Scaled sandbox experiments with high basal friction, simulating the gr
owth of accretionary wedges, display cycles alternating between fronta
l imbricate thrusting and underthrusting of long, undeformed sheets, B
y contrast, low basal friction experiments with otherwise similar and
constant, initial conditions produce a classic frontal imbricate fan t
hrough repeated failure along frontal thrusts, The cyclical behavior o
bserved in high basal friction experiments is expressed by three quant
ities: (1) the average spacing between frontal thrusts, (2) the advanc
e and retreat of the deformation front, and (3) the frontal slope (a)
of the actively deforming wedge, As a long sheet is underthrust, the f
ront is steepened through slumping until the maximum critical angle is
reached, Then frontal thrusting resumes and the accretion of imbricat
e slices builds the wedge forward, thereby lowering the taper to the m
inimum critical angle. At shallow tapers, a long unit is underthrust a
nd subsequently uplifts, shortens, and steepens the overlying wedge th
rough backthrust deformation, thus completing the cycle. Underthrustin
g of long units offers a simple mechanism for underplating overlying u
nits, It also provides a possible explanation for temporally and spati
ally varying wedge geometries in nature, when basal frictions attain 8
0%-90% of the internal friction.