Torque and rotational inertia  - Rotational Motion

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Torque and rotational inertia 

Lessons

Notes:

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=rFsinθ  \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


τr \tau \, \propto \, r : the further the force, the bigger the torque
τθ \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
  • Intro Lesson
  • 1.
    A person exerts a force of 45N on the handle of a door 65cm wide.
  • 3.
    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
  • 4.
    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
  • 6.
    Determine the moment of inertia for the following uniform objects:
  • 7.
    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
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Torque and rotational inertia 

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