Natural composite materials are renowned for their mechanical strength and
toughness: despite being highly mineralized, with the organic component con
stituting not more than a few per cent of the composite material, the fract
ure toughness exceeds that of single crystals of the pure mineral by two to
three orders of magnitude(1). The judicious placement of the organic matri
x, relative to the mineral phase, and the hierarchical structural architect
ure extending over several distinct length scales both play crucial roles i
n the mechanical response of natural composites to external loads(.)(2-4) H
ere we use transmission electron microscopy studies and beam bending experi
ments to show that the resistance of the shell of the conch Strombus gigas
to catastrophic fracture can be understood quantitatively by invoking two e
nergy-dissipating mechanisms: multiple microcracking in the outer layers at
low mechanical loads, and crack bridging in the shell's tougher middle lay
ers at higher loads. Both mechanisms are intimately associated with the so-
called crossed lamellar microarchitecture of the shell, which provides for
'channel' cracking in the outer layers and uncracked structural features th
at bridge crack surfaces, thereby significantly increasing the work of frac
ture, and hence the toughness, of the material. Despite a high mineral cont
ent of about 99% (by volume) of aragonite, the shell of Strombus gigas can
thus be considered a 'ceramic plywood', and can guide the biomimetic design
of tough, lightweight structures.