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Derive deflection angle of transition curve

Short answer

For a cubic spiral with ρl = RL, the spiral angle φ = l²/(2RL), coordinates x ≈ l, y ≈ l³/(6RL). The deflection angle δ = y/x ≈ l²/(6RL) radians, which converts to 573 l²/(RL) minutes.

Prove the deflection angle of transition curve is α=573 l2RL\alpha = \frac{573\,l^2}{RL} mins where symbols have their usual meaning.

Transition curve (cubic spiral)

A transition curve connects a straight with a circular curve so that the radius changes gradually from ∞\infty to RR. The radius at a distance ll from the start is inversely proportional to ll:

ρ∝1l⇒ρ l=RL\rho \propto \frac{1}{l} \quad\Rightarrow\quad \rho\, l = RL

where RR is the radius of the circular curve and LL is the length of the transition curve.

        y
        |        . P(x, y)
        |     .  
        |  .    deflection angle = delta
   T1 --+-----------------------> x   (tangent)

Derivation

Take T1 (start of the curve) as the origin and the tangent as the x-axis. For a point P at a distance ll along the curve, the tangent angle (spiral angle) ϕ\phi is given by dϕ=dlρ=l dlRLd\phi = \dfrac{dl}{\rho} = \dfrac{l\,dl}{RL}:

ϕ=∫0ll dlRL=l22RL\phi = \int_0^l \frac{l\,dl}{RL} = \frac{l^2}{2RL}

The coordinates of P are, for small ϕ\phi (cos⁡ϕ≈1\cos\phi \approx 1, sin⁡ϕ≈ϕ\sin\phi \approx \phi):

dx=dl,dy=ϕ dl=l22RL dldx = dl,\quad dy = \phi\,dl = \frac{l^2}{2RL}\,dl x≈l,y=∫0ll22RL dl=l36RLx \approx l, \qquad y = \int_0^l \frac{l^2}{2RL}\,dl = \frac{l^3}{6RL}

This is the equation of a cubic parabola.

The deflection angle δ\delta at T1 between the tangent and the line T1P:

tan⁡δ=yx=l36RL⋅l=l26RL\tan\delta = \frac{y}{x} = \frac{l^3}{6RL\cdot l} = \frac{l^2}{6RL}

As δ\delta is small, tan⁡δ≈δ\tan\delta \approx \delta (in radians):

δ=l26RL radians\delta = \frac{l^2}{6RL}\ \text{radians}

Converting radians to minutes: 1 rad=180π×60=3437.75′1\ \text{rad} = \dfrac{180}{\pi}\times 60 = 3437.75':

δ=3437.756⋅l2RL=572.96 l2RL≈573 l2RL minutes\delta = \frac{3437.75}{6}\cdot\frac{l^2}{RL} = 572.96\,\frac{l^2}{RL} \approx \boxed{\frac{573\,l^2}{RL}\ \text{minutes}}

Hence proved.

At the end of the transition (l=Ll = L): δL=L6R\delta_L = \dfrac{L}{6R} rad =ϕs3= \dfrac{\phi_s}{3}, where ϕs=L2R\phi_s = \dfrac{L}{2R} is the spiral angle. This is the usual check on the last peg.

✓ Answer checked by Claude Opus 5.5 (high effort)

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