Numerical relativity codes now being developed will evolve initial dat
a representing colliding black holes at a relatively late stage in the
collision. The choice of initial data used for code development has b
een made on the basis of mathematical definitiveness and usefulness fo
r computational implementation. By using the ''particle limit'' (the l
imit of an extreme ratio of masses of colliding holes) we recently sho
wed that the standard choice is not a good representation of astrophys
ically generated initial data. Here we show that, for the particle lim
it, there is a very simple alternative choice that appears to give exc
ellent results. That choice, ''convective'' initial data, is, roughly
speaking, equivalent to the start of a time sequence of parametrized s
olutions of the Hamiltonian constraint; for a particle in circular orb
it, it is the initial data of the steady state solution on hypersurfac
e. The implementation of related schemes for equal mass holes is discu
ssed.