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C A R B O N 4 7 ( 2 0 0 9 ) 1 0 1 2 – 1 0 1 7
. sc iencedi rec t .com
ava i lab le at wwwjournal homepage: www.elsevier .com/ locate /carbon
Using alkali metals to control reactivity and porosity duringphysical activation of demineralised kraft lignin
Suhas, P.J.M. Carrott*, M.M.L. Ribeiro Carrott
Centro de Quımica de Evora e Departamento de Quımica, Universidade de Evora, Colegio Luıs Antonio Verney, 7000-671 Evora, Portugal
A R T I C L E I N F O
Article history:
Received 13 October 2008
Accepted 1 December 2008
Available online 10 December 2008
0008-6223/$ - see front matter � 2008 Elsevidoi:10.1016/j.carbon.2008.12.001
* Corresponding author: Fax: +351 266745303E-mail address: [email protected] (P.J.M. Ca
A B S T R A C T
Demineralised kraft lignin was impregnated with between 6.2% and 50% NaCl or KCl and
physically activated in CO2 at 750 �C. The results presented show that a considerable reduc-
tion in activation time even at a comparatively low activation temperature could be
achieved, particularly when using KCl. Considering a fixed level of burn-off, the impregna-
tion did not affect the pore volume and only increased the pore width by about 0.1–0.2 nm,
depending on the concentration of NaCl or KCl used. By controlling the conditions it was
possible to obtain predominantly ultramicroporous materials with mean pore widths over
the range 0.53–0.77 nm. On the other hand, at high levels of burn-off there was evidence for
micropore widening into the small mesopore range and also for the formation of a second-
ary mesopore structure. Under these conditions it was possible to obtain materials with
pore volumes as high as 0.82 cm3 g�1.
� 2008 Elsevier Ltd. All rights reserved.
1. Introduction
Lignin is one of a wide variety of bioresources that has been
used to produce activated carbons [1–7]. For a given type of acti-
vation method, the precise properties of the product and the
optimum operating conditions will depend on the molecular
structure of the biopolymers present and also on the presence
of inorganic impurities (ash) [8]. For instance, in the specific
case of physical activation of lignin with CO2, higher micropore
volumes and narrower micropore widths can be obtained from
pure hydrolytic lignin or demineralised kraft lignin than from
impure raw kraft lignin [9]. The disadvantage is that ash free
lignin is extremely non-reactive. For instance, it was found
that a burn-off of 20% could be reached after about 1 h at
750 �C using raw kraft lignin but over 16 h were needed with
demineralised kraft lignin [9]. This difference in reactivity is
probably due to the presence of sodium, which is a known car-
bon gasification catalyst, and is the main impurity in kraft lig-
nin [10–14]. Evidence that this is the case has come from a
recent preliminary study where addition of NaCl to deminera-
lised kraft lignin was found to increase the reactivity again [15].
er Ltd. All rights reserved
.rrott).
Surprisingly, however, the deliberate addition of NaCl did not
adversely affect the porosity of the product. That is, the effect
of sodium seems to be associated not only with the amount
present but also with the manner in which it is incorporated
into the lignin. It occurred to us that impregnating deminera-
lised lignin with sodium under controlled conditions could
be an effective way to obtain activated carbons with good
porosity characteristics but with a much reduced period at
comparatively low activation temperature, thereby reducing
considerably the energy costs associated with the activation
process. A more systematic study of the effect of the alkali
metals sodium and potassium and the alkali earth metal cal-
cium on the activation of demineralised kraft lignin was there-
fore carried out and the results are presented in this paper.
2. Experimental
2.1. Materials and methods
The kraft lignin sample, designated alfa lignin, was obtained
from Lignotech Iberica and is similar to that used in previous
.
C A R B O N 4 7 ( 2 0 0 9 ) 1 0 1 2 – 1 0 1 7 1013
work [9,10,15,16]. In order to eliminate the mineral content,
10 g of alfa lignin was treated with 500 mL 1% H2SO4 with con-
tinuous stirring at 300 rpm for 1 h at room-temperature and
then kept overnight. The dispersion was then filtered and
washed with 500 mL 1% H2SO4 followed by �1 L distilled
water. Finally the treated sample, designated alfa-A, was
dried overnight at 110 �C and stored in sample flasks for fur-
ther use. The ash content, determined according to ISO stan-
dard 1171, was 0.2%.
Impregnation of alfa-A with KCl, NaCl or CaCl2 was carried
out by mixing dry lignin and inorganic salt in fixed weight ra-
tios, corresponding to weight percentages of 6.2%, 33% or 50%,
and then adding 25 mL distilled water. The mixture so ob-
tained was stirred, kept overnight for drying, and used for
the preparation of activated carbons.
For the production of the activated carbons about 5 g of
precursor were placed in a ceramic boat and positioned in
the central constant temperature zone of a conventional hor-
izontal tubular furnace. Carbonisation was carried out by
heating to 750 �C at a rate of 8 �C min�1 under a constant
N2 flow of 85 cm3 min�1 and maintaining for 30 min. Physical
activation in CO2 was carried out by switching to a CO2 flow
of 85 cm3 min�1 at the same temperature, maintaining for
the appropriate time at 750 �C in order to obtain samples
with different levels of burn-off, switching back to the N2
flow and allowing to cool to below 50 �C before removing
the product from the furnace. The impregnants were re-
moved by washing with 2 L of distilled water, followed by
drying at 110 �C overnight and were then stored in sealed
sample flasks. The burn-off, X, of the samples was calculated
from
X ¼ 100 ðwo �wÞ=wo ð1Þ
where wo is the weight of carbonised lignin and w is the final
weight of activated carbon after, in both cases, removal of the
impregnant.
2.2. Characterisation
Characterisation of the alfa lignin by thermogravimetric anal-
ysis and FTIR, as well as elemental analyses of C, H, N, S and
O, and humidity and ash determinations according to ASTM
and ISO standards, have been described previously [9,15]. N2
isotherms at 77 K were determined using a CE Instruments
Sorptomatic 1990, using helium (for dead space calibration)
and nitrogen of 99.999% purity supplied, respectively, by Linde
and Air Liquide. Prior to the adsorption measurements all
samples were outgassed for 4 h at 300 �C. The N2 isotherms
were analysed by means of the as method using published
standard data in order to obtain the external surface area,
As, and total pore volume Vs [17]. They were also analysed
by means of the DR equation in order to obtain the DR pore
volume, Vo, and the mean pore width, Lo, from the relation-
ship [18]:
Lo ¼ 10:8=ðEo � 11:4Þ ð2Þ
where Eo is the characteristic energy obtained by application
of the DR equation. The liquid density of N2 was taken as
0.808 g cm�3 and the affinity coefficient as b = 0.34 [19].
3. Results and discussion
3.1. Reactivity
Values of activation time and the corresponding burn-offs are
given in Table 1. The reaction rate, assuming first order
kinetics, is given by –dw/dt = kw. If Eq. (1) is used to replace
the weight, w, by the burn-off, X, it follows that estimates of
the first order rate constants, k, can be calculated as
(ln(1�X/100))/t and these values are shown as a function of
burn-off in Fig. 1. For each sample the value of k obtained is
a mean value averaged over the whole range of burn-off from
0 to X. Nevertheless, the results obtained are in general
agreement with published results from other authors for
pre-carbonised kraft lignin containing 2.1% ash and activated
at the same temperature of 750 �C and determined using a
more rigorous thermogravimetric technique [6].
For the demineralised lignin the value of rate constant ob-
tained was approximately 0.0002 min�1. After impregnation
the rate constant increased by at least 16 times to values
>0.0033 min�1. In a previous study it was found that the k val-
ues were fairly constant over a range of burn-off up to about
55% but then increased significantly at higher burn-offs [6].
The number of data points on Fig. 1 is too small to verify if ex-
actly the same behaviour is observed here. However, it is clear
that the k values are higher for the higher burn-off samples.
In the previous study k values in the approximate range
0.002–0.005 min�1 were reported for activation at 750 �C [6].
It can be seen from Fig. 1 that the range of k values obtained
in this work for burn-offs less than 41% are within the same
range. The results in Fig. 1 also indicate that, considering
the overall trend of the data, the rate constants increase as
the amount of Na or K increases, and that the values for
KCl impregnation are higher than those for NaCl impregna-
tion. Results for CaCl2 are not shown in Fig. 1. However it
was found that the use of this impregnant also resulted in sig-
nificant increases, similar or greater than KCl, in the rate
constants.
These results show that addition of even a relatively low
amount of NaCl, KCl or CaCl2 provokes a significant increase
in the rate constants for the activation and allows degrees of
activation, or burn-offs, to be controlled over a reasonably
short time scale even at the comparatively low activation
temperature of 750 �C.
3.2. Qualitative isotherm analysis
Representative N2 isotherms of chars and activated carbons
prepared from the alfa lignin have been presented previously
[9,15]. Most of the isotherms determined in the present work
were similar and representative examples for low burn-off
and high burn-off samples are shown in Figs. 2 and 3. All of
the isotherms presented Type I character at low relative pres-
sures indicating the presence of microporosity in all samples.
With the low burn-off samples obtained in this work it was
found that the isotherms were highly rectangular and almost
horizontal at relative pressures above 0.02p�, which
confirms that they were predominantly ultramicroporous
materials.
Table 1 – Textural characteristics of the activated carbons obtained from alfa-A lignins on activation in CO2 at 750 �C beforeand after impregnation with NaCl, KCl or CaCl2.a
(%) tact h Burn-off (%) ABET m2 g�1 As m2 g�1 Vs cm3 g�1 Vo cm3 g�1 Lo nm
No impregnation
0 0.5 0.2 520 4 0.17 l.p.h.b l.p.h.b
8 9 742 2 0.24 0.25 0.53
16 19 914 1 0.31 0.30 0.63
20 19 890 3 0.30 0.29 0.59
24 19 889 4 0.30 0.29 0.60
28 22 n.d.c n.d.c n.d.c n.d.c n.d.c
NaCl
6.2 0 0 442 6 0.15 l.p.h.b l.p.h.b
0.5 12 654 9 0.22 0.21 0.58
1 18 797 8 0.28 0.27 0.70
2 40 1111 26 0.45 (0.37)d (0.98)d
3 64 1325 47 0.82 (0.43)d (1.27)d
33 0 0 564 4 0.19 0.19 0.71
0.5 12 810 5 0.28 0.26 0.75
1 22 850 10 0.32 0.28 0.77
2 70 1199 29 0.81 (0.39)d (1.28)d
50 0.5 15 817 4 0.30 0.27 0.74
KCl
6.2 0.5 11 868 11 0.29 0.29 0.70
2 62 1907 19 0.68 (0.60)d (1.78)d
33 0.5 15 903 19 0.29 0.30 0.76
1 56 1454 41 0.61 (0.44)d (1.50)d
CaCl26.2 0.5 – 594 172 0.14 0.20 0.89
33 0.5 17 453 26 0.14 0.15 0.72
2 81 379 52 0.11 0.13 1.11
a tact = activation time, ABET = apparent surface area obtained by BET method, As and Vs = external surface area and total pore volume (in terms
of equivalent liquid volume) obtained by as method, Vo and Lo = micropore volume and mean pore width from DR plot.
b l.p.h. = low pressure hysteresis (see text).
c Not determined.
d Overestimated (see text).
0.000
0.002
0.004
0.006
0.008
0.010
0.012
0.014
0 10 20 30 40 50 60 70X / %
k / m
in-1
Fig. 1 – Variation of first order rate constant, k, for activation
at 750 �C to burn-off of X% of alfa-A lignin impregnated with
NaCl (open symbols) or KCl (full symbols). Circular buttons –
no impregnation. Squares – 6.2%. Triangles – 33%. Diamond
– 50%.
0
5
10
15
20
25
30
0 0.2 0.4 0.6 0.8p/pº
nads
/ m
mol
g-1
1
Fig. 2 – Representative N2 at 77 K adsorption–desorption
isotherms determined on activated carbons prepared at
750 �C from alfa-A lignin impregnated with 33% NaCl.
Squares – 0.5 h activation. Circles – 2 h activation. Open
symbols – adsorption. Full symbols – desorption.
1014 C A R B O N 4 7 ( 2 0 0 9 ) 1 0 1 2 – 1 0 1 7
With regard to the high burn-off samples, it is clear from
Figs. 2 and 3 that their pore size distributions were consider-
ably broader than those of the low burn-off samples and ex-
tended into the mesopore region. Furthermore, the extent of
pore widening was clearly much greater when the lignin
was impregnated with NaCl rather than KCl.
0
5
10
15
20
25
30
0 0.2 0.4 0.6 0.8p/pº
nads
/ m
mol
g-1
1
Fig. 3 – Representative N2 at 77 K adsorption–desorption
isotherms determined on activated carbons prepared at
750 �C from alfa-A lignin impregnated with 33% KCl.
Squares – 0.5 h activation. Circles – 1 h activation. Open
symbols – adsorption. Full symbols – desorption.
0.0
0.2
0.4
0.6
0.8
1.0
0 10 15 20 25
X / %
L o /
nm
5
Fig. 4 – Variation of mean micropore width estimated by the
DR method with increasing burn-off, X, for activated carbons
prepared from alfa-A lignin impregnated with NaCl (open
symbols) or KCl (full symbols). Circular buttons – no
impregnation. Squares – 6.2%. Triangles – 33%. Diamond –
50%. Solid lines – trend lines.
C A R B O N 4 7 ( 2 0 0 9 ) 1 0 1 2 – 1 0 1 7 1015
It can be seen from Fig. 2 that the hysteresis loop on the
isotherm of the high burn-off NaCl impregnated sample has
a step which may be an indication of a bimodal pore size dis-
tribution. On the one hand, increasing burn-off widens the
micropores into the small mesopore range and this gives rise
to a Type H4 hysteresis loop. On the other hand, a secondary
mesopore structure may form at high burn-off giving rise to a
Type H1 or H2 hysteresis loop. Overlapping of the two hyster-
esis loops would give rise to the stepped character seen in
Fig. 2. Additional evidence for the formation of a secondary
mesopore structure is referred to below.
N2 isotherms were also determined on samples impreg-
nated with CaCl2 but are not shown as the uptake was always
significantly lower which indicates that CaCl2 is not a very
interesting impregnating agent in the present context.
3.3. Quantitative isotherm analysis
The results of the analysis of the isotherms by the as and DR
methods are given in Table 1. For the two samples indicated
by l.p.h. in Table 1 it is not appropriate to apply the DR meth-
od due to the presence of low pressure hysteresis. This is
indicative of non-equilibrium conditions at very low relative
pressures and equilibrium equations such as the DR equation
should not therefore be applied over this range of the
isotherm.
For the low burn-off samples, with burn-off <40%, the cor-
responding values of Vs and Vo are in close agreement (within
0.04 cm3 g�1), the values of external surface area (As) are low
and the values of mean micropore width, Lo, are all less than
or close to 0.7 nm. These features provide further confirma-
tion that the low burn-off samples were predominantly
ultramicroporous.
For these low burn-off samples, Fig. 4 shows the variation
of mean micropore width with burn-off and it can be seen
that NaCl or KCl addition causes a small increase. Addition
of 6.2% increases the Lo values by about 0.1 nm, while
addition of 33% or 50% increases Lo by a further 0.1 nm. The
results in Fig. 4 suggest that, in the case of these low burn-
off ultramicroporous materials, there is no significant differ-
ence between NaCl and KCl even though, as already pointed
out above, NaCl appears to provoke significantly more pore
widening in high burn-off samples. In comparison with other
precursor materials, the overall porosity of these low burn-off
activated carbons is similar to that found with activated car-
bons prepared from PAN [20] or cork [21] but slightly inferior
to what it is possible to achieve using Kevlar [22] or phenolic
fibres [23] as precursor where, for a fixed narrow pore size, the
micropore volume is somewhat higher.
For the samples with burn-off >40% larger differences,
especially for the NaCl impregnated samples, were found be-
tween corresponding values of Vs and Vo. In all cases, the for-
mer gives the total pore volume including micropores and
mesopores when they are present. Vo, on the other hand,
gives an estimate of a volume of micropores which includes
ultramicropores and may include some, but probably not all,
supermicropores. It does not include mesopores. Before
applying the DR Equation a correction should be made for
adsorption on the non-microporous surface area [24,25]. If
this is not done, then both Vo and Lo will be overestimated
[26]. A very large error can be involved when mesopores are
present as, even at very low relative pressures, the amount
adsorbed on the high surface area of the mesopore walls
can be comparable to the amount being adsorbed in the
micropores. This is the case with the high burn-off samples
prepared in this work and for this reason the calculated val-
ues of Vo and Lo for these samples are given in parentheses
in Table 1.
As the high burn-off samples contain mesopores we can
obtain an estimate of the maximum pore size of these sam-
ples by applying the Kelvin equation with correction for mul-
tilayer adsorption. In the case of the sample impregnated
with 33% KCl and activated for 1 h the linear region of the cor-
responding as plot began at about 0.6p� and we can assume
that all pores were filled at or below this relative pressure.
On the basis of the data in Ref. [27] and assuming slit-shaped
1016 C A R B O N 4 7 ( 2 0 0 9 ) 1 0 1 2 – 1 0 1 7
pores, this gives a value slightly greater than 3 nm for the
upper limit of pore width. For the sample impregnated with
33% NaCl and activated for 2 h the linear range of the corre-
sponding as plot began at about 0.8p� (including desorption
points) or 0.9p� (only adsorption points). These relative pres-
sures correspond to slit-shaped pore widths of 6 nm or
11 nm, respectively. If cylindrical pores are assumed, instead
of slit pores, these values increase to pore diameters of
10 nm or 20 nm, respectively. It is difficult to imagine that
such large pores would be formed by a normal process of
micropore widening and this therefore seems to provide addi-
tional evidence for the formation of a secondary mesopore
structure at high burn-offs in, at least, the samples impreg-
nated with NaCl.
For both low and high burn-off samples the total pore vol-
ume, Vs, is plotted as a function of burn-off in Fig. 5. It can be
seen that up to about 40% burn-off all of the data lies on a
common line. That is, although the addition of NaCl or KCl
significantly decreased the time needed to achieve a given le-
vel of burn-off, it did not affect the corresponding pore vol-
ume, which increased from 0.19 cm3 g�1 at 0% burn-off up
to 0.45 cm3 g�1 at 40% burn-off. On the other hand, if the line
on Fig. 5 is extrapolated to 70% burn-off, a value of
0.65 cm3 g�1 is predicted, which is lower than the values
determined for 3 of the 4 higher burn-off samples on the fig-
ure. This difference, and the corresponding upward devia-
tions seen on Fig. 5, may be a consequence of the formation
of the secondary mesopore structure.
The results in Fig. 5 are in marked contrast to the behav-
iour of raw alfa lignin, where the micropore volume was
found to reach a maximum of about 0.3 cm3 g�1 at about
20% burn-off and then decreased at higher burn-offs [9]. In
the present work, the total pore volumes always increased
and values greater than 0.8 cm3 g�1 were obtained under
appropriate conditions. These differences confirm that the ef-
fect of alkali metals on the activation does not depend just on
the amount present, but also on the manner in which they are
incorporated in the lignin structure.
0
0.2
0.4
0.6
0.8
0 10 20 30 40 50 60 70X / %
V s /
cm3 g-1
Fig. 5 – Variation of micropore volume estimated by the as
method with increasing burn-off, X, for activated carbons
prepared from alfa-A lignin impregnated with NaCl (open
symbols) or KCl (full symbols). Circular buttons – no
impregnation. Squares – 6.2%. Triangles – 33%. Diamond –
50%. Solid line – trend line for data from 9% to 40% burn-off .
4. Conclusions
The results presented show that a considerable reduction in
activation time even at a comparatively low activation tem-
perature could be achieved by impregnating demineralised
kraft lignin with relatively small amounts of NaCl or KCl.
Higher activation rates were observed when using KCl. Con-
sidering a fixed level of burn-off, the impregnation did not af-
fect the pore volume and only increased the pore width by
about 0.1–0.2 nm, depending on the amount of NaCl or KCl
used. By controlling the conditions it was possible to obtain
predominantly ultramicroporous materials with mean pore
widths over the range 0.53–0.77 nm. On the other hand, at
high levels of burn-off there was evidence for micropore wid-
ening into the small mesopore range and also for the forma-
tion of a secondary mesopore structure. Under these
conditions it was possible to obtain materials with higher
pore volumes up to 0.82 cm3 g�1. The presence of a secondary
mesopore structure in these materials could be advantageous
as it should improve accessibility of adsorptives to the micro-
pore entrances and hence increase rates of adsorption from
the gas or liquid phase.
Acknowledgements
This work was supported by the Fundacao para a Ciencia e a
Tecnologia (Plurianual Finance Project Centro de Quımica de
Evora (619) and post-doctoral Grant SFRH/BPD/20535/2004)
with national and European community (FEDER) funds and
by the Lignocarb Project funded by the European Commission
(Project ALFA-II-0412-FAFI). The authors thank Dr. V. Fierro for
providing the alfa lignin.
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