Tangential Component of Centrifugal Acceleration

Click For Summary
SUMMARY

The discussion centers on the tangential component of centrifugal acceleration as described in Taylor's physics text on page 347. The equation for the tangential component is established as g_tan = Omega^2 * R * sin(theta) * cos(theta), with theta being the complement of the latitude angle L (θ = 90 - L). The participants clarify the geometric relationships between the centrifugal force, gravitational force, and the angles involved, emphasizing that at the equator, the centrifugal force is maximized while the tangential component is zero. The conversation concludes with a clear understanding of the angles involved in the context of centrifugal acceleration.

PREREQUISITES
  • Understanding of centrifugal acceleration and its components
  • Familiarity with trigonometric functions and their applications in physics
  • Knowledge of the relationship between latitude and angles in spherical geometry
  • Basic comprehension of vector forces in physics
NEXT STEPS
  • Study the derivation of centrifugal acceleration equations in physics textbooks
  • Learn about the effects of latitude on gravitational and centrifugal forces
  • Explore geometric interpretations of forces in rotational motion
  • Investigate the implications of centrifugal acceleration in real-world applications
USEFUL FOR

Students of physics, educators teaching mechanics, and professionals in engineering fields who require a deeper understanding of rotational dynamics and centrifugal effects.

SebastianRM
Messages
39
Reaction score
4
The thing is in page p.347 Taylor, it is said that the component is:

g_tan = Omega^2*Rsin(theta)cos(theta) However the angle between the centrifugal Force and the axis normal to the direction of the grav Force is actually 90 - theta, I am not really getting where I am going wrong understanding this.
 
Physics news on Phys.org
The angle in question is between the perpendicular to the Earth's axis (the direction of the centrifugal force component) and a tangent to the surface. That angle is θ which you can see by geometry. θ is the complement of the angle of latitude, L (θ = 90-L).

The magnitude of the centrifugal acceleration (see equation 9.43) is: acf = Ω2Rsinθ. So the tangential component is acfcosθ. At the equator, where θ is 90° (L=0), the centrifugal force is maximum (sinθ = 1) but the tangential component is 0 because it is all in the radial direction (cosθ = 0). Towards the pole, the direction is almost tangential (cosθ=1) but the magnitude of the centrifugal force approaches 0 (sinθ = 0).

AM
 
  • Like
Likes SebastianRM
kuruman said:
I thought I explained that to you here.
https://www.physicsforums.com/threads/what-is-the-tangential-component-taylor-p-347.965665/
If there is something you still did not understand, you should have responded there instead of starting a new thread. In any case, post a drawing of what you think is the case. I suspect you have misidentified something.
Sorry about that, I could not track the post I had done already. Here is the sketch of how I am working it out on my mind.
spbCzfS
https://imgur.com/spbCzfS
Since he says: 'the tangential component of g (the component normal to the true grav force)'
 
SebastianRM said:
Sorry about that, I could not track the post I had done already. Here is the sketch of how I am working it out on my mind.
spbCzfS
https://imgur.com/spbCzfS
Since he says: 'the tangential component of g (the component normal to the true grav force)'
In the drawing you have provided, you have shown two angles of 90-θ making up a right angle! The angle between the Fcf vector and the tangent is 90 - (90-θ) = θ! (the angle of the tangent to the radial vector being necessarily a right angle).

AM
 
  • Like
Likes SebastianRM
To supplement post #5 by @Andrew Mason, it is known from geometry that two angles that have their sides mutually perpendicular are equal. In your diagram, the z-axis (along Ω) is perpendicular to Fcf and the radial vector is perpendicular to the tangential component (not shown). Therefore the angle that you show as θ is equal to the angle formed by Fcf and the tangential direction.
 
  • Like
Likes SebastianRM
Thank you so much guys! I see it now!
 
  • Like
Likes kuruman

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 17 ·
Replies
17
Views
3K
  • · Replies 9 ·
Replies
9
Views
3K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 11 ·
Replies
11
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 11 ·
Replies
11
Views
6K
Replies
4
Views
2K
  • · Replies 43 ·
2
Replies
43
Views
11K