Looking down on the pole. East is counterclockwise. Parallel radius is R cos φ — the only lever arm Earth gives you. Tangential speed is ω R cos φ.
Latitude increment, same heading
81.6m/s
183 mph. That is the rotation story. Not 500.
Pad A east speed
408.7 m/s
Pad B east speed
327.1 m/s
vrot(φ) = veq cos φ
Pad A
Cape Canaveral
Florida
- cos φ
- 0.8788
- v_rot due east
- 408.7 m/s
Pad B
Canso
Nova Scotia
- cos φ
- 0.7034
- v_rot due east
- 327.1 m/s
Mission
Losses 1.70 km/s combined
Falcon-class sea-level east LEO: gravity ~1.2–1.5, drag ~0.1–0.3, steering ~0.05–0.15. Same losses at both pads unless the trajectory is wind-loaded.
What the rocket must supply
Δvveh = v + Δvg + Δvd + Δvs − vrot
burn 9076 · Earth gives 409 · inertial target 9484
burn 9157 · Earth gives 327 · inertial target 9484
- v insert
- 7784 m/s
- Losses
- 1700 m/s
- Δv_veh A
- 9076 m/s
- Δv_veh B
- 9157 m/s
Vehicle Δv difference: 81.6 m/s — equal to Δv_lat when both pads fly due east with the same losses.
Inclination — the equation that actually hurts
imin = |φ| · Δvpc = 2 v sin(Δi / 2)
A short east burn from latitude φ yields i = φ. Canso’s proper product is i ≥ 45.3° (including polar and SSO). Then Δv_pc = 0 and you only pay the rotation term.
Pad A
i = 28.5° · A = 90°
cos i = cos φ sin A. Useful rotation 409 m/s.
Pad B
i = 45.3° · A = 90°
cos i = cos φ sin A. Useful rotation 327 m/s.
Payload sensitivity
mf/m0 = e−Δv / v_ev_e = I_sp g_0
Stack sized for pad A. Dry mass held fixed. Extra Δv at pad B is taken out of payload. v_e = 3138 m/s.
95%
Pad B payload relative to a pad-A-sized stack.
Rotation vs latitude
v_rot = 465.10 cos φ · due east
|φA| = 28.5° → 408.7 m/s (914 mph). |φB| = 45.3° → 327.1 m/s (732 mph).
Constants and boxed equations
1. Constants
μ = 3.986004418×1014 m³ s⁻² · R_E = 6.378137×106 m · ω = 7.2921150×10⁻⁵ rad s⁻¹
v_eq = ω R_E = 465.10 m/s
2. Rotation you actually get (due east)
v_rot(φ) = v_eq cos φ
3. Speed you must reach in orbit
v_circ = √(μ / (R_E + h))
vis-viva: v = √(μ (2/r − 1/a)) · a = (r_p + r_a)/2
4. What the rocket must supply
Δv_veh = v_circ + Δv_g + Δv_d + Δv_s − v_rot(φ)
5. Inclination
i_min = φ · Δv_pc = 2 v sin(Δi / 2) · cos i = cos φ sin A
6. Payload
m_f / m_0 = e−Δv / v_e · v_e = I_sp g_0