International
Journal &Mass
Spectrometry
LASER
INDUCED
F. P, NOVAK,
MASS
SPECTROtlETRY:
K. BALASANFIUGAH,
D. MATTERN
and
Department
of Chemistry,
53 (1983) 135-149
and Ion Physics,
Elsevier Science Publishers B.V., Amsterdam
-
135
in The Netherlands
Printed
ION FORMATION
PROCESSES
K. VISWANADHAH,
AND
RECENT
DEVELOPMENTS*
Z. A. WILK,
C. D. PARKER,
D. M. HERCULES University
of Pittsburgh,
Pittsburgh,
PA
15260 (U.S.A.1
ABSTRACT A summary of the ion formation processes in laser mass spectrometry presented. Particular emphasis is placed on the process of solid state Recent results on the direct analysis of materials chemical ionization. LMS are also presented.
is
using
INTRODUCTION During prolific
the
growth.
ionization" field
last
This
solid
desorption
state
spectrometry labile
(LWS).
spectrometry
is in a large
part
due to development
Each
of samples
techniques
(PD),
have
permitted
it is suited,
of molecular
ones
being
(FAB),
requirements
laser mass
of thermally
by conventional for sample
solution,
and fragment
spectrometry
and
analysis
or its ability
weight
"soft
ion mass
to analysis
to be a universal
of the
prominent
bombardment
has its own
has proved
has experienced
secondary
atom
not amenable
samples,
to which
of the more
desorption of fast
technique
both characteristic
some
techniques,
These
and no one technique types
mass
technique
or nonvolatile
spectrometry.
decades
(FD), plasma
the related
(SIMS),
several
mass
preparation
either
to provide
in the ions that
ions characteristic
are
of
structure. Although at least energy
a decade
transfer,
Similarities be some energy may
these
molecular
spectra
steps
transfer
differ
or more,
from
among
related
to the nature
the similarities
*Dedicated
OOZO-7381/83/$03.00
ionization
the various
and
and
involved
Although
energy
chemical
of the there
the nature
levels,
This
and the differences
may
of the
to the sample into
which
reactions,
for
are known.
that
packets)
of this energy
its environment.
the techniques
the same
or another
suggest
(or photon
phonon)
form
of the mechanisms processes
the dissipation
(exciton,
in some
techniques
particles
ionization,
among
to Professor
understanding
and
of the sample
employing
available
in the mechanisms.
the techniques,
or macromolecular
laboratories
from
involved
in volatilization,
been
no clear
the impinginq
results both
have
volatilization,
among
common
techniques
in turn
is most could
likely
explain
among
technique.
R.D. MacFarlane
on the occasion
0 1983 Elsevier Science Publishers
B .V.
of his 50th birthday.
136 The tried
use of a laser
in the early
as an ionization
1960's.
The&instruments
and metals,
and for a variety
is referred
to a recent
mass LMS
spectrometry. for
Heraeus)
commercial
of inorganic was
soon
species
in our
determining
Eleuzelaar
(2) among
species.
spectrometer
mass
although
Later
very
used
practical.
others
The reader of laser
reported
that year,
developed
s,ystems, the
on the
use of
the development
of
by Leybold-
for microprobe
utility
were
on inorganics
development
(3) (the LAMEIA-500R
originally
in bTologica1
not
primarily
historical
laser
laboratory
the types
mechanisms
the
of sample
influence
that
formation
paper
to the area
concerned
to which
give
of the
we will
processes
been
rise
preparation
an understanding
In this
has
of samples
fragmentation
of LMS
were
the
experiments
analysis
for organic.analysis
realized.
Work
gaining
(1) for
is not new;
were
of organic
reported;
was
of reasons
review
In 1978,
the analysis
the first
source
the
of direct
analysis.
spectra,
of spectra
of our
we will
aspects
of LMS.:
is suited,
of a laser
a summary
in addition
technique
types
interaction
in LHS;
several
to the observed
on the
provide
with
observed,
with
a solid
observations
present
evaluating
determining and sample.
on ion
several
new
applications
EXPERIMENTAL LMS ments.
spectra These
summary,
were
instruments
a Nd:YAG
Q-switched
(ca.
laser
15 ns)
W./cm2).
The
TOF mass
spectrometer
energy and
stored
This
ions
spreads
500 and
laser
laser
is brought normal
and
can
were
at a 45"
in
the
instrument;
with
signal The
at which 1.
~3 urn). from
In this
translation
from
laser
In the
case
while must
either
the ions
thus
stage
Elsewhere, being
are
be thin
kinetic
between
and
the
spectra
the the
any
solid
of the sample
chamber
(70 x 50 x 50 mn).
section were
from
for
are again
essentially
can make
the the
extracted
enough
ions
SEM
on the sample.
in the LAMMA-1000,
analysis
similar.
into the for
of the LAMMA-500,
is the size
to in the direct
%106-10'
by a 17 stage
impinges
In
and
accelerated
p'rimary difference
the
the front
sample
density
is detected
instru-
(4,5).
nm)
,to compensate
configuration
restriction
the LAHIIA-1000.
and
In contrast,
the only
referred
the results
The
Samples
angle
(power
focused,
of the sample,
to the front.
the spectra
sample
elsewhere
(h = 265
an ion reflector
in Figure
(generally
be analyzed;
obtained
back
the
recorder_ angle
to the surface.
the displacement All
is the
in detail
quadrupled
extracted,
formed.
transient
on the
normal
to penetrate
sample
ions
described
onto
employs
schematically
laser
extracted
are
which
in the
is focused
the front,
been
on the LAJltlA-500 or LAFtlA-1000
is frequency
is focused
versions
is shown
either
have that
generated
in a fast
1000
obtained
of the paper
obtained
on either
137
ion
optlom
&f ‘F
Ion optloo
Fig.
1.
Schematic representation impingement path
TLC-LrlS spectra of the dyes solvent
The
All
samples
of laser mechanism and
on this
situation
emission
and
to some
topic
independent;
the
energy.
vs.
(Whatman)
by standard
as received
TLC
LAMMA-
laser
Separations
plates.
methods
without
pulse
observed. laser
dealt
(ref.
further
shape The
of the
with
a solid
6, p. 38,
purification.
book
organic
have
however,
is the
by Ready molecules found
appears
in
of systematic
of lasers
understood.
been
important
resulting
A majority
interaction
less well
laser
process
density
the
in a recent
is even
with
understood.
with
of a laser
species
power
of a laser
is not well have
can be found
of molecular
of spectra
photon
ionization
summary
extent
HP-K
performed
used
for the interaction
the type
were
from
LAMNA-500
ionization
investigations A good
were
of the interaction
volatilization metals.
obtained
(Chem Service)
7).
Mechanism
were
contrasting
(7).
with
The
resulting
in
The duration
to influence
the
to be wavelength
parameter,
not
the single
138 There observed
are
undoubtedly
spectra.
and define
One
several
processes
several
can use
regions
the very
that
occurring
simplistic
are important
that
model
to the
give
rise
depicted
laser
to the
in Figure
2
interaction
phenomenon.
Lorw
beom
Region of “gas-phase’ moctionr I4 1 Surface ionization I3 1
-
ionization Fig.
2.
Regions
Region sample. of ca.
1 is the area
characterized of atomic a plasma thermal can some
solid
of which The
last
particles
into
could
occur.
since
this
peak
the The
which
sort
even
laser
with
Effective This
is
region
the
temperatures a region
of the formation
to the extent
this
ions
is depicted
vacuum_ collision
observed
has
interaction
been
can
be classified
as
This
area
reactions.
must
where
occur
cross-sections
in the LOIS spectra.
are
collisions
is also
where
region can occur, a majority
formed.
formed
is the region
however,
This
phase.
where
This
of high
to as the selvedge,
mobile
are presumably
as a cloud
is a region
referred
yet
is a likely
in chemical
reactions
laser
of condensed
phase
significant
region
of the
region.
on a LTE model.
densities,
of direct
and gas
can result
is where
symmetries
power
region,
as some
of the molecularly
interaction
sense.
This
state
based
interaction
in this
fragmentation,
to the region
upon
occurs
proposed
At high
true
gradient.
be looked
between
been
species.
Adjacent
of the direct
by extensive
in the
to laser/sample
undoubtedly
have
ianitotion
by loser 4 I 1
of importance
Ionization 7000°K
Direct
(2)
from
the emission
ion-mol
reasonably favorable;
ecu1 ar
close also
of reactions
to the
surface,
to retain
the
139 Given
the
difference
This
regions. direct
result
to have result
above
one might
model,
in the time
domain
is shown
qualitatively
of the intepaction
essentially
the same
of secondary
expect
that
of the formation in Figure
of the
time
as the
from
Fig.
3.
Time
or from
ion-molecule
broadened expected These
dependence
to some
extent.
have
emission
taken
Neutrals
are emitted
of the
laser
Ionization can
the gain
been
several
gradient
*
on the other pulse
by Cdtter
ionization
hundred
are a
of high thermal
to later
the laser
demonstrated
of by post
for
emission
be expected
that
in LriS
be offset
time after
times
hand, would
be
had terminated,
(8,9) and
by an electron
microseconds
and be
after
the neutral
beam
(8).
the termination
pulse.
4 summarizes
be classified
the types as being
or loss of an electron,
ionization solid
indeed
advantage
should
Neutral
for some
emission
as a
processes
Figure
Ions
reactions,
to continue
features
of particle
Species
laser.
Time
be a
the various
the solid would
the region
I
would
Ions that are formed
3.
laser with
profile
either
processes,
there
of ions from
state
of salts,
formed
from
the gain
ion-attachment
"CI" reactions
of ionization
observed
one of the following
or loss of a proton,
reactions,
or ion-molecule
processes
or what
reactions.
we shall
in
LW.
processes: the direct refer
to as
140
-K+n’
M+B M+ntl-
mf++B-
n+c+ -rc* H + A- -
Fig.
Summary
4.
Direct production found
in conventional process
is observed electron
rarely
result
The
that
loss
cation.
however, of molecular
aromatic
positive
this
which
are
electron
is not
the
ion
a very
by this
process
The
situation
for
anion
is rarely
seen.
known
to form
affinities,
stable
molecular
anions
observed_
most
common
species
observed
in LMS are due
Acids
tend
to loose
a proton
while
expected
from
chemical
properties.
properties,
their
that
quasimolecular also
and
typical
cations
molecular
proton.
Note
is the
hydrocarbons.
hydrocarbons, have
of an electron
This
production
in the odd electron
aromatic and
in the
spectrometry;
for polynuclear
polynuclear
in LMS
molecular
EI mass
resulting
in solution
The
would
in LMS.
mainly
capture
for
anions are
photoionization
processes
of the odd electron
prominent
Even
of ionization
M’
the
is they
anion
form
(M-H)-,
fragmentation
both
Many
to the
tend
species
the quasimolecular
as shown which
bases
for
could
a substituted
be useful
gain
or loss
to gain
one,
exhibit
amphoteric
cation
(M+H)+
chromone
of a
as and
the
in Figure
in identification
and
5.
141 structural basic
The charge
in solution
third
process,
separation.
the cation
C+ and
in the negative clusters
The
result
in many
that
exhibit
one would
properties
ionization
is that
instances
do not exhibit these
of salts,
in the positive
clusters observe
appreciable on laser
is brought ion mode
corresponding the anion
acidic
about
by
one observes
to C+(C+A-),,
A- and
or
irradiation.
and
the corresponding
A-(C+A-).
Another
important
situation,
organic
moiety.
are otherwise
5.
may
the direct
ion mode
In this
Fig.
Compounds
elucidation.
behavior
process
inorganic This
that occurs ions
can be utilized
obtainable.
The
in LMS
by some mechanism
sample
Positive and negative ion LMS 4H-1-benzopyran-3-yl)propanoate
in many
"attach"
situations
can be mixed
spectra
is cation
with
or anion
attachment.
themselves
where
to an
no LOIS spectra
an inorganic
salt,
of 2-(Acetylamino)-3-(4-oxo-
in
142 expectation most
of
important
forming in
forming
have
most
useful .
been
studied, The the
of
cul ar , are
parti
the
attachment drawback
species
does
Ion-molecular lastest
addition
process
is
in
or to
reacts
with
by
particular
limited
number
However, are
the
there
currently
Sol id
As part
would
systems,
is
great
occur
negative
ion
derivatives
In
C3N-,
addition
(M+15)-
for
demonstrates The
this
LMS.
a species M,
of
when when
samples,
the
trace cause
in
type
of
are
The
solid
A+ is
forming
a new
We have
this
the
ionization formation
organic show
detail
ion
the
reaction,
as
for
a
and
next
CI which
MB+,
this
in
the state
generated
observed
of
processes of
are
a series
that
ectron
the of
in
LFlS,
odd-electron
molecules
odd-e1
behavior
the
was
these
section.
more
systems
we were
molecular contain
molecular
anions
electron
A class
anions.
ni trobenzene
derivatives;
dinitrobenzenes
species,
negative
molecular
observed,
o-dinitrobenzene,
and
the
base
an
additional
at
corresponding
the
ion
be
represented
were
LMS spectra
peak
substitution in
anion
nor
the
following
peak
generally intense
the
thus,
of the
related
quasimolecular species:
m/z to
reaction
substitution by
of
of = 183
an aromatic
(M+O-H)-.
is
and
most
initiated hydrogen
CN-,
was
to likely by
CNO-, to
observed
(M-NO}-. at
1 ,3,5-trinitro-
ni trobenzene
corresponds is
(M+l5)that
o-di
anion
corresponding peak
1,8-dinitronaphthalene, ion
The
results can
formation
reactions
in
be discussed
the
(Il-NO)- , with
and
species
and
studied.
this.
nucleophilic
the
most
ionization”
interest,
if
frequently
What
The
benzene.
the
observed
be misleading in
observed
of
neither
to
be
be disheartening
can
one:
in
EI-MS,
LMS behavior was
observed.
NO2-,
In
of
Surprisingly, were
study
LMS.
typical
species
to
ionization”
our
groups
compounds
only
study,
determining
in
withdrawing
potential
chloride
seems widely
ion
(10).
impurity
involved.
as wi 11
the
sodium
unintentionally.
conventional of
the
currently can
it
an
of
of sodium
not
more
that It
“chemical
species
of
of in
the
are
observed is
processes
reaction
“chemical
interested
species
one
halides,
are
also
is
instance, attachment
they
however,
which
solid-state
the
under
state
form;
sodium
to
defined
are
For the
cationization
predictable.
ionization
analogous
salts, sodium
reactions
not
a cationized
to
alkali
phenomenon
not
instance of
used
this
is
due
the
however,
reactions of
species
formation
Though
cationization
major
for
species. is
widely
(10);
Although
ion-attached
turn
!1+23.
most
utilized
ion-attached
the
attached reactions
mass
anion
impurities,
ion
cationization
a species
that
an
shown
in
Figure
6
(M+15)-. the the
result laser.
by oxygen;
the
of The
a process
resulting
143
Fig.
Negative
6.
ion
In contrast, benzene nitro
show
LMS spectrum
the negative
a negligible
groups
1,3,5_trinitrobenzenene high
at and
spectra
of meta
and para
dinitro-
some interaction
(M+O-H)-.
Thus,
ortho
substitution
although
(TNB)
nitrobenzene
is not
1,8_dinitronaphthalene
of the
essential
show
since
{Vl+l5)- with
intensity. In order
aromatics
was
formation
of
other also
o-di
ion LMS
peak
is important,
of
to study-this studied. ortho
facilitated
generally between
have only
aromatic positive
series
to make of PAH's
of dinitro
of these
groups
side
reactions,
carboxylic
is necessary
studies,
adjacent
and
in order
for
The
to each
The
is not mandatory.
for the
hydrocarbons electron
infrequently
aromatics
work
series
process
instance
is the
phenolic
to elucidate
the
reaction.
and
the above
The
donors
(RlPD)
use of these
(PAHIS)
affinities;
in LKS.
and electron
methyl-p-phenylelediamine attempt
more
this
nitro
of competing anion
a larger
the results
by two
however,
absence
Considerably of this
Polynuclear observed
or peri);
by.the
effect
7 summarizes
of the quasimolecular
compounds. mechanism
Figure
(11+0-H)- is facilitated
(either
formation
positional
electron
however,
formation
and
and TNB
reactions,
having
acceptors,
LMS spectra and
or more
molecular
rings
anions
of charge-transfer like
respectively,
donor
three
N,N,N',N'-tetra-
is well
were
acceptor
are
complexes
known.
obtained species.
with
In a
an
144
Fig.
Summary of study compounds showed
7.
The
presence
exception
of
corresponding
to the
results; hydrocarbon) results
were Since
must
of
samples
contain
no effect
that
had
benzyl
The
presence
of
a peak
as many
observed the
TMPD had
(M-H)-.
presence just
of [M+O-HIformation in nitrobenzenes. the nucleophilic substitution reaction
reactant an oxygen
for
of all
species atom,
on
the
aromatic
i c hydrogens
at
of
(!1+15)-
TNB however, (where
nitro-substituted of
the in
we attempted
compounds, showed showed
had
Boxed LMS analysis
with
surprising to
shown.
the These
studied.
nucleophilic to
use
substitution other
oxygen
the
peaks
tl corresponds
samples
PAH’s
the
; these
on
reaction containing
aromatic
145 species, All
Na20,
e.g.
of the above
observed
gave
the same
of the potential
the relative
amounts
observed.
combination
The
and
nitrocellulose
result;
reactants
of these
formation
ion LMS
O-',
species
polymer,
the formation
The negative
for all reagents.
formation was
NaN02
NaN03,
02-'
and the
of the species
as CI reagents.
of a peak
spectra
(M+15)-
of the reagents
and N02-; intensity
at
show
no correlation of the
was
with
(M+O-H)-
(M-+0-H)- can be the result
ion of any
of the following:
ArH + O-'
+
ArO-+H-
(1)
ArH+02-'+
ArO-+OH.
(2)
ArH + NO2- +
ArO-
(3)
+ HNO
It is difficult of solution brought
about
variety extend
existing
of samples
of selective
We have
important
quasimolecular formation
reactions
What
can be produced
can-be
of completing
analyzed
(M+H)'
or simply
from
a detailed The
and
of the quasimolecular
"plasma"
states.
are analogs
of reactions is hoped
that will
by LMS,
in the LMS characterization
compounds.
ions,
reactions
is that
a
not only
but also
to add
the
of amino
acids.
We
transfer
interested
in the process
of these
in excited
that
these
or are the result
ionization.
proton been
to say whether
thermally,
of chemical,ionization
Intermolecular
the
point
induced
by species
the range
dimension
are
at this
chemistry
amino
(M-H)-. cation
study
acids
of the fragmentation
show
high yields
The question results
intermolecular
from
proton
arises
as to whether
a protonation
transfer
Datterns
of the reaction
among
amino
in
acid
molecules.
In
order
mechanism, exchanged valine-d3 appeared
to distinguish
a study
was
with
deuterium.
were
obtained.
that
functionality
positive
In the case
the proton and not
plasma
out where
The
at m/z = 122 while
indicates
between
carried
from
and the
hydrogens
ion LMS spectra of valine-d3
for valine
responsible
protonation
the labile
it appeared chain,
of both
valine
the quasimolecular at m/z
for protonation
the aliphatic
transfer
on valine
must
= 118. come
substantiating
were and
catio n
This from
the am ine
the transfer
mechanism. One
could
labile,
and
density
until
conditions
still
are the
only
for valine-d3,
both
argue only
that
ones
the
ionized.
H+ and D+ were
the This
quasimolecul shows
hydrogens
that
ar
the amino
We therefore
observed ion
from
gas-phase
increased
in the spectrum.
corresponding protonation
group
to
the Even
(bI+D)+
was
are more laser under
power these
observed
is not responsible
for
146 the quasimolecular whether
this
multimer Direct
ion
(M+H)"
in amino
is due tb a "solid
over
the
acids.
state"
It is not
reaction
clear
however,
or to the dissociation
of a
surface.
analysis
The
LAMMA-1000
potential
for
summarize
some
not
configured
of solids.
in our
analysis.
practical,
similarly
analysis
experiments
LMS to direct though
and other
the direct
laboratory
dealing
A few of the examples demonstrate
LMS
instruments
have
In this last section
the variety
have
with
great
we
the application
ootential
of samples
of
use, while
from
which
LMS
others, spectra
can be obtained. The shown
coupling
itself
of separation
to be very
techniques
useful.
The
coupling
HPTLC
with
LMS.
We will
analysis
of samples
from
an HPTLC
We have be analyzed
been
groups
triphenylmethane method
Dyes
plate
characterized rosaniline
hydrochloride,
separated
by LMS.
The
obtained
from
on a HPTLC spectra
the neat
lower
mass
shown
in Figure
end
These determine determine The analysis black
due
samples,
to silica
of
on the direct
violet, The
the One
layer
an assignment
This
spot.
of seven green,
would
be
plate was
TLC-LMS
their blue
and
was
were
ethyl
then
B, violet)
analyzed
analogous
a contribution
spectra
location
previously
Victoria
green,
TLC
there
since
dyes
the plates
that The
are
obtained.
is by thin
to confirm
cannot
of new dyes.
malachite
from
except
dyes
dyes
of ionic
of dyes
of TLC-LMS
air dried
species.
class
are readily
the TLC
study
Most
to those to the
of two dyes
are
8.
initial
results
are
of samples
detection
limits.
encouraging
results
possibilities.
pen mark
from
brilliant
directly
the types
Reproducible marker,
obtained
these
A mixture
violet,
gentian
results
to the presence
such
structures
noted.
plate.
has already
the possibility
by LMS.
to be able
spectrum
for an initial
(methyl
due
however,
identifying
in authenticating
by LMS
of dyes
One
spectra
be advantageous
is readily
initial
spectrometry
and
spectrometry
affords
plate.
LHS
a mass
are convenient
our
volatility.
Their
It would
helpful
on the TLC
was
limit
on Rf by obtaining
especially
mass
of separating
chromatography. based
that dyes.
present
in the analysis
by conventional
functional common
interested
to mass
LAMMA-1000
on paper.
spectra
were
and of a variety
very
prompted
Figure The
promising
for which
spectrum
of colors.
and further technique
further
9 shows
obtained
the
from
investigation
the positive is that
technique
is underway
of pen may
and
of other
ion LMS
of gentian
a variety
This
work
is suitable,
spectra
to
direct of a
violet. types,
thus
roller
have
and
forensic
to
147
m
I)
l VI
GENTIAN
n-
VIOLET
1
’ I
mL
.
Fig. 8.
Positive
ion TLC-LMS
of brilliant
green
and gentian
violet
3 I
Fig.
9.
Positive
ion LMS spectrum
of pen
mark
directly
from paper
148 application;
work
conventional
analytical
One Figure
further
is currently example
the spectrum
in lob is that
to caffeine,
detectable
amount)
does
not have much
one of a variety
Fig.
of the direct
10a is the negative
correspond
10.
to compare
caffeine potential
analysis
ion CMS spectrum
this method
potential
of a brand
of the decaffeinated
and that
of samples
Negative coffee
underway
with
methods.
as expected,
as an analytical from
which
ion LMS spectra
coffee
crystal.
there
in the decaffeinated
crystal.
of a) regular
that
less
it does
while the spectra
this example rcpiesent
directly.
and b) decaffinated
ACKNOWLEDGEMENTS This National
work
was
Science
supported
Foundation
by the Office (Grant
of Naval
Research
and-by
the
No. CHE-8108495).
REFERENCES 1. 2. 3.
R. J. Conzemius and J. 34 (1980) 179. W. A. Posthumus, P. G. Noever de Brauw, Anal. R. L. Kaufman, et al.,
M. Capellen,
Int. J. Mass
Spectrom.
10.
(yet a
Though
can be obtained
coffee
in Figure
crystal
Note
is much
technique,
spectra
Ss shown
Ion
Phys.,
Kistemaker, H. L. C. Meuzelaar and M. C. Ten Chem., 50 (1978) 985. Hicroscopica Acta, Vol. 73, 1972, p. 1.
149 4. 5. 6. 7. 8. 9. 10.
E. Denoyer, R. Van Grieken, F. Adams and D. F. S. Natusch. Anal. Chem., Vol. 54, No. 1, 1982, p. 26-41A. H. J. Heinen, S. Meier, H. Vogt, R. Wechsung, Int. J. Mass Spectrom. Ion Phys., 47 (1983), p. 19-22. K. Venkataraman (Ed.), The Analytical Chemistry of Synthetic Dyes, J. Wiley, New York, 1977. John F. Ready, Effects of High Power Laser Radiation, Academic Press, New York, 1971. R. J. Cotter, Anal. Chem., Vol. 52, No. 11, 1980, 1767-1770. R. 8. Van Breemen, M, Snow and R. J. Cotter, Knt. J. Mass Spectrom. Ion- Phys,, 49 (1983) p. 35-50. K. Balasanmugam, T. A. Dang, R. J. Day and D. f1. Hercules, Anal. Chem., Vol. 53, No, 14, 1981, p. 2296-2298,