SEM image of silica material Run 8b (Figure 3a)
with 5000 times magnification shows the material has
a particle shape in the form of a mixture consisting of
dispersed spherical spherical particles ( sign) and
particles in the form of thin sheets that blend together
to form wrinkled roundabouts and multiples (sign ).
There are also particles that have thin skin / walls that
are susceptible to damage forming sheets (Liu H,
2010)
SEM photo of silica material Run 9b with a
magnification of 15,000 times (Figure 3b) shows
spherical particles of small size having a uniform
shape to form together to form a tight and compact
surface so that there are no gaps between particles. An
increase in the ratio of the amount of methanol added
seems to have an effect on particle size. The particle
size of Run 9b is smaller than the particle size of Run
8b. SEM image of silica material Run 10b with 5000
times magnification (Figure 3c) shows spherically
shaped particles forming an aggregate ( sign) and
also there is a particle shape in the form of large
chunks ( sign) and between particles there is a gap
( sign).
SEM image of silica material Run 11b with 5000
times magnification showing spherical particle shape
that is uniform in shape and dispersed with a more
perfect particle shape. Particle size is greater than
particle size Run 9b and Run 10b.
3.1.4 Adsorption-desorption Isotherm
Nitrogen
Porosity analysis of mesoporous silica material and
pore size distribution of Run 8b, Run 9b, Run 10b and
Run 11b were carried out by desorption nitrogen
analysis with isotherm at -196C. The isotherm
adsorption graph was calculated using the Brunauer-
Emmet-Teller (BET) method (Figure 4) and the pore
size distribution was calculated using the Barret-
Joyner-Halenda (BJH) method (Figure 5). Based on
Figure 4, the desorption isotherm adsorption chart
from Run 8b (black graph) shows a graph of
desorption of Type IV adsorption isotherms
according to the IUPAC classification, this is also
adjusted to the literature (Khalil, 2007). The type of
loop hysteresis is caused by the pores in the non-
turbulent aggregate of the particles which results in
slit-shaped pores according to the literature (Shah,
2009). While the desorption adsorption isotherm
graph from Run 9b (red graph) shows Type IV
desorption isotherm adsorption according to the
IUPAC classification is characteristic for mesoporous
material (Khalil, 2007). The existence of a hysteresis
loop is due to the narrow pore gap and includes the
pore of the micropore region, according to the
literature (Shah, 2009). The adsorption isotherm
adsorption graph from Run 10b (blue graph) shows
adsorption of Type IV isotherm according to the
IUPAC classification which is characteristic for
mesoporous material (Khalil, 2007). Pore adsorption
is a type of capillary condensation having a hysteresis
loop which can be caused by channels such as
cylinders or pores formed from coarse homogeneous
spheres forming tight agglomerates according to the
literature (Shah, 2009). Then the adsorption
desorption graph isotherm Run 11b (green graph)
shows adsorption of Type IV isotherm according to
the IUPAC classification which is a characteristic of
mesoporous material (Khalil, 2007). The presence of
a hysteresis loop can be caused by pores formed from
pore channels such as cylinders or pores from coarse
homogeneous sphere particles according to the
literature (Shah, 2009).
Figure 4: Adsorption desorption graph isotherm
nitrogen silica material from Run 8b, Run 9b, Run
10b and Run 11b.
Based on Figure 5, a graph of the pore size
distribution of silica material Run 8b (black graph)
shows a non-uniform pore size distribution in the
range between 1.44 nm to 9.53 nm, this is according
to SEM analysis. Mesopore silica material consists of
mixed particle forms so produced various pore
shapes. The pore size distribution chart of the silica
material Run 9b (red graph) shows that the pore size
distribution is not uniform from 1.43 nm to 9.53 nm.
This is in accordance with SEM photos that show the
form of particles that combine to form a compact and
tight surface. The particle size distribution chart of
silica material Run 10b (blue graph) shows a regular
pore size distribution (uniform) dominated by pore
size at 2.76 nm and 3.07 nm. This is consistent with
SEM photos where dominant particles are spherically
shaped in small sizes. The pore size distribution chart
for silica material Run 11b (green graph) shows a