockwise
  5. 5.A solid cylinder of mass 2.0 kg and radius 0.50 m rotates about its central axis. What is its moment of inertia? (I = ½MR²)

    Medium
    • A0.25 kg m²
    • B0.50 kg m²
    • C1.0 kg m²
    • D0.125 kg m²
  6. 6.A star of mass M and radius R rotates with angular velocity ω. It collapses to a sphere of radius R/4 without losing mass. What is its new angular velocity? (Assume it remains a uniform sphere.)

    Hard
    • A16ω
    • B4ω
    • Cω/4
    • Dω/16
  7. 7.Which of the following statements about a couple are correct? (Select all that apply.)

    Medium
    • AThe resultant force of a couple is zero.
    • BA couple produces a net torque.
    • CThe moment of a couple depends on the choice of pivot.
    • DA couple causes angular acceleration.
    • EThe forces in a couple must act along the same line of action.
  8. 8.Which of the following are units of angular momentum? (Select all that apply.)

    Medium
    • Akg m² s⁻¹
    • BN m s
    • Ckg m s⁻¹
    • DJ s
    • Ekg m² s⁻²

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