Angular Acceleration and tangential acceleration

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SUMMARY

The discussion centers on the relationship between tangential acceleration (At) and angular acceleration (Ar), specifically the equation At = R * Ar. It is established that while At and Ar are vector components, the rearranged equation Ar = At/R does not maintain vector integrity due to the non-commutative nature of angular displacement. The conversation highlights the importance of defining angular displacement as a vector, requiring unit vectors for both radius and angle, and references the vector equation for angular motion, V = ω × R, as discussed in Resnik and Halliday's advanced mechanics texts.

PREREQUISITES
  • Understanding of vector components in physics
  • Familiarity with angular motion concepts
  • Knowledge of cross products in vector mathematics
  • Basic principles of rotational dynamics
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  • Study the vector cross product and its applications in physics
  • Learn about angular motion equations and their vector representations
  • Explore advanced mechanics texts, specifically Resnik and Halliday
  • Investigate the implications of non-commutative properties in vector addition
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Seph
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Hmmm. I have a question...

We know that the tangential acceleration (At) is equal to the radius (R) multiplied by angular acceleration (Ar), of which At and Ar are vector components.
At = R Ar

Then I was told that Ar = At/R is not a vector equation. Why is that true?

~Seph :confused:
 
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Well mainly, because those relations refer to the magnitude of those vectors, the problem is angle displacement does not work with vectorial addition communitative property, but as it gets smaller it works with vectorial addition, that's why angular velocity and aceleration are vectors.

Also, you could define angular displacement as a vector, but you will need an unit vector for the radius and the angle, so you will give them direction.
 
Your equation is one component of the basic vector equation for angular motion:

V = omega X R where v is the velocity vector, omega is the angular velocity vector, and R is the position vector , and X indicates the vector cross product. (If an object is rotating around the z axis, then the omega vector points along the positive z axis for counterclockwise rotations.)

This vector approach is discussed in Resnik and Halliday, and in most more advanced texts on mechanics.


Regards,
Reilly Atkinson
 

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