Radial and tangential components of acceleration

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Discussion Overview

The discussion revolves around the representation of acceleration in different coordinate systems, specifically focusing on the radial and tangential components of acceleration in 2D kinematics. Participants explore the use of intrinsic coordinates versus polar and cylindrical coordinates, examining the implications for understanding tangential and centripetal acceleration components.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that acceleration can be expressed in intrinsic coordinates using the tangential vector ##T## and normal vector ##N##, with the tangential component being the tangential acceleration and the normal component being the centripetal acceleration.
  • Others argue that expressing acceleration in polar coordinates may not allow for a clear distinction between tangential and centripetal components, as the radial unit vector may not always be perpendicular to the trajectory curve.
  • One participant suggests that in cylindrical coordinates, the velocity vector can be decomposed to find the tangential and normal components of acceleration through dot products with the respective unit vectors.
  • There is a clarification regarding the difference between polar and cylindrical coordinates, with some participants noting that they are often used interchangeably in 2D contexts.
  • Some participants highlight that the intrinsic basis vectors ##(T,N,B)## are typically used in introductory physics texts to discuss centripetal and tangential accelerations, rather than other coordinate systems.
  • Disagreement arises regarding the interpretation of the radial unit vector ##\textbf{i}_r##, with some asserting it is not necessarily normal to the trajectory of a moving particle.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of tangential and centripetal components in polar coordinates, with no consensus reached on whether these components can be clearly defined in that context. The discussion remains unresolved regarding the relationship between the radial unit vector and the trajectory of the moving particle.

Contextual Notes

Limitations include the potential ambiguity in the definitions of coordinate systems and the assumptions regarding the orientation of unit vectors in relation to the trajectory. The discussion also reflects varying interpretations of the mathematical relationships involved.

fog37
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Hello,
In 2D kinematics, the acceleration vector ##a(t)## can be expressed either in Cartesian coordinates ##a_x## and ##a_y## or in polar coordinates ##r## an ##\theta##. It depends on the problem.
But it is also possible to express the acceleration ##a(t)## in the so called "intrinsic coordinates" using the intrinsic unit vectors ##T## (the tangential vector), ##N## (the normal vector).

The unit vectors ##T## and ##N## form an orthonormal basis. Each vector changes direction as the object travels its trajectory since the vectors from a moving basis. The component of the acceleration along the ##N## vector is called the centripetal component while the component along the ##T## vector is the tangential acceleration, correct?

Can we talk about tangential and centripetal acceleration components even when we express the acceleration vector in polar coordinates? I don't think so since the radial unit vector is not always perpendicular to the trajectory curve. Just checking...

What are the benefits of intrinsic coordinates?

thanks.
 
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I think this can be done with cylindrical coordinates. In cylindrical coordinates, the velocity vector is given by $$\mathbf{v}=\frac{dr}{dt}\mathbf{i_r}+r\frac{d\theta}{dt}\mathbf{i_{\theta}}$$From this it follows that the unit vector in the tangential direction is
$$\mathbf{t}=\frac{\mathbf{v}}{|\mathbf{v}|}=\frac{\frac{dr}{dt}\mathbf{i_r}+r\frac{d\theta}{dt}\mathbf{i_{\theta}}}{\sqrt{\left(\frac{dr}{dt}\right)^2+\left(r\frac{d\theta}{dt}\right)^2}}$$and the unit vector in the normal direction is:$$\mathbf{n}=\frac{-r\frac{d\theta}{dt}\mathbf{i_r}+\frac{dr}{dt}\mathbf{i_{\theta}}}{\sqrt{\left(\frac{dr}{dt}\right)^2+\left(r\frac{d\theta}{dt}\right)^2}}$$In addition, the acceleration vector is equal to the time derivative of the velocity vector: $$\mathbf{a}=\left[\frac{d^2r}{dt^2}-r\left(\frac{d\theta }{dt}\right)^2\right]\mathbf{i_r}+\left[2\frac{dr}{dt}\frac{d\theta}{dt}+r\frac{d^2\theta}{dt^2}\right]\mathbf{i_{\theta}}$$
The tangential component of the acceleration is obtained by dotting the acceleration vector with the unit vector in the tangential direction. What do you get when you do this? The centripetal component of the acceleration is obtained by dotting the acceleration vector with the unit vector in the normal direction. What do you get when you do this?
 
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rcgldr said:
Did you mean polar coordinates? Cylindrical coordinates would include a Z term (r, θ, z). I'll delete this post later.
Yes. I usually use the terms interchangeably.
 
In 2D, polar and cylindrical are indeed the same unit basis vectors.

I think the decomposition of the acceleration vector ##a(t)## into a tangential component (locally tangent to the path) and centripetal component (perpendicular to the path) truly derivies from using the intrinsic basis: $a(t) = a_centripetal(t) \hat{N} + a_tangential \hat{T}$

and considering the local osculating plane. For example, at a specific point ##P## on the trajectory, the unit basis vector ## \hat{N} ## is exactly in the direction of the radius of the local osculating circle and directed towards its center while, when using polar coordinates, the polar unit vector ##\hat{r}## is not directed to the center of the osculating circle.

As Chestermiller suggests, we can always with the dot product between the polar unit vector and the tangential unit vector but that is an extra step.
 
fog37 said:
As Chestermiller suggests, we can always with the dot product between the polar unit vector and the tangential unit vector but that is an extra step.
I didn't say polar unit vector. I said normal unit vector.
 
You did. But the unit radial vector ##\textbf{i}_r## is not necessarily normal to the trajectory of the moving particle, correct? The vector ##\textbf{i}_r## is normal to the angular unit vector ##\textbf{i}_\theta##.
 
fog37 said:
You did. But the unit radial vector ##\textbf{i}_r## is not necessarily normal to the trajectory of the moving particle, correct? The vector ##\textbf{i}_r## is normal to the angular unit vector ##\textbf{i}_\theta##.
That’s what my equations indicate. So?
 
Nothing wrong mathematically indeed, just noticing that when many intro physics book talk/introduce the concepts of centripetal and tangential accelerations as vector components of the acceleration vector they implicitly use the local intrinsic unit vectors and intrinsic basis ##(T,N,B)## to express them and not other coordinate systems like cylindrical, spherical or rectangular.

The rate of change of the three unit vectors ##(T,N,B)## are called the Frenet equations...
 

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