Simple Rotational Motion Problem

Click For Summary
SUMMARY

The discussion focuses on calculating the force exerted on a bolt by a helicopter rotor blade during uniform rotation at 320 revolutions per minute (rev/min). The blade, with a length of 6.20 meters and a mass of 150 kg, can be treated as a point mass at its center of mass for this calculation. The force is determined using the formula F = mω²r, resulting in a magnitude of approximately 4,961 N on the bolt. This calculation emphasizes the importance of understanding rotational dynamics and the uniform distribution of mass in rigid bodies.

PREREQUISITES
  • Understanding of rotational motion principles
  • Familiarity with angular velocity and its conversion from revolutions per minute to radians per second
  • Knowledge of the formula F = mω²r for calculating forces in rotational systems
  • Concept of center of mass in rigid bodies
NEXT STEPS
  • Study the derivation and applications of the formula F = mω²r in various rotational motion scenarios
  • Learn about the effects of torque on angular acceleration in rigid body dynamics
  • Explore the concept of center of mass and its significance in physics
  • Investigate the principles of uniform circular motion and its implications in engineering applications
USEFUL FOR

This discussion is beneficial for physics students, mechanical engineers, and anyone involved in the design and analysis of rotating systems, particularly in aerospace applications.

veraction
Messages
1
Reaction score
0
A uniform helicopter rotor blade is L = 6.20 m long, has a mass of 150 kg, and is attached to the rotor axle by a single bolt.

(a) What is the magnitude of the force on the bolt from the axle when the rotor is turning at 320 rev/min? (Hint: For this calculation the blade can be considered to be a point mass at its center of mass. Why?)

Ok, this problem has been driving me crazy. I was thinking that the force is zero since the magnitude of the angular acceleration is zero, however that is not the case.

Please help :)
 
Physics news on Phys.org
Do you know that the acceleration of the centre of mass of a rigid body is equal to
(The net extenal force)/The total mass ? ( That's what the hint implied).
If you apply this theorem to the blade,the force will be (Total mass)*( The acc. of the centre of mass, which is L/2 into the angular speed squared).
I am, with great respect,
Einstone.
P.S.- Angular acceleration results only in case of an external torque.
 


The magnitude of the force on the bolt from the axle can be calculated using the formula F = mω²r, where m is the mass of the blade, ω is the angular velocity in radians per second, and r is the distance from the center of mass to the bolt. Since the blade can be considered a point mass at its center of mass, the distance r is equal to half of the length of the blade, or L/2.

Substituting the given values, we get F = (150 kg)(320 rev/min)(2π/60 sec)²(6.20 m/2) = 4,961 N. This means that the force on the bolt is almost 5,000 N.

The reason we can consider the blade as a point mass at its center of mass is because the blade's mass is evenly distributed along its length. This means that regardless of where the bolt is attached, the force on the bolt will be the same. Additionally, the rotation of the blade is uniform, so the force on the bolt will also be uniform.

I hope this helps clear things up for you. Remember to always consider the formula F = mω²r when dealing with rotational motion problems.
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
2K
Replies
67
Views
5K
Replies
17
Views
1K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
1
Views
1K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 20 ·
Replies
20
Views
2K
  • · Replies 10 ·
Replies
10
Views
2K