Hi Kieron,
I got the height of maximum deceleration wrong in my previous post.
Im not sure this is a correct representation of Öpik's equations, but it makes some sense. The following is based on a 20Kg stone (about 20 cm across at the start) entering the Earth's atmosphere at 30 degrees from horizontal and with velocities of 12, 16 and 20 km/s.
Remaining as a single body, only a fraction of the slower body survives to the ground - about 0.5 kg. The bodies with greater initial velocities are fully ablated, but see below.
- Mass remaining (kg)
The quicker the entry velocity the less time there is to loose mass early in the meteoric flight.
- Velocity remaining (km/s)
As a consequence, the deceleration is more dramatic for the quicker entries and almost certainly the rock would not survive as one piece. There'd be fragmentation and each fragment would loose part of its cosmic velocity. Fragmentation would start at 55 km, for a relatively robust object entering at 20km/s, and higher for quicker and less robust objects.
- Deceleration (g)
Looking at my calculations, I see that I haven't applied the "jet correction factor" (see Opik equation 4-68) to the deceleration calculation. As I say, I'm not sure the rest is correct, but if anyone fancies working on this, I'd be happy to pass on what I've done. It's written in a handful of Java objects. I have a copy of G. W. Wetherill and D. O. ReVelle's
Which fireballs are meteorites? A study of the Prairie Network photographic meteor data, which would be a good place to start looking to validate the model.