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A.4.2 Rotational Equilibrium — IB Physics HL Revision Notes & Topical Questions

5 min read 8 parts Lesson 44 of 63 1 quiz

📚 IB Physics HL Hub / Topical Revision
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Curriculum Equation Key قوانين الرقم الهيدروجيني والاتزان الأيوني - pH & Acid-Base Equilibrium FormulasFast Exam Solution
pH = -log[H⁺] | pOH = -log[OH⁻] | pH + pOH = 14 | [H⁺][OH⁻] = 10⁻¹⁴
Word Equation & Conditions: الرقم الهيدروجيني = -لوغاريتم تركيز أيون الهيدروجين | pH + pOH = 14
Location & Specifications: الاتزان الأيوني، كيمياء 3 ثانوي، التحصيلي، و AP Chemistry.
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Lesson summary

A.4.2 Rotational Equilibrium — IB PHYSICS HL notes: State the conditions for rotational equilibrium and apply the principle of moments to beams.Rotational equilibrium = zero resultant torque on a body.A body in rotational equilibrium stays at rest or rotates with constant angular…

  • Sum of clockwise torques
  • Torque of each force τ
  • Choose a point through which unknown forces act
  • A resultant torque causes angular acceleration
  • Net torque
  • Displacement

Part 1 of 6Rotational equilibrium

Rotational equilibrium
Rotational equilibrium zero resultant torque on a body.
A body in rotational equilibrium stays at rest or rotates with constant angular velocity.
It is the rotational analogue of Newton's first law for translational equilibrium.
A rigid extended body, such as a beam, can be in rotational equilibrium.

Part 2 of 6Principle of moments

Sum of clockwise torques
Sum of clockwise torques sum of anticlockwise torques.
Torque of each force τ
Fr sin θ, and τ = Fr when the force is perpendicular.
Balanced forces either side of a pivot give a beam with zero resultant torque.
Both conditions are needed for full equilibrium.
  • Zero resultant force for translational equilibrium.
  • Zero resultant torque for rotational equilibrium.

Part 3 of 6Choosing the pivot point

1
Any point can be used, not just the axis of rotation.
2Choose a point through which unknown forces act
  • Choose a point through which unknown forces act their torque is zero and they drop out.
3
Choose a point where the torque of most forces is known.
4
The weight of a uniform beam acts at its centre.

Part 4 of 6Unbalanced torque

Unbalanced torque
A resultant torque causes angular acceleration
  • A resultant torque causes angular acceleration like a resultant force causes linear acceleration.
The direction of the angular acceleration is the direction of the net torque.
A beam with more clockwise than anticlockwise torque rotates clockwise with increasing angular speed.

Part 5 of 6Tipping and limiting conditions

1
A plank just about to tip has the support force at one support equal to zero.
2
At that point take torques about the other support.
3
Method.
  1. Identify all forces and which pivot to use.
  2. Write the clockwise and anticlockwise torques about it.
  3. Equate them and solve for the unknown distance or force.
4
Torque is a vector, but only its clockwise or anticlockwise sense is needed at this level.

Part 6 of 6More from the specification

More from the specification
Static equilibrium in a rotating system
  • Static equilibrium in a rotating system vanishing resultant forces and zero net torque ensure static mechanical equilibrium within a rigid body system.
Conditions for Rotational Equilibrium
  • A rigid body is in complete rotational equilibrium when the vector sum of all external torques acting about any arbitrary axis equals zero (sigma_tau = 0), preventing angular acceleration.
Torque of a Couple
  • A couple consists of two parallel forces of equal magnitude acting in opposite directions along parallel lines;
    • its resultant torque is independent of pivot position and equals force multiplied by perpendicular separation: tau = F d.
Moment of Inertia and Angular Acceleration
  • Moment of inertia (I) quantifies rotational inertia;
    • an applied net torque produces an angular acceleration alpha according to the rotational analogue of Newton's second law: tau = I alpha.
Rotational Kinetic Energy and Work Done
  • A spinning object possesses rotational kinetic energy Ek_rot = 1/2 I omega2;
    • the work done by a net torque during an angular displacement delta_theta is given by W = tau delta_theta.
Kinetic energy
  • K = ½mv2, energy of motion.
Inertia
  • Resistance of an object to changes in its motion.
Displacement
  • Change in position.
Couple
  • A pair of equal opposite forces with different lines of action.
Impulse
  • J = FΔt = Δp.
    What the symbols mean: F = force (N) · Δt = time the force acts (s) · Δp = change in momentum (kg m s−1); FΔt is the impulse (N s)
Radius
  • Distance from the centre to the circular path.

Key terms

TermMeaning
Rotational equilibriumZero resultant torque.
Principle of momentsClockwise torques equal anticlockwise torques at equilibrium.
PivotPoint about which torques are calculated.
BeamRigid extended body, often supported at points.
Net torqueResultant torque on a body.
Angular accelerationRate of change of angular velocity.

Avoid these mistakes

1
Using only the force balance and forgetting the torque balance.
2
Measuring distances from the wrong pivot for different forces.
3
Forgetting the weight of the beam, which acts at its centre.
4
Using non-perpendicular distances without a sine factor.
5
Treating zero net torque as meaning the body must be at rest.

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3 & IGCSE —

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