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