Reprinted from
the Journal of the American
Chemical Society, 1990, 112.
Copyright @ 1990
by the American
Chemical Society
and
reprinted
by
permission
of
the copyright
owner.
Quantifying
Acid-Base Properties
of Organic
Functional
Groups at
a
Polyethylene-Water
Interface
by Photoacoustic
Calorimetry
Lijian Zhang, Matthew
A. Shulman,
George M.
Whitesides,
and
Joseph J. Grabowski*
Department
of Chemistry, H art'ard L' nir ersi
t.t'
Camhridge, Ma.rsachusetts 02 I
38
Receired ,4pril 26, 1990
This
paper
describes
the use of
photoacoustic
calorimetry
(PAC)r
to characterize
acid-base
equilibria involving
organic
chromophores
covalently
attached
at the interphase between
surface-functionalized polyethylene
(PE)
film2'3 and
water. We
use
proton
transfer reactions
to define
the
polarity'
and solvating
capability
of the interphase
between
organic surfaces and
water.a
Characterizing
these
physical-organic
properties
of
interphases
is difficult:
light
scattering
at
interfaces
(especially
rctugh
in-
terfaces)
complicates
many
UV-vis absorption
and
fluorescence
methods;
infrared
spectroscopy
cannot
be applied routinely to
systems
involving water;
thermometric
and
conductometric
methods
are insensitive for
solids having
low surface areas. The
measurement
of the
contact angle of
buffered
water
on surfaces
as a function
of
pH-"contact
angle
titration"-yields
valuable
information
about
acid-base equilibria,3
but
depends
on unverified
assumptions.5
(l)
Rothberg,
L. J.;
Simon, J. D.;
Bernstein, M.; Peters, K. S.
J.
Am.
Chem. Soc. 1983, 105,3464-3468.
Braslavsky,
S.
E.; Ellul, R.
M.;
Weiss,
R.
G.; Al-Ekabi,
H.;
Schaffrier, K.
Tetahedron 1983, J9, 1909-1913.
Burkey, T.
J.; Majewski,
M.;
Griller, D.
J.
Am.
Chem. Soc.
1986,
/08,
22t8-222t.
(2)
Whitesides,
G. M.; Ferguson,
G. S. Chemtracts 1988, /, l7l-187.
Whitesides,
G. M.; Laibinis,
P. E,
Langmuir 1990, 6,87-96.
(3)
Holmes-Farley,
S. R.; Bain,
C.
D.; Whitesides,
G. M, Langmuir 1986,
4,921-931.
Wilson,
M.D.;Whitesides,
G. M.,/. Am, Chem. Soc. 1988, 110,
8718-8719.
Holmes-Farley,
S. R.;
Whitesides,
G. M. Langmuir 1987, J,
62-16.
(4)
Bordwell, F.
G. Acc.
Chem. Res. 1988. 21.456-463.
7070
J. Am.
Chem. Soc,,
Vol.
I12.
No. 19. 1990
Communications to the Editor
Table L Experimental
Values
of
pK172
and
pKu
for Organic
Functional
Groups in Aqueous
Solutibn
and at a Polyethylene-Water
I nterfaceo
R
NH{CH:)5NH
Dansyl
-ra
. :-,..,,:
J+g1-_,e'
______f_
a
L
c
q\R=pe
R=HJ
I
R
=
PE-COb
R=H
PKr/z
PK^
RNH(CH2)rNH-dansyl
0.56
+
0.1I
RNH(CH2)rNH-dansyl
1.2
*.
0,2'
RNHC6HT-3-NO2-6-OH
9.3
+
0.1
RNHNHCOC6H4-4-OH
12.4
+
0.2
3 3.52
*
0.03. 2
3 3.57
*
0.09.
2
3
7.00
+
0.10d 2
3 8.29
*
0.30
3
oAqueous
solutions
oi HCI
and NaOH were
used to
vary
the
pH
during
these
acid-base titrations.
The addition
of these
trace amounts
of acid
or base themselves
cause
no change in
the PAC signal
other
than that due
to degree
of
protonation
of the
substrate. The
errors
listed
are
I
standard deviation
of the number
of independent
experi-
ments indicated
by n.
DAll
films were prepared
from
PE-CO-CI
as
described
in rei 8. A fresh
film
was
prepared
for each
measurement.
Any
acid chloride
functionality
that
was
not converted
to the
appro-
priate
amide
is hydrolyzed
during
the synthetic
workup.
.See
refs
8
and 13
for
previous
estimates
of these
values.
dThe
pK"
of R
=
COCH3, as determined
by PAC. is
6.02
+
0.03
(n
=
2\.
We
have
used as substrates
for
this
work
surface-oxidized
polyethylene
films
(p
=
0.92
glmL,l00
pm
thick;
pretreated
to
remove
additives)
to
which
were
covalently
attached
l-(di-
methylamino)naphthalene-5-sulfonyl
(dansyl)
or
phenolic
groups
(Table
I).6
These
functionalized polyethylene
films
were
sus-
pended
in
water
in a standard
UV-vis cuvette
and irradiated with
a low-energy,
unfocused light pulse
from
a nitrogen
laser
(337.1
nm;
ca. l0
pJ/pulse:
2-mm-diameter
spot).7
The
photoacousric
signal
generated
from
each
of the four films
exhibited
an
excellent
signal-to-noise
ratio
(Figure
l).
Control experiments
established
that these PAC
signals were
due to
the
attached
organic func-
tionality
and that each system was
stable
to irradiation:
(i)
Both
unfunction
alized
(PE-H)
and oxidized
(PE-COrH)
polyethylene
films
gave
weak, pH-independent
PAC
signals.
(ii)
The func-
tionalized
polyethylene
films
that
gave
strong,
pH-dependent
signals showed
contact
angle
titration
behavior
consistcnt with
that
reported
earlier,s
(iii)
The intensity
of the
PAC signal from
a functionalized
film
at constant pH was
linearly proportional
to
laser
energy.T'e
(iv)
The PAC
signal remained
invariant
over long
periods
of time at fixed pH,
indicating
that no
solvolytic
chemistrr
occurred.
(v)
Extended
irradiation
had
no
effect on
the
pAC
signal,
implying
that
no
beam damage
occurred.
(vi)
Upon re-
moval
of the films
from
the cuvette,
no PAC
signal was
detected
in
the
aqueous
solution.
The changes
in
the PAC
signal as
a
function
of
the degree
of
protonation
are due
to changes
both in
the
heat release
quantum
yield,/.,,
and
in
the extinction
coefficient
of the
protonated/de-
protonated
substrates.
For
example,
the dansyl
moiety
has
an
extinction
coefficient
of
-4000
M-r cm-r
at 337.1 nm while
the
protonated
dansyl
moiety
has
a value
of
-200
M-l cm-I.10
In
addition,
the fluorescence quantum
yields
of
these two
species
are
quite
different.
The
pH
titration
data
generated
in
these
pAC
experiments were
readily
fit by
a standard pK.
titration
expres-
sion.rr
The
similar
quality
of
the
fit for
the dita
from
the irlms
and
from solution
suggests
that
the PAC
experiment
samples
a
single
population
of functional
groups
in the
interphase.
.
The value
of
pKr12-the
solution
pH
at
which
the surface
ionization
of a functional
group
in the
interphase
appeared
to be
half
complete-differed
from
the
value
of
pK.
for
that
group
in
homogeneous
solution
in
the
direction
predicted
if one
issumes
it
is
more difficult
to create
a charge
in the
interphase
than
in
(5)
Bain,
C. D.; Whitesides,
G. M.
Angew.
Chem., Int.
Ed. Engt.19g9,
28,
506-5t2.
_
(6)
Jh9
polyethylene
film used
in
this study was
a
gift
from
Flex-Glas
Inc.
(
Flex-O-
Film DRT-600B).
(7)
Jain,
A.; Marzlufl
E.
M.; Jacobsen,
J. E.; Whitesides,
G.
M.;
Gra-
bowski,
J. J.
J. Chem.
Soc.,
Chem.
Commun.l9t9,
1557-1559.
(8)
Holmes-Farley,
S.
R.;
Whitesides,
G.
M. Langmuir
19t6,
2,266-2gt.
(9)
Grabowski,
J.
J.;Simon,
J. D.;
Peters,
K.
S.
/.
Am.
Chem.
Soc. 19g4.
r06,46t5-4616.
(10)
Measured
in
this
work.
(l
l)_The_procedure
used is
described
in
supplementary
materiar
in the
microfilm
edition.
E
o
LLJ
a
o
u
a
-cc
i:,
.
^i
T
,c
I
--j4:+=--%*
HO
A ):..
R'C
NH{
/)
NO
\
\
04
6
pH
Figure l. Acid-base titration curves
for the molecules
and
polyethylene
films indicated. The solid lines are the
calculated titration
curyes.r' S
I
Eo
refers to
the observed PAC signal normalized
to laser energy
and is based
on
the basic
PAC
equation. S
=
KfofL(l
-
l0-/). Inset
A: Photoacoustic
waves
at
pH
=
I
I 5
(-
- -)
and
pH
=
0.3
(-)
for the dansyl film
shown,
and for distilled
water
(--).
Inset B: Photoacoustic
waves
at
pH
=
10.0
(---)
and
ptl
=
0.8
(-)
ior the dansyl
derivative in homogeneous
solu-
tion. and ior distilled
water
(--).
For both insets,
the hatched
area
indicates
the
*integration-
pe
rformed
to obtain
S, the experimental value
of thc
photoacoustic
signal.
solurion.:
r'
T-hc
nragnirude of these
shifts
(2.3-4,1
pH
units)
is consistent
with
a
prei'ious
characterization of
a
PE-dansyl-water
interphase
as
hav'ing
an
effective dielectric constant
e
lu
9.8 For
all functionalizcd
films examined,
the fractional
change in the
amplitude of the PAC
signal for the functionalized
films
on
going
from low-
to high-pH
asymptotes
was
consistently
smaller than
that
for the
same
chromophore in
solution
(Figure
l). Experiments
are in
progress
to define the cause
of the changes in
relative
amplitudes.
Our
results demonstrate
that
PAC is a simple
and sensitive
method to
quantify
acid-base equilibria
at the interface
between
polyethylene
film
and
water.
This
photoacoustic
technique has
the advantages that it is insensitive
to scattering
of light from
the
interface and is easily
applicable to systems
in
which water
is
the
liquid
phase.
For PAC
to be useful
as a technique for
charac-
terization
of
interphases,
the signal
due to molecules
at the in-
terphase must be large compared
to
that
arising from
bulk solid
or liquid
phases.
The chromophore
used
to
label
the interphase
and to characterize the degree
of ionization should
therefore have
a high extinction coefficient relative
to that of the solid
and liquid
phases.
The system used here-with
optically
transparent
poly-
ethylene
and
water
as the two
phases
and
strongly absorbing
functional
groups
attached
at the
polyethylene-water
interphase-takes
advantage
of one
of the strengths
of
photoa-
coustic
spectroscopy: the
ability to detect very weak
absorption
against
a near-zero
background.l2
(
l2)
Harshbarger, W.
R.; Robin,
M. B. Acc.
Chem. Res. 1973,6,329-334.
Patel,
C. K. N.: Tam,
A. C. Reu.
Mod. Phys.198l,
5J, 517-550.
Sigrist, M.
W.
J. Appl. Phys.1986,60,
R83-Rl2l.
Tam, A.
C. Reu.
Mod. Phys.1986,
J8, 381-431.
Anderson,
V.
E.;Cheng,
H. Z.; Diebold,
G.
J.;
Mahmood, A.;
Sweigart,
D. A.
"/.
Am. Chem.
Soc. 1987, 109,6191-6193.
(13)
Strauss,
U. P.;
Vesnaver,
G. J. Phvs.
Chem.
1975.79.1558-1562.
707
|
We
believe that
PAC
has the
characterisrics to
be a highly
useful
tool for
studying interphases
between
optically transparent
solid
and liquid
phases,
provided
that an
appropriate reporter
group
with
a suitable
extinction
coefficient
can
be
localized
in thar
environmcnt.
Acknowledgment.
This
research
was
supported
by the Harvard
University
Materials
Research
Laboratorv
(\SF
Grant DMR-
86-14003). We
acknowledge
C. R.
Bertozzi.
.f
.
R. Jacobsen.
and
E. M.
Marzluff for
experimental
assistance
and
valuable
dis-
cussion.
Supplementary
Material
Available:
Methodologi' for
exrracting
pKr's
from the data
generated
in the PAC
studies described
in
the
paper
(2
pages).
Ordering information
is
grven
on
an\
current
masthead page.