ISSN 0018ꢀ1439, High Energy Chemistry, 2011, Vol. 45, No. 1, pp. 18–24. © Pleiades Publishing, Inc., 2011.
Original Russian Text © E.M. Kholodkova, A.V. Ponomarev, 2011, published in Khimiya Vysokikh Energii, 2011, Vol. 45, No. 1, pp. 21–27.
RADIATION CHEMISTRY
Formation of Furans upon ElectronꢀBeam Heating of Cellulose
E. M. Kholodkova and A. V. Ponomarev
Frumkin Institute of Physical Chemistry and Electrochemistry, Russian Academy of Sciences,
Leninskii pr. 31, Moscow, 119991 Russia
eꢀmail: ponomarev@ipc.rssi.ru
Received June 30, 2010
Abstract—Similarity between cotton cellulose and sulfate and sulfite pine celluloses in degradation during
electronꢀbeam distillation has been shown. The yield of the distillate liquid slightly depends on the type of
cellulose and makes up ~60 wt %. The product liquid contains organic compounds with molecular masses of
32 to 128, of which furfural and its derivatives prevail. Electronꢀbeam distillation can be used as an effective
method for the manufacturing of furfural and other furan derivatives from cellulose (along with the traditional
pentosan conversion processes). It has been shown that grinding and preheating of cellulose lead to an
increase in the proportion of furfural and other furans in the condensates.
DOI: 10.1134/S0018143911010085
INTRODUCTION
sweep width 245 mm, scanning frequency of 1 Hz).
Irradiation was carried out at atmospheric pressure
without air in 100ꢀml cylindrical quartz vessels. The
reaction vessels were filled to 60% of their volume at an
average packing density of 0.15 g/ml. The electron
beam was scanned along the vertical axis of the vessel.
The vapors were condensed in the air and waterꢀ
Destructive distillation initiated by radiation heatꢀ
ing with a fastꢀelectron beam (electron beam distillaꢀ
tion) is of interest as an efficient means of conversion
of lignocellulose raw materials into furans, phenols,
and acyclic carbonyl compounds demanded by a variꢀ
ety of chemical and fuel industries [1]. Concerning the
problem of deep processing of renewable raw materiꢀ
als, it is of primary importance to reveal of the basis
features of degradation of cellulose, which is the key
structural component of cell walls in all plants [2]. In
this work, we investigated the efficiency of electronꢀ
beam conversion of cellulose into liquid organic comꢀ
pounds, depending on temperature, degree of commiꢀ
nution, and the type of feedstock.
cooled condensers (at 16 2
°С
and 15 2 С, respecꢀ
°
tively) outside of the irradiation zone. To study the
temperature dependence, the O2 samples were preꢀ
liminary thermostated in a muffle furnace over 30 min.
To avoid the initiation of pyrogenetic dry distillation of
the samples, the preheating temperature was mainꢀ
tained not higher than 250
С.In this case, the preheatꢀ
°
ing step was immediately followed by electronꢀbeam
heating. Dosimetry was performed with the use of a
copolymer containing a phenazine dye SO PD(F)Rꢀ
5/50 (GSO (State Standard Sample) 7865ꢀ2000). The
EXPERIMENTAL
average dose rate
Р was 2.1 kGy/s. Distillation prodꢀ
Cotton cellulose (O1) according to GOST (State
Standard) 5556ꢀ81; pine unbleached sulfate pulp
(O2), GOST 12765ꢀ88; and pine bleached sulfite pulp
(O3) according to GOST 3914ꢀ89 were studied. Celluꢀ
ucts were determined chromatographically on a “Perꢀ
kin Elmer AutoSystem XL” instrument (the carrier gas
helium, glass capillary column of 60 m length and an
internal diameter of 0.25
µ
m, mass spectrometer and
lose samples were dried at 107
С and deaerated. To
°
thermal conductivity detectors).
study the dependence of electronꢀbeam distillation on
the degree of grinding of raw materials, O2 samples
with a specific surface area of 49–104 cm2/g (shredꢀ
ding by cutting sheets of EKBꢀ1 cardboard) were used.
The effect of the type and the initial temperature of
RESULTS AND DISCUSSION
According to telemetric observation data, the O1,
cellulose was studied using samples with a specific surꢀ O2, and O3 samples do not significantly differ in the
face area of 104 4 cm2/g. Distillation was initiated by dynamics of electronꢀbeam distillation. Heavy vapor
the radiation heating of samples with fast electrons begins to flow from the reaction vessel to the conꢀ
generated by a UELVꢀ10ꢀ10T linear accelerator denser and the receiving container at a dose of
(energy 8 MeV, pulse duration 6
µ
s, pulse repetition ~250 kGy. Its color varies from the original white to
frequency of 300 Hz, average beam current
≤800
µ
A, bright yellow. The formation of vapor and the rise of
18