Rotational Inertia about Rotation Axis Through COM

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SUMMARY

The discussion centers on calculating the rotational inertia of a wheel subjected to a constant horizontal force of 10 N, with a mass of 10 kg and a radius of 0.30 m. The acceleration of the center of mass is given as 0.60 m/s². Participants clarify that the rotational inertia formula for a hoop, I = MR², is not applicable due to the wheel's complex structure, which includes an outer and inner radius. The net torque is determined using the relationship net torque = Iα, where α is derived from the acceleration of the center of mass divided by the radius.

PREREQUISITES
  • Understanding of net torque and its calculation
  • Familiarity with angular acceleration and its relationship to linear acceleration
  • Knowledge of rotational inertia and its formulas
  • Basic principles of friction in rolling motion
NEXT STEPS
  • Study the derivation of the net torque equation in rotational dynamics
  • Learn about the differences in rotational inertia for various shapes, including hoops and solid disks
  • Explore the concept of rolling without slipping and its implications on friction
  • Investigate the effects of complex wheel structures on rotational motion
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and rotational dynamics, as well as educators seeking to clarify concepts related to torque and rotational inertia.

Reefy
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Homework Statement



A constant horizontal force of magnitude 10 N is applied to a
wheel of mass 10 kg and radius 0.30 m as shown in the figure.
The wheel rolls smoothly on the horizontal surface, and the
acceleration of its center of mass has magnitude 0.60 m/s2.

(a) What are the magnitude and direction of the frictional force on
the wheel?

(b) What is the rotational inertia of the wheel about the rotation
axis through its center of mass?

Homework Equations



angular acceleration α = acceleration (COM) over radius

net torque =

The Attempt at a Solution



I finished part a and found out that I have to use the equations above for part B. What I'm confused about is why I can't use the rotational inertia for a hoop about its central axis I = MR^2

attachment.php?attachmentid=8544&d=1165455553.gif
 
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Also, torque = RFsin∅. What is ∅ in this case because R can be measured from any point...

edit: actually i might have figured this angle part out. the frictional force is at the point where the wheel is touching the floor (pointing to the left or negative x-direction) and the distance from the center of the wheel to that point is R (point straight down or negative y-direction), making the angle 90 degrees.
 
Last edited:
Hi Reefy! :smile:

(never first-reply top your own question :redface: … it takes you off the "Unanswered" list!)
Reefy said:
…why I can't use the rotational inertia for a hoop about its central axis I = MR^2

attachment.php?attachmentid=8544&d=1165455553.gif

because the picture shows clearly that the wheel has an outer radius and an inner radius, and you're not told what they are (also the spokes are clearly not negligibly thin, as in a bicycle wheel)
Reefy said:
the frictional force is at the point where the wheel is touching the floor (pointing to the left or negative x-direction) and the distance from the center of the wheel to that point is R (point straight down or negative y-direction), making the angle 90 degrees.

yes :smile:
 
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