1930
RYBAKOV et al.
of argon. The variation of temperature in the course
of time was recorded with the ChA thermocouple
and a secondary EPP-09 potentiometer. Then the zero
level was set and the loss of mass by the sample in
the course of fluorination was monitored. Fluorine
with the content of the main component of 92
96 vol % was used in the study; argon of A brand
served to dilute fluorine.
Before the experiments, we passivated the setup at
a temperature of 300 400 C and F2 concentration in
argon of about 30 vol % until a stable fluoride film
was formed on the surface. The ChA thermocouple
was placed within a corundum straw, with only its
junction contacting with the fluorine argon mixture.
The error in weighing in the range 0 500 mg did not
exceed 1 2%.
The heterogeneous reaction between metallic Mo
and elementary F2 occurs in accordance with the fol-
lowing overall equation
Fig. 2. Variation of the sample mass, (m
of temperature T in the reaction between metallic molyb-
denum and elementary fluorine with time
m)/m , and
0
0
.
Mo + 3F2
MoF6.
moving the reactor up and down in the furnace.
The iron core of the induction transducer 2 is sus-
pended on the right arm of the balance, and the ther-
mocouple 3 and the reaction boat 4, on the left arm.
At the technological parameters used in actual prac-
tice, the reaction of fluorination is strongly exothermic
and, therefore, certain difficulties were encountered in
experimental data processing. The results obtained
using the procedure we suggested are shown in Fig. 2:
after a stable temperature Ti was reached at an instant
of time i, the derivative of the curve describing
the variation of the sample mass with time was found
The unbalance of the balance leads to motion of
the iron core in the induction coil 2, which gives rise
to an induction voltage proportional to the change in
the mass of the sample as a result of the reaction of
metallic Mo with elementary F2. The induction trans-
ducer 2 is connected into an arm of the differential-
transformer circuit of a DSR-35 instrument. The linear
portion of the plot of the change in mass against
the induction voltage corresponded to variation of
the sample mass in the range 0 500 mg. The con-
version of the metallic Mo was determined from
the loss of mass by the sample as a result of the for-
mation of gaseous MoF6. The variation of the mass of
a sample of metallic Mo was continuously monitored
with a secondary DSR-35 instrument. The completion
of the reaction was judged from termination of varia-
tion of the sample mass.
graphically at
[2]. This derivative is numerically
i
equal to the rate constant of fluorination, kT , at a
temperature Ti. The rate constants were determined
at two temperatures and the apparent activation energy
(kJ mol ) of the heterogeneous reaction between
powdered Mo and elementary F2 was calculated using
the equation
i
1
kT
19.1479T2T1
2
E =
log
.
(1)
kT
T2 T1
1
We carried out more than 40 experiments, and typ-
ical S-shaped curves describing the variation of
the mass of metallic Mo in the course of fluorination
were obtained. During the first 2 min, there is no re-
action, i.e., an induction period is observed. Further,
the sample mass somewhat increases because of the
formation of solid molybdenum fluorides MoF5 and
MoF4. Then volatile MoF6 starts to be formed, which
leads to a decrease in the sample mass.
A weighed portion ( 400 mg) of powdered metallic
molybdenum (particle size 20 50 m) was charged
into a cylindrical nickel boat 15 mm in diameter and
3 mm high. The boat with the sample was attached
with a special clamp to the suspended Chromel
Alumel (ChA) thermocouple so that the thermojunc-
tion was close to the sample surface.
After that the fluorination reactor was hermetically
sealed and heated to a required temperature in a flow
We processed the results of the experiments on
the kinetics of fluorination of metallic Mo with
RUSSIAN JOURNAL OF APPLIED CHEMISTRY Vol. 77 No. 12 2004