Lagrangian statistics have been obtained from large eddy simulations o
f fully developed turbulent channel flow, Calculations were performed
at Reynolds numbers of 3200 and 21,900 (based on centerline velocity a
nd channel half-width); statistics of the Eulerian velocity field are
in good agreement with both direct numerical simulation data and exper
imental measurements. Single-particle Lagrangian velocity autocorrelat
ions and particle mean-square dispersion were obtained from trajectori
es measured for 5000 fluid elements initially in either the viscous su
blayer, buffer layer, or logarithmic region. The Lagrangian velocity a
utocorrelation of particles initially located in the log region decrea
ses less rapidly than for particles initially in the buffer layer, whi
ch in turn decreases more slowly than for particles initially in the v
iscous sublayer. The ratio of the Lagrangian to Eulerian integral time
scales were found to be proportional to the inverse of the turbulence
intensity, in agreement with theoretical predictions and atmospheric m
easurements. Growth of particle mean-square dispersion at long diffusi
on times is propertional to time and in agreement with theory (with th
e exception of the surface-normal coordinate in which the presence of
the channel wall limits dispersion). However, extremely long transport
times are required to achieve the asymptotic state for the dispersion
.