The M-component mode of charge transfer to ground is examined using (1) mul
tiple-station measurements of electric and magnetic fields at distances ran
ging from 5 to similar to 500 in from triggered-lightning channels and (2)
measured currents at the channel base. Data have been obtained in 1997, 199
9, and 2000 at the International Center for Lightning Research and Testing
at Camp Blanding, Florida, for (1) "classical" M-components that occur duri
ng the continuing currents following return strokes and (2) impulsive proce
sses that occur during the initial stage of rocket-triggered lightning and
are similar to the "classical" M components. All lightning events considere
d here effectively transported negative charge to ground. For one triggered
-lightning event the electric field 45 km from the lightning channel was me
asured together with the current and close fields. The shapes and magnitude
s of the measured close electric and magnetic fields are generally consiste
nt with the guided-wave mechanism of the lightning M component. Specificall
y, the M-component electric field peak exhibits logarithmic distance depend
ence, ln(kr(-1)), which is indicative of a line charge density that is zero
at ground and increases with height. Such a distribution of charge is dist
inctly different from the more or less uniform charge density that is chara
cteristic of the dart leaders in triggered lightning, as inferred from clos
e electric field measurements. The M-component magnetic field peak decrease
s as the inverse distance (i.e., r(-1)), which is generally consistent with
a uniform current within the lowest kilometer or so of channel. The M-comp
onent electric field at 45 km appeared as a bipolar, microsecond-scale puls
e that started prior to the onset of the M-component current at the channel
base. M-component-type processes can produce acoustic signals with peak pr
essure values of the same order of magnitude as those from the leader/retur
n stroke sequences in triggered lightning.