That mercury atoms excited by absorption of the line 2537Å are able to activate various kinds of atoms by collisions of the second kind has been shown in several different ways. Using pressure measurements to follow the reaction, Cario and Franck (1) showed that hydrogen, in the presence of excited mercury vapor, can be activated and made to reduce copper oxide or tungsten oxide, while Dickinson (2) repeated the experiment using gaseous oxygen instead of solid oxide. Employing spectroscopic methods of detection, Cario (3) activated thallium vapor by collisions with excited mercury atoms and observed the radiation of the green thallium line 5351 Å and indeed all the thallium lines which would theoretically be expected

Mitchell, Allan C. G.

English

Caltech Authors - Main

CHEMISTRY: A. C. G. MITCHELL
THE ACTIVATION OF HYDROGEN BY EXCITED MERCURY
ATOMS
By ALLAN C. G. MITCHELL
GATES CHEMICAL LABORATORY, CALIFORNIA INSTITUTE OF TECHNOLOGY
Communicated June 9, 1925
Introduction.-That mercury atoms excited by absorption of the line
2537A are able to activate various kinds of atoms by collisions of the
second kind has been shown in several different ways. Using 'pressure
measurements to follow the reaction, Cario and Franck' showed that
hydrogen, in the presence of excited mercury vapor, can be activated and
made to reduce copper oxide or tungsten oxide, while Dickinson2 repeated
the experiment using gaseous oxygen instead of solid oxide. Employing
spectroscopic methods of detection, Cario3 activated thallium vapor by
collisions with excited mercury atoms and observed the radiation of the
green thallium line 5351k and indeed all the thallium lines which would
theoretically be expected.
Donat,4 and later Stuart,5 investigated the decrease of resonance-radia-
tion of mercury in the 2P2 state on the addition of certain gases, including
hydrogen, oxygen and argon; and found that the resonance-radiation of
mercury was greatly decreased by the addition of quantities of hydrogen
up to 5 mm., somewhat less by the addition of the same quantities of
oxygen, and very slightly by the addition of argon. This decrease in the
case of hydrogen is due to the fact that the mercury in the 2p2 state acti-
vates the hydrogen and falls back to its normal (1S) state without emitting
radiation. Donat, following up the work of Cario on the emission of the
green thallium line showed that on the addition of argon or nitrogen the
intensity of the thallium line was greatly increased, which result has been
confirmed in this Institute by Loria.6
Donat explains this increase in the intensity of the thallium line in the
following manner. By collisions with argon, the mercury atoms in the
2P2 state are forced into the 2p3 state, which has a slightly lower amount
of energy. The mercury atoms in this lower energy state are forbidden
by the quantum theory to lose energy by radiation, and furthermore in
accordance with the hypothesis of Donat can endure many collisions with
argon without losing energy. Hence they have a very long life, and the
only way they can give up their energy is by collisions with thallium atoms.
This they do, activating the thallium atoms thus causing them to emit
the green line, 5351!. This would also account for the slight decrease in
the resonance-radiation of mercury on addition of argon, as observed by
Stuart and by Donat.
The purpose of this research was to extend Dickinson's experiments, in
458 PROC. N. A. -S.
VL11195 CHEMISTRY: A. C. G. MITCHELL
order to determine the effect of varying the pressures of hydrogen and
oxygen and of adding argon on the rate of the reaction between the hydro-
gen and oxygen.
Experimental Procedure.-Light from a quartz-mercury arc lamp was
passed through a quartz lens into a reaction tube of quartz contained in a
cylindrical electrically heated furnace. The furnace -was kept at about
450 as in the experiments of Dickinson. The quartz reaction tube, 2 cm.
in diameter and 16 cm. long, had a clear quartz window fused to one end
and a small quartz tube joined to the other. A sealing-wax joint connected
the latter to a glass trap which was kept immersed in liquid air. A side
bulb containing mercury which could be drawn out permitted the gas to
be expanded and recompressed, thus facilitating the removal of condensible
miaterial by the use of liquid air. By means of stopcocks the gas space
could be put in communication either with a mercury diffusion pump or a
gas mixing chamber containing the desired reaction miixture. Hydrogen
and oxygen, generated electrolytically from a barium hydroxide solution
could be introduced by means of stopcocks. Argon could also be let into
the gas mixing chamber at suitable pressures. In order to keep the line
2537A fronm being reversed, the anode of the mercury arc lamp was cooled
by a blast of air, kept constant with the aid of a Pitot tube. The rate of
reaction was measured by means of the decrease in pressure as read on a
MacLeod gauge.
The experimental procedure was as follows. After pumping out the
whole system, a known mixture of hydrogen and oxygen was admitted and
the pressure read on the MacLeod gauge, so that the partial pressures of
oxygen and hydrogen could be calculated.. The reaction tube was now
illuminated with the light from the mercury arc, the intensity being kept
constant with the help of an ammeter, voltmeter, and slide-wire resistance.
After a definite time of illumination, usually ten minutes, the condensible
matter was removed and the pressure read. This process was repeated six
times, giving a total time of illumination of about an hour. About 2 cc.
of mercury were placed in the reaction tube at the beginning of the series
of experiments and were replenished once in the latter part of the series.
In the cases where argon was added the procedure was modified as
follows. An approximately equal mixture of hydrogen and oxygen was
admitted to the mixing chamber and thence to the reaction tube, and the
pressure read. The gas-mixing chamber was then shut off and the reaction-
tube system pumped out. In the meantime a definite amount of argon
was let into the gas-mixing chamber. The mixture of hydrogen, oxygen,
and argon was then admitted to the reaction tube and allowed to come to
equilibrium. The pressure was again read. The ratio of the volume of
the mixing chamber to that of the reaction tube having been determined,
the ratio of argon to hydrogen and oxygen could now be calculated.
459VOL. 1 1, 1925
CHEMISTRY: A. C. G. MITCHELL
The Experimental Results.-The experiments of Dickinson were re-
peated with similar results, and in addition experiments were carried out
to show the dependence of the rate of reaction on the pressures of hydrogen
and oxygen.
When the concentration of oxygen was kept constant at about 0.036
to 0.04 mm., the rate was found to increase as the pressure of hydrogen
was increased, but seemed to reach a saturation value as in the experiment
with Cario and Franck. It was, however, difficult to get reproducible
results with pressures of hydrogen much above the usual of about 0.04 mm.
The important fact, nevertheless, was demonstrated that at pressures of
hydrogen as high as 0.6 to 0.7 mm., there was a large rate of reaction as
great as 11-12 X 10-4 mm./min. This result will be referred to again
in connection with our discussion of the effect of large additions of argon.
Experiments were also made keeping the pressure of hydrogen constant
and varving the amount of oxygen. When no oxygen was present the rate
was found to be zero. On addition of small quantities of oxygen the rate
increased very rapidly (almost linearly) until it reached a maximum at
0.01 mm. of oxygen, then decreased until a small but measurable rate was
reached. Table 1 shows the rate of reaction as a function of the pressure
of oxygen, the pressure of hydrogen being kept constant at 0.041 mm.
TABLE 1
EFFECT OF OXYGEN ON THE RATE OF REACTION
PRESSURE OF NYDROGEN CONSTANT AT 0.041 MM.
OXYGEN PRESSURE RATE OXYGEN PRESSURE RATS
IN MM. MM./MIN. IN MM. MM./MIN.
0.002 0.7 X 10-4 0.081 3.0 X 10-4
0.003 0.7 0.117 2.0
0.004 2.4 0.120 2.0
0.004 2.2 0.194 1.8
0.009 6.7 0.305 1.7
0.01 5.5 0.343 1.2
0.027 3.7 0.345 1.4
0.041 3.2 0.351 1.5
0.080 2.5 0.355 1.5
The addition of relatively large quantities of argon was found to stop
the reaction completely. Two sets of experiments were carried out with
two different samples of argon. In the first set argon made by the General
Electric Company was taken from a tank under pressure. It was thought
to be pure, but no guarantee was given. In the second set compressed
argon, guaranteed by the General Electric Company to be 99.8% pure,
was used. The results in the two cases were found to be the same. The
results of a typical experiment are shown in the figure. The pressure of
hydrogen and oxygen are plotted against the time of illumination. Curve
I gives the rate when the ratio of argon to hydrogen is about twelve to one.
Curve II gives the rate when there is no argon present.
460 PROC. N. A. S.
VoL. 1,1925CHEMISTRY: A. C. G. MITCHELL
Further expenrments were made in which the pressure of hydrogen and
oxygen were kept constant (within five per cent) and the pressure of argon
0
QoSe~~ 0oo 3 o 50 o i0
Tlme /Alt7ueo.
was varied. The rate of reaction was found to decrease as the pressure
of argon increased. Table 2 shows this effect for both sets of experiments.
TABLE 2
EFFECT OF ADDITION OF ARGON ON THE RATE oF REACTION
PRNSSURB Or HYDROGNN CONSTANT AT 0.036 MM.; PRNSSURB OP OXYGrN CONSTANT AT 0.036 mm.
FIRST GROUP SUCOND GROUP
PRBSSUR OP ARGON RATE PRNSSURZ OF ARGON RATS
IN MM. MM./MIN. IN MM. MM./MIN.
0.0 2.2 X 10-4 0.00 3.2 X 10-4
0.067 1.67 0.190 2.0
0.180 1.50 0.358 1.3
0.216 1.41 0.372 1.2
0.219 1.25 0.379 1.5
0.299 0.67 0.380 1.4
0.431 0.00 0.458 0.7
0.455 0.00 0.458 1.0
0.478 0.8
0.571 0.0
0.575 0.0
Discussion of the Results.-The dependence of the rate of reaction on
the pressure of oxygen may be explained as follows. Below the optimum
pressure of oxygen (0.01 mm.) many of the hydrogen molecules which are
activated by collisions with mercury atoms in the 2p2 state lose their activa-
tion before they have made contact with an oxygen molecule. On the other
hand, when the oxygen is above the optimum pressure many of the excited
mercury atoms are killed off by collision with oxygen molecules, as is also
shown by the work of Stuart, thus leaving fewer excited mercury atoms to
activate the hydrogen. Collisions between excited mercury atoms and
oxygen molecules seem not to activate the latter sufficiently to allow them
to form water by collisions with hydrogen molecules.
VOL. 1 l, 1925 461
CHEMISTRY: A. C. G. MITCHELL.
The experiments showing the decrease of rate of formation of water on
the addition of argon seem not to be in agreement with what might have
been expected on the basis of the results reported by Donat; nor are they
to be fully explained by the experiments of Stuart, which show that the ad-
dition of argon cuts down the resonance radiation of mercury but slightly.
That no increase in the rate of reaction was observed on addition of
argon due to collisions with mercury atoms which have been put into the
2p3 state by collisions with argon may be explained by one of the following
hypotheses:
(a) That mercury atoms in the 2p3 state, while able to give up their
energy to thallium, are not able to interact with hydrogen molecules.
(b) That mercury atoms in the 2p8 state, while able to endure many
collisions with argon atoms without losing energy, are immediately de-
activated by collisions with oxygen atoms.
That such a large decrease in the rate of formation of water was ob-
served on. addition of atgon might be explained by the assumption that
hydrogen is dissociated by excited mercury atoms and that addition of
argon furnishes a means whereby two hydrogen atoms may combine
through a triple collision with an argon atom, thereby decreasing the rate
of reaction. An attempt to test this hypothesis was made by measuring
the rate vhen a large amount of- hydrogen was present, since the excess
of hvdrogen should also furnish molecules for the triple collisions. The
rate, nevertheless, did not decrease as might have been expected, as will
be seen from the large rate which was observed when the pressure was 0.6
to 0.7 mnu. This is not conclusive proof, however, that hydrogen atoms
are not combining through triple collision with hydrogen molecules, since
the large rate observed might be due to the increased chance of forming
a greater amount of activated hydrogen which masks the effect of triple
collisions.
An alternative hypothesis is that activated hydrogen is not atomic,
as assumed by Cario and Franck, but is molecular hydrogen in a higher
quantum state, having for example one or more quanta of energy of oscil-
lation, with a definite life-time and capable of being deactivated by col-
lisions with argon. This assumption as to the nature of activated hydro-
gen affords an even shnpler explanation of the Dickinson experiment than
does the hypothesis of monatomic hydrogen, and is in accord with the
speculations of Compton and Turner7 concerning equilibrium in a region
containing hydrogen and mercury. Since, however, it has been shown by
Cario and Franck that activated hydrogen can diffuse through high pres-
sure hydrogen gas and still, remain activated, the above assumption would
necessitate the further hypothesis that this higher quantum state of hydro-
gen is metastable towards collisions with hydrogen molecules.
The above hypotheses do not exhaust the possibilities of explanation,
462 PROC. N. A. S.
VoL. 11, 1925 CHENMISTRY: S. A. WAKSMAN 463r
and further work will be necessary to elucidate the exact mechanism of all
the processes occurring.
The writer wishes to express his thanks to Prof. R. C. Tolman for his
advice and interest in this work, and to Dr. R. M. Badger and Dr. 0.
Oldenberg for many helpful suggestions; also to the Carnegie Institution
of Washington for financial assistance received from a grant made to Prof.
A. A. Noyes.
1 G. Cario and J. Franck, Zt. Physik., 11, 161 (1922).
2 Dickinson, Proc. Nat. Acad. Sci., 10, 409 (1924).
3 Cario, Zt. Physik., 10, 185 (1922).
4 K. Donat, Zt. Physik., 29, 345 (1924).
6 Herbert Stuart, Zt. f. Physik., 32, 262 (1925).
6 Loria, Phys. Rev., 25, 212 (1925).
7 Compton and Turner, Phil. Mag., 48,360 (1924).
WHAT IS HUMUS?'
By SZLMAN A. WAKSMAN
Nzw JZRSEY AGRICULTURAL EXPZRIM1NT STATIoNs, DPArMT"NT o0 Son CxHiwsTY-
AND BACTERIOLOGY
Communicated July 7, 1925
Several theories have been proposed at various times to explain the
origin of the black-colored organic substances, which go to make up the
bulk of the soil organic matter and which are commonly known as "humus."
None of these theories, however, sufficiently explained processes involved
in the formation of the complex mass of soil organic matter, to be uni-
versally accepted. The very nature of the chemical constituents of this
"humus" is little understood, although an extensive literature concerning
some of these constituents, namely the "humic acids," is available. A
number of methods have been suggested for determining quantitatively
this soil "humus" and "humic acid," since this was usually considered to
be the available portion of the soil organic matter. However, none of the
methods proved satisfactory; the results obtained for the same soil bv
different methods varied greatly, and we are still in the dark concerning
the nature of the soil organic matter, its formation, and physical and
chemical properties. Schreiner and Shorey, in summing up in 1909 the
survey of the literature on this subject, came to the conclusion that "the
most conspicuous feature is the lack of specific knowledge concerning the
organic matter of the soil." Since then, new theories and new methods
have been proposed, but even at present "the complete lack of knowledge
concerning the nature of soil organic matter, the indefinite limit between


The activation of hydrogen by excited mercury atoms

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The activation of hydrogen by excited mercury atoms

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