Torque and rotational inertia 

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Intros
Lessons
  2. Definition of "Torque"
  3. Rotational Inertia
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Examples
Lessons
  1. A person exerts a force of 45N on the handle of a door 65cm wide.
    1. What is the magnitude of the torque if the force is exerted perpendicular to the door?
    2. What is the magnitude of the torque if the force is exerted at a 35°?
  2. Calculate the net torque about the axle of the of the wheel shown below. Assume that a friction torque of 0.60 N.mN.m opposes the motion.

    Torque and Rotational Inertia
    1. A torque of 66 N.mN.m is required to tighten the bolts on the cylinder head of a car engine. The wrench used to tighten the bolt is 26cm long.

      Torque and Rotational Inertia
      1. What is the perpendicular force that is exerted by the mechanics to the end of the wrench to tighten the bolts?
      2. If the six-sided bolt head has a diameter of 20mm, how much force will be applied near each of the six points?
    2. Two small weights of mass 4.0kg and 6.0kg are mounted 6.0m apart on a light rod as shown below. Calculate the moment of inertia of the system;

      Torque and Rotational Inertia
      1. When rotated about an axis halfway between the weights.
      2. When rotated about an axis 0.40m to the left of the 4.0kg mass.
    3. A 12.0N force is applied to a cord wrapped around a pulley of mass MM = 6.00kg and radius RR= 22.0cm. The pulley accelerates uniformly from rest to an angular speed of 40.0 rad/s in 2.00s. If there is a frictional torques τfr\tau _{fr} = 1.20m.Nm.N at the axle, determine the moment of inertia of the pulley as it rotates around its center.
      1. Determine the moment of inertia for the following uniform objects:
        1. A 12.80 kg sphere of radius 0.464m rotating through its center.
        2. A bicycle wheel 88.2cm in diameter. The rim and tire have a combined mass of 1.36kg
        3. A helicopter rotor blade (long thin rod), 2.76 m long and has a mass of 140kg.
      2. An Atwood's machine consists of two masses, m1m_{1} = 4.0kg and m2m_{2} = 7.0kg, which are connected by a massless inelastic cord that passes over a pulley. The pulley has radius RR = 0.4m and moment of inertia II =4.0 kg. m2m_{2} about its axle.

        Torque and Rotational Inertia
        1. Determine the acceleration of the masses m1m_{1} and m2m_{2}.
        2. Find tensions supporting m1m_{1} and m2m_{2}.
      Topic Notes
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      In this lesson, we will learn:

      • Definition of Torque
      • Translational equilibrium Vs. Rotational equilibrium
      • Rotational Inertia
      • Moment of inertia of uniform objects

      Notes:


      Torque

      • To have better understanding of the meaning of “torque”, let’s try the following activity and compare the motion of object as different forces are exerted.
      • A ruler is placed on a horizontal flat surface.

        • (a) The force is applied at the center of mass

      Torque and Rotational Inertia

        \quad The whole object (ruler) will accelerate in the direction of the force exerted.

        (b) The force is applied away from the center of mass

      Torque and Rotational Inertia

      The whole object (ruler) will rotate about the center of mass.

      Torque and Rotational Inertia


      As the result of exerting force, the object will rotate about the “Pivot” or “Axis of Rotation”.

      Therefore, we can define Torque as the “Turning Effect of a Force”.

      Torque is represented by the Greek letter τ\tau and the standard unit is N.m.N.m.


      Conclusion:
      • Force causes acceleration; F=maF=ma

      • Torque causes angular acceleration: τ=rFsin⁡θ  \tau = r F \sin \theta \; (vector quantity)
        θ\theta : angle between r r and F F
        r r : distance between the pivot and point at which the force is exerted on.

      Torque and Rotational Inertia


      τ ∝ r \tau \, \propto \, r : the further the force, the bigger the torque
      τ ∝ θ \tau \, \propto \, \theta : the larger the angle, the bigger the torque 

      The object could be in Translational Equilibrium and Rotational Equilibrium;

      ∑F=0 \sum F = 0 \qquad \qquad “Translational Equilibrium”   ⇒  \; \Rightarrow \, acceleration is zero
      ∑τ=0 \sum \tau = 0 \qquad \qquad “Rotational Equilibrium”   ⇒  \; \Rightarrow \, angular acceleration is zero


      Rotational Inertia

      Let’s consider a mass m rotating in a circle of radius r about a fixed point. The object is going to experience tangential and angular acceleration.

      Torque and Rotational Inertia

      I=mr2I = mr^{2} \quad (scalar quantity) Unit: kg.m2


      “Rotational Inertia represents the resistance to angular acceleration”

      • Large Rotational Inertia: the mass of the object is distributed far from the axis of rotation.
        Objects with larger Rotational Inertia are harder to get rotating and harder to stop rotating.
      • Small Rotational Inertia: the mass of the object is distributed close to the axis of rotation.


      I=mr2I = mr^{2} \qquad (single mass rotating of a single radius)
      I=∑mr2  I = \sum mr^{2} \enspace \; (multiple individual masses rotating in circles of different radius)


      • Moment of inertia for objects of uniform composition is constant;

      Torque and Rotational Inertia