388 | Nature | Vol 584 | 20 August 2020
Article
during the sol–gel transition (Extended Data Fig. 3a). The ink has
a shelf life of more than 20 days (Extended Data Fig. 2e, f ). During
printing, the ink flows easily through the nozzle because of shear
thinning, but the filament retains its shape after printing because
of the rapid viscosity increase in the absence of shear. Objects have
been printed with filament and nozzle diameters as low as 100 μm
(Extended Data Fig. 3b). Smaller diameters should be feasible, given
the particle size of the aerogel powder (Fig. 1f), provided the printing
system can operate at sufficiently high pressure. A silica sol, incor-
porated in the ink before printing, is activated with ammonia vapour
after the object has been printed to bind the aerogel particles and fill
the interstitial voids with silica gel. The printed gel may optionally be
hydrophobized before the solvent is removed by supercritical CO 2
drying. MnO 2 (ramsdellite) microspheres are mixed into some of the
inks to illustrate the ease of functionalization (light absorption or
photothermal catalysis)^28 ,^29.
We printed various aerogel objects with high shape fidelity and preci-
sion (Fig. 2a–c, e), including honeycombs, 3D lattices and multi-layered
continuous membranes. The printed filaments retain a circular
cross-section with a well-defined diameter (for example, 327 ± 6 μm).
The rheology of the ink can be adapted to the application: higher vis-
cosity for open structures with large overhangs (up to 45°) and wide
spans (for example, 10 mm for a filament with a diameter of 400 μm)
(Fig. 2d); lower viscosity to enable filaments to merge into continuous
membranes without voids (Fig. 2e). The original aerogel grains are
embedded in, and infused by, a low-density aerogel matrix derived from
G′
G′′
G′
, G
′′ (Pa)
Shear stress (Pa)
100 101 102 10 –3
10 –2 10 –1
100
101
102
103
104
105
10 –1
100
101
102
103
104
105
106
10 –2 10 –1 100 101 102 103 10 –4 10 –3 10 –2 10 –1 100 101 102 103 104
0
2
4
6
8
10
12
Volume (%
)
Particle size (μm)
In air ow
In isopropyl alcohol
NH 3 vapour
Direct ink writing
Ink
Conical
nozzle
Gelation
Supercritical
CO 2 drying
SiO 2 aerogel particles MnO 2 spheres SiO 2 colloids
a
b
f
c
g h
d e
Apparent viscosity (Pa s)
Shear rate (s–1)
SP1.4
SP1.6
SP2.5
SP1.3M0.9
pH < 3 pH > 4
Fig. 1 | Additive manufacture of silica aerogel by direct ink writing.
a, Scheme for direct ink writing of silica aerogels. The inks, either neat (blue) or
functionalized with, for example, MnO 2 nanoparticles (gold), are printed
pneumatically through micronozzles. The printed objects are gelled by a
vapour-based pH change, and dried from supercritical CO 2. b, 3D lotus f lower
of silica gel printed from ink SP2.5 (Extended Data Table 1) through a conical
nozzle with an inner diameter of 410 μm, with a f low rate of 15 mm s−1.
The f lower is printed using 38 layers; printing took 26 min. Supplementary
Video 1 shows a high-speed version of the printing process. c–e, Photographs
of the hydrogel from b before solidification (c), after ammonia-vapour-induced
gelation (d) and after drying (e). f, Particle size distribution for the silica
aerogel. g, Shear-thinning behaviour of different inks. h, Storage (G′) and
loss (G′′) modulus versus shear stress for the different inks.