Problem (polar destroyer):
(ds/dt)^2 = (dx/dt)^2 + (dy/dt)^2
= r^2 (dθ/dt)^2 + (dr/dt)^2
(√3/ t) dt = d θ
(√3 ln t) + c= θ
√3 ln (⅕) + c = 0
c = -√3 ln (⅕)
θ(t) = (√3 ln t) - √3 ln (⅕)
recall: r/15 = t
θ(r) = (√3 ln r/15) - √3 ln (⅕)
θ(r) = √3 ln (r/3)
r = 3e^(θ/√3)
Time:
max θ = 2 π
max t of curve = ⅕(e^(2π/√3))
upper bound of T): ⅕(e^(2π/√3)) + ⅕
Visualize solution (logarithmic curve) of DE for problem of two bodies in 2D space. Final project for MATH 206.
Logarithmic spiral has many special properties: Self-similarity (i.e. zooming out makes rotation of itself) Turnings of a logarithmic spiral increase in geometric progression Constant angle between an intersecting circle centred at the origin and a logarithmic spiral
Particularly, these properties imply that when you increase the radius (ex. circle), there will be a constant angle of rotation no matter what size the circle is.
Same pattern as hawks circling to catch prey, or hurricane!