Processing math: 100%

TAM 212: Introductory Dynamics

Coordinate system comparison #rkm

The different coordinate systems and bases have different strengths and weaknesses, and no single coordinate system or basis is always best. Depending on the application, several different coordinate systems or bases may be used simultaneously for different purposes.

NameCoordsBasisProsCons
Cartesian x,y,z ˆı,ˆȷ,ˆk
  • No singularities or discontinuities
  • Fixed for all time
  • Easy differentiation
  • Independent of origin choice
  • No insight into dynamics
Cylindrical
or polar
R,θ,z
or r,θ
ˆeR,ˆeθ,ˆez
or ˆer,ˆeθ
  • Ideal for circular and helical movement
  • Gives insight into centripetal and coriolis acceleration
  • Good if there is a clear motion center with 2D (single-axis) rotation
  • Singularity when r=0
  • Dependent on origin choice
  • Complex differentiation
Spherical r,θ,ϕ ˆer,ˆeθ,ˆeϕ
  • Ideal for rotations in 3D
  • Good if there is a clear motion center with 3D (multi-axis) rotation
  • Singularity when r=0, ϕ=0, or ϕ=π
  • Dependent on origin choice
  • Complex differentiation
Tangential/
normal
ˆet,ˆen,ˆeb
  • Decomposes acceleration into speed and direction changes
  • Allows computation of radius of curvature
  • Independent of origin choice and orientation
  • Discontinuous when curve direction changes
  • Not uniquely defined when a is parallel to v
  • Complex differentiation

Warning: Coordinate systems and bases are different. #rkm‑wc

2D Motion #rkm‑s2

Movement: circle var-circle ellipse arc
trefoil eight comet pendulum
Show:
Coords: none Cartesian polar
Basis: none Cartesian polar tangential/normal
Origin: O1 O2
Components:

Comparison of coordinate systems and bases in 2D. #rkm‑f2

3D Motion #rkm‑s3

Movement: saddle Viviani eight clover
Lissajous deltoid pentagram
Show:
Coords: none Cartesian cylindrical spherical
Basis: none Cartesian cylindrical spherical tang./norm.
Origin: O1 O2
Components:

Comparison of coordinate systems and bases in 3D. #rkm‑f3