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Synthesis, Self-Assembly Behavior, and BiologicalApplication of a New Photochromic Azo AmphiphilicDiblock Copolymer
Han Ding, Zheng Wang, Lijiao Sheng, Gongwu SongMinistry-of-Education Key Laboratory for the Synthesis and Application of Organic Functional Molecules,College of Chemistry and Chemical Engineering, Hubei University, Wuhan 430062, People’s Republic of China
Polymer (N,N-dimethyl-ethylamine methacrylate)-block-poly{6-[4-(4-methoxy phenyl-azo) phenoxy] hexylacrylate}p(DMAEMAm-b-AZOMn) was synthesized by successivereversible addition-fragmentation chain transfer poly-merization in the hydrothermal reactor. The productswere characterized by hydrogen nuclear magnetic reso-nance, differential scanning calorimetry, gel permeationchromatography, and ultraviolet and visible absorptionspectroscopy (UV-vis). In H2O/THF mixture, we foundamphiphilic p(DMAEMAm-b-AZOMn) self-assemblesoccurred. p(DMAEMA79-b-AZOM7) self-assembled intorods, p(DMAEMA79-b-AZOM5) self-assembled into giantmicrospheres with rods wind around, p(DMAEMA79-b-AZOM2) self-assembled into microspheres. Photochro-mic behaviors of the polymers in different environmentswere investigated. We found the colors of diblockcopolymers in films changed from yellow to orange afterirradiation by ultraviolet and visible (UV) light. The ratesof trans-cis photoisomerization in films were almost thesame for the three p(DMAEMAm-b-AZOMn) copolymers.The rates in aqueous micellar solutions were onlymarginally faster than those in films for all the threediblock copolymers. The observation of a sizable ratedifference in different environments for p(DMAEMAm-b-AZOMn) suggested that a rotational mechanism mightbe operative for these water-soluble amphiphilic diblockcopolymers. The self-assembly behaviors of threecopolymers and the application of p(DMAEMA79-b-AZOM2) microspheres in biochemistry were investigatedin present work. POLYM. ENG. SCI., 51:1662–1668, 2011.ª 2011 Society of Plastics Engineers
INTRODUCTION
Recently, much attention has been directed to the poly-
mer-based colloids because they are found to have some
potential usages in new areas such as microreactors,
targeted drug delivery, contrast enhanced imaging, and
mimic for biological membranes [1, 2]. Like small-mole-
cule surfactants, amphiphilic block copolymers can self-
assemble into micellar aggregates of various morpholo-
gies including star micelles, spheres, rods and vesicles in
selective solvents [3, 4]. Different factors, such as the ini-
tial copolymer concentration, the components of the
blocks and their ratio in the copolymers, the nature and
composition of the solvent, the temperature, the presence
of additives, and the polydispersity of the hydrophilic
block, provide control over the types and sizes of block
copolymer aggregates produced in solution [5, 6]. Many
efforts have been made to elucidate the formation of
block copolymer aggregates, with special emphasis on the
factors that control their types, the nature of the interface,
and their stability [7, 8].
Azobenzene-containing polymers (azo polymers for
short) have received considerable attention in recent years
because of their potential applications in the fields of opti-
cal data storage, liquid crystal displays, and holographic
surface relief gratings [9–11]. Upon light irradiation, azo
polymers show various photoinduced variations including
phase transition, chromophore orientation, surface-relief-
grating formation, and photomechanical bending, which
are based on the trans-to-cis and the cis-to-trans photoiso-merization of azo chromophores [12, 13]. The photores-
ponsive properties of azo polymers are connected with
the chemical structure of backbone and types of azo chro-
mophores. As a result, molecular design and synthesis of
azo polymers with desired photoresponsive properties
have aroused considerable research interest [14].
Functional polymer microspheres with carbonyl, hydroxyl,
and amino groups on their surfaces have been used to
covalently bind antibodies and other proteins onto micro-
spheres.
In this article, we report the synthesis of several azo
diblock copolymers of 2-(dimethylamino)ethyl methacry-
late (DMAEMA) monomer with azobenzene methacrylates
via reversible addition-fragmentation chain transfer (RAFT)
polymerization. To realize the anhydrous, high-pressure,
Correspondence to: Zheng Wang; e-mail: [email protected]
Contract grant sponsor: Foundation of Hubei Department of Education;
contract grant number: D20091006; contract grant sponsor: Opened
Research Foundation of Ministry-of-Education Key Laboratory for the
Synthesis and Application of Organic Functional Molecules of Hubei
University; contract grant number: 2007-KL-002.
DOI 10.1002/pen.21956
Published online in Wiley Online Library (wileyonlinelibrary.com).
VVC 2011 Society of Plastics Engineers
POLYMER ENGINEERING AND SCIENCE—-2011
and nitrogen environment, we use hydrothermal reactor to
process the polymerization. The self-assembly behaviors of
amphiphilic azo polymer p(DMAEMAm-b-AZOMn) with
different degrees of functionalization are investigated. In
addition, the photochromism of azo polymers in the film
and in the H2O/THF suspension are also investigated in
this article. We then discussed the biological application
of p(DMAEMAm-b-AZOMn) microspheres by fluorescence
technique.
EXPERIMENTAL
Materials
N,N-dimethylformamide (DMF), tetrahydrofuran
(THF), hexachlorohexanol, and 2,20-azobisisobutyronitrile(AIBN) were purchased from Sinopharm Chemical Rea-
gent Co. Ltd. Acryloyl chloride was purchased from Alfa
Aesar. 2-(dimethylamino)ethyl methacrylate (DMAEMA)
was purchased from Aladdin Reagent Co. Ltd. All the
chemicals were of analytical grade. All the solvents were
freshly distilled and were dehydrated before use.
The monomer {2-[4-(4-methoxy phenyl azo) phenoxy]
hexyl acrylate (AZOM)} was synthesized according to the
procedure similar to the published method [15]. The addi-
tion-fragmentation chain transfer agent dithiobenzoate [S ¼C(Ph)S-Ph] was synthesized according to the literature [16].
The stock solution of bovine serum albumin (BSA)
was 1.0 3 1025 mol L21 and was kept at 0–48C. The ini-
tial solution of p(DMAEMA79-b-AZOM2) microspheres
was 1.5 mg mL21.
Preparation of the Block Copolymer and Its Film
The synthetic route of p(DMAEMAm-b-AZOMn) diblock
copolymer was outlined in Scheme1. The macro-RAFT
agent, poly(2-(dimethylamino)ethyl methacrylate) capped
with dithiobenzoate (PDMAEMA-SC(S)Ph), was synthe-
sized by RAFT polymerization using [S ¼ C(Ph)S-Ph] as
chain transfer agent in THF at 758C for 48 h. PDMAEMA-
SC(S)Ph was then reacted with hydrophobic azobenzene
monomer {2-[4-(4-methoxy phenyl azo) phenoxy] hexyl
acrylate (AZOM)} to obtain poly (N,N-dimethyl-ethylamine
methacrylate)-block-poly{6-[4-(4-methoxy phenyl-azo) phe-
noxy] hexylacrylate} p(DMAEMAm-b-AZOMn). The proc-
dure was described as follows: PDMAEMA-SC(S)Ph
(0.25g), AZOM (0.5 g, 0.26 g, and 0.128 g, respectively)
and AIBN were dissolved in anhydrous THF (5 mL). The
mixture was added to the Teflon-lined reactor with N2
protection, and was heated at 758C for 24 h. The polymer
was obtained by precipitation in excess of hexane. The
reprecipitation process was carried out for three times. The
polymer was dried in a vacuum oven at 308C. The % yields
of p(DMAEMA79-b-AZOM7), p(DMAEMA79-b-AZOM5),
and p(DMAEMA79-b-AZOM2) copolymers are 41.2%,
SCHEME 1. Synthetic route of the p(DMAEMAm-b-AZOMn) diblock copolymer.
DOI 10.1002/pen POLYMER ENGINEERING AND SCIENCE—-2011 1663
39%, and 31.7%, respectively. The film of the polymer was
obtained by dip-coating from THF solution (10 wt %) onto
a quartz surface.
The Self-Assembly of p(DMAEMAm-b-AZOMn) in theSolution
The self-assembly process was performed by adding
Milli-Q water at a rate of 10 lL/s, with stirring into a
THF solution of the diblock copolymer p(DMAEMAm-b-AZOMn) with the initial concentration of 2 mg/mL. The
volume ratio of H2O/THF was about 1:1. And the mixture
was left to equilibrate for 24 h.
Measurements
The hydrogen nuclear magnetic resonance (1H NMR)
spectra of the block copolymer was measured in CDCl3using a UNITY INOVA 600 NMR spectrometer. Thermal
phase transitions were examined using a Perkin-Elmer
DSC-7 differential scanning calorimeter with a heating rate
of 108C/min. An Agilent 1100 series gel permeation chro-
matography (GPC) system equipped with a LC pump, a
PLgel 5 lm Mixed-C column calibrated using linear poly-
styrene standards and a refractive index (RI) detector was
used to determine polymer molecular weights and molecu-
lar weight distributions. Transmission electron microscopy
(TEM) images of the polymer vesicles and cylindrical
micelles were obtained by using a Tecai/G2-20-S-TWIN
(Fillip) microscope. The fluorescence emission spectra and
resonance light scattering (RLS) spectra were obtained on a
RF-540 spectrofluorophotometer (Shimadzu, Kyoto, Ja-
pan). Ultraviolet and visible absorption spectroscopy (UV-
vis) were recorded on a UV-2300 PC spectrophotometer
(Techcomp Bio-Equipment LTD, Shanghai, China).
Spectroscopic and Transmission Electron MicroscopyMeasurements
Bovine serum albumin (BSA) concentration was fixed at
3.333 1026 mol L21 and the solution was titrated by succes-
sive additions of working solution of p(DMAEMA79-b-AZOM2)microspheres (1.533 1025mol L21). Titrations were
done manually by using a microinjector. The BSA
fluorescence emission spectra were then obtained at the
excitation of 280 nm in the wavelength range of 300–500 nm.
Resonance light scattering (RLS) spectra of p(DMAEMA79-b-AZOM2) microspheres, BSA, and microspheres-BSA systems
were obtained by simultaneously scanning the excitation and
emissionmonochromators (Dk¼ 0 nm) from 300 to 600 nm.
The morphologies of the aggregates self-assembled
from p(DMAEMA79-b-AZOM7), p(DMAEMA79-b-AZOM5) and p(DMAEMA79-b-AZOM2) copolymers were
characterized by TEM technique. Samples were first
stained with uranium acetate, and a drop of the samples
was then placed on a Formvar-coated copper grid which
was dried in air. The TEM images were obtained at 258Cat an electron acceleration voltage of 120 kV.
RESULTS AND DISCUSSION
Characterization of Polymers
The composition of the block copolymer p(DMAEMA79-
b-AZOM5) is determined by 1H NMR spectrum, which
is illustrated in detail in Fig. 1. In Fig. 1, each band in1H NMR spectra is listed in accordance with the ‘‘H’’ atoms
in the structure of copolymer (named from a to q).
Molecular weights (Mn) and polydispersity index (PDI)
of the macroinitiator p(DMAEMA-SC(S)Ph) and the
diblock copolymer p(DMAEMAm-b-AZOMn) are deter-
mined by GPC. Well-controlled copolymerizations of
hydrophobic azobenzene monomers are observed. The
results are summarized in Table 1.
The differential scanning calorimetry (DSC) heating
curves of diblock copolymer p(DMAEMA79-b-AZOM7)
(Fig. 2a) and p(DMAEMA79-b-AZOM5) (Fig. 2b) are
shown in Fig. 2. PAzoMA is known to have a smectic (S)
and nematic (N) phase [17, 18]. For p(DMAEMA79-b-AZOM7), the glass transition was observed to occur at Tg¼ 518C, the liquid crystalline transition at 888C, and the
isotropic transition at 1158C. The diblock copolymer
p(DMAEMA79-b-AZOM5) and p(DMAEMA79-b-AZOM2)
show similar DSC thermograms, but with lower corre-
sponding transitions temperatures, respectively, due to the
decrease of AZOM block. The phase transition tempera-
tures for 3 copolymers are included in Table 1.
Self-Assembly of p(DMAEMAm-b-AZOMn) in theH2O/THF Solution
In solution, the formation of block copolymer aggre-
gates of various morphologies is controlled by a forceFIG. 1. Hydrogen nuclear magnetic resonance (1H NMR) spectrum of
p(DMAEMA79-b-AZOM5) in CDCl3.
1664 POLYMER ENGINEERING AND SCIENCE—-2011 DOI 10.1002/pen
balance between three different factors: the degree of
stretching of the core-forming blocks, the interfacial ten-
sion between the micelle core and the solvent outside the
core, and the repulsive interactions among corona forming
chains [19]. The morphologies can be controlled through
variations in the copolymer composition, the initial copol-
ymer concentration, the nature of the common solvent,
the amount of water present in the solvent mixture, the
temperature and so on [20]. In this article, the self-assem-
bly behaviors of p(DMAEMAm-b-AZOMn) with different
degrees of functionalization are investigated in H2O/THF
dispersion media. Amphiphilic polymers can self-assem-
ble into an ordered architecture to minimize the interfacial
energy in suitable solvents. THF is used to dissolve
both the hydrophobic and hydrophilic blocks of
p(DMAEMAm-b-AZOMn) to form a diblock copolymer
solution. Water is then added as a precipitant for the
hydrophobic block to induce self-assemble. Figure 3a–3c
show the TEM images of the self-assembled aggregates
of p(DMAEMA79-b-AZOM7), p(DMAEMA79-b-AZOM5)
and p(DMAEMA79-b-AZOM2) in the H2O/THF disper-
sion media, respectively. Rods are observed in Fig. 3a.
And microspheres with different diameters are observed
in Fig. 3b and c. As the hydrophobic block length
decreases, the morphology of the diblock copolymer
p(DMAEMAm-b-AZOMn) changes from rods to micro-
spheres. Besides, it is interesting that the surface of
p(DMAEMA79-b-AZOM5) microspheres is smoother than
that of p(DMAEMA79-b-AZOM2) microspheres. From the
facts above, we can conclude that the block length ratio
of the hydrophilic block p(DMAEMA) to hydrophobic
block p(AZOM) provides control over the types, sizes
and microstructures of block copolymer aggregates pro-
duced in H2O/THF dispersion media. The higher the
block length ratio was of p(DMAEMA) to pAZOM, the
greater the tendency was to form microspheres. It may be
that as the length of the pAZOM block increases, the
morphology changes for equal p(DMAEMA) block
lengths, this results in a decrease in repulsion.
Photochromic and Photoisomerization of the DiblockCopolymer p(DMAEMAm-b-AZOMn)
The color of diblock copolymers in films changes from
yellow to orange after irradiation by ultraviolet and visi-
ble (UV) light because of the isomerization. We can see
from Fig. 4 that the absorbance at 460 increases with the
irradiation time.
The trans-to-cis photoisomerization of the
p(DMAEMAm-b-AZOMn) diblock copolymer in the film
and in the H2O/THF suspension are studied respectively.
The film and the stable suspension of the diblock copoly-
mer are irradiated with 365 nm ultraviolet and visible
FIG. 2. (a) Differential scanning calorimetry (DSC) heating curves of
diblock copolymer p(DMAEMA79-b-AZOM7). (b) Differential scanning
calorimetry (DSC) heating curves of diblock copolymer p(DMAEMA79-
b-AZOM5).
TABLE 1. Synthesis conditions and characteristics of p(DMAEMA79) homopolymer and p(DMAEMAm-b-AZOMn) diblock copolymers.
Sample Time (h) [AIBN] mol L21 1023 [Monomer] mol L21 Mn (GPC) PDI
Phase transition
temperature (8C)
p(DMAEMA79) 48 2 12,635 1.09
p(DMAEMA79-b-AZOM7) 24 1 0.524 15,228 1.25 g51 S88 N115
p(DMAEMA79-b-AZOM5) 24 1 0.282 14,742 1.20 g48 S79 N111
p(DMAEMA79-b-AZOM2) 24 1 0.134 13,412 1.16 g41 S78 N102
g, glassy phase, S, smectic phase, N, nematic phase.
DOI 10.1002/pen POLYMER ENGINEERING AND SCIENCE—-2011 1665
(UV) light until they reach the photostationary state. The
samples were then kept in the dark where the reverse
cis-to-trans isomerization occurred due to thermal energy
as the trans form was thermodynamically more stable.
The samples irradiated with 440 nm visible light can also
result in reverse cis-to-trans isomerization. In aqueous
solutions, the copolymers formed giant microspheres and
rods. The spectra changes with different irradiation time
and the reverse cis-trans thermal isomerization at differ-
ent time intervals are shown in Fig. 5 for p(DMAEMA79-
b-AZOM2) in films: (a) before and after ultraviolet and
visible (UV) irradiation at 366 nm reaching the photosta-
tionary state; (b) after in the dark; (c) irradiation at 460
nm reaching the photostationary state. The absorbance at
360 nm corresponds to the trans azobenzene (p-p* transi-
tion) and the maximum at 450 nm belong to the cis azo-
benzene. Similar behavior was observed in aqueous solu-
tions. The UV-vis spectra of p(DMAEMA79-b-AZOM7)
and p(DMAEMA79-b-AZOM5) show similar features. The
rate of isomerization was analyzed from the absorbance at
360 nm, corresponding to the p-p* transition. From the
equation ln(A!2At)/(A!2A0) ¼ 2kt [20], the first-order
rate constant of isomerization is determined, where At, A0,
and A! are the absorbance a 360 nm at time t, time zero,
and infinite time, respectively. Similar linear plots were
obtained for the three copolymers in aqueous solutions.
The corresponding first-order rate constants kt-c (for transto cis) obtained is shown in Table 2.
The photoisomerization rates were found to be about the
same for p(DMAEMA79-b-AZOM7), p(DMAEMA79-b-AZOM5) and p(DMAEMA79-b-AZOM2) films. The kt-c(s21) of above 3 copolymers in solutions are 10.857 31023, 11.5873 1023, and 12.0013 1023, respectively. The
kt-c (s21) of above 3 copolymers in films are 9.594 3 1023,
9.228 3 1023, and 10.362 3 1023, respectively. Interest-
ingly, the rates of photoisomerization were fractionally
slower for all the corresponding copolymers in solutions.
In aqueous solution, the diblock copolymers self-assembled
into microspheres and rods. Apparently, the structural
differences of the polymeric micelles and the films did not
FIG. 3. Transmission electron microscopy (TEM) images of
p(DMAEMAm-b-AZOMn): (a) p(DMAEMA79-b-AZOM7) (rods), (b)
p(DMAEMA79-b-AZOM5) (giant microspheres with tubes wind around),
and (c) p(DMAEMA79-b-AZOM2) (microspheres).
FIG. 4. Photochromic of the p(DMAEMAm-b-AZOMn) diblock copoly-
mer: (a) p(DMAEMA79-b-AZOM7); (b) p(DMAEMA79-b-AZOM5); (c)
p(DMAEMA79-b-AZOM2).
1666 POLYMER ENGINEERING AND SCIENCE—-2011 DOI 10.1002/pen
result in any significant differences in the rate of photoiso-
merization. which is similar to the previous results obtained
by Sin et al. [21]. In aqueous solution, the diblock
copolymer self-assemble into core-shell micelles with the
hydrophobic core formed by azo block. The formation of
micelles shield the core azobenzene from the solvent
water, and the core azobenzene is in a more hydrophobic
environment than in the film. It can be estimated that the
isomerization of p(DMAEMAm-b-AZOMn) proceeds via a
rotational mechanism.
The Application of p(DMAEMA79-b-AZOM2)Microspheres in Biochemistry
Drug and Biomacromolecules Delivery System. The
amphiphilic diblock copolymers can self-assemble into
microspheres which are composed of a hydrophobic core
and a hydrophilic shell and the microspheres can then
potentially act as drugs and biomacromolecules carriers.
They will interact with serum albumin, the most abundant
carrier protein in blood plasma. So it is important to
investigate the interaction of serum albumin with carriers.
In present work, fluorescence quenching technique [22] is
used to discuss the binding interaction between
p(DMAEMA79-b-AZOM2) microspheres and a model pro-
tein-BSA. The fluorescence quenching spectra of BSA in
the presence of p(DMAEMA-b-AZOM) microspheres are
shown in Fig. 6. The results revealed that with more
p(DMAEMA79-b-AZOM2) microspheres, the fluorescence
intensity of BSA at 350 nm (exited at 280 nm) decreased
FIG. 6. Effect of p(DMAEMA79-b-AZOM2) microspheres on fluores-
cence spectra of BSA (kex ¼ 280 nm). (a?g) c(BSA)¼ 3.33 3 1026
mol L21, working solution of spheres is 1.53 3 1025 mol L21, V(Azo
microspheres) (lL): 20, 40, 60, 80, 100, 120, and 140, respectively.
FIG. 5. UV-vis spectra of p(DMAEMA79-b-AZOM2) film (a) before
and after UV irradiation at 366 nm reaching the photostationary state,
(b) after in the dark, and (c) irradiation at 460 nm reaching the photosta-
tionary state.
TABLE 2. First-order rate constants, kt-c, for the trans-to-cisphotoisomerization of p(DMAEMA79-b-AZOM7), p(DMAEMA79-b-
AZOM5), and p(DMAEMA79-b-AZOM2) in film and aqueous solution.
Diblock copolymers 103kt-c (s21)
Dip-coated films
p(DMAEMA79-b-AZOM7) 9.594
p(DMAEMA79-b-AZOM5) 9.228
p(DMAEMA79-b-AZOM2) 10.362
Aqueous solutions
p(DMAEMA79-b-AZOM7) 10.857
p(DMAEMA79-b-AZOM5) 11.587
p(DMAEMA79-b-AZOM2) 12.001
DOI 10.1002/pen POLYMER ENGINEERING AND SCIENCE—-2011 1667
significantly with a slight blue shift and the emission band
of azobenzene at 470 nm emerged step by step
(Fig. 6a?g), indicating that microspheres could act as
quenchers and the binding interaction between BSA and
microspheres occurred with complex formation. The
above phenomenon revealed that p(DMAEMA79-b-AZOM2) microspheres can be potentially applied as pro-
tein carriers and the inherent binding information such as
binding mode, binding sites, interaction force, etc., can be
investigated in detail in future studies.
Detection of Proteins. We also used RLS spectra to
discuss the interaction and the RLS spectra of
p(DMAEMA79-b-AZOM2) microspheres-BSA system
were displayed in Fig. 7. The RLS intensities of both
BSA and azo microspheres in the wavelength range of
300–600 nm were rather weak. When mixed together,
however, an enhanced peak could be observed at 370 nm
and the RLS signals increased with increasing BSA con-
centration. According to the RLS theory [23], the
enhanced RLS signals in this work could further prove
that the micron sized complexation of azo microspheres
and BSA occurred. Apart from that, the results indicated
that the amphiphilic diblock copolymer p(DMAEMA79-b-AZOM2) and the microspheres can be potentially used as
fluorescence probes in the determination of BSA by RLS
method. The optimization of experimental conditions in
the detection can be further discussed in future papers.
CONCLUSION
A new amphiphilic azobenzene diblock copolymer
p(DMAEMAm-b-AZOMn) was synthesized via reversible
addition-fragmentation chain transfer polymerization in
the hydrothermal reactor. Colloidal spheres, rods and
microspheres are obtained through gradual hydrophobic
aggregation of azobenzene diblock in H2O/THF disper-
sion media. With the decrease of length of the pAZOM
block, p(DMAEMAm-b-AZOMn) self-assembly morphol-
ogy changes from rods to microspheres. The colour of
diblock copolymers in films changes from yellow to or-
ange after irradiation by ultraviolet and visible (UV) light.
The lower photoisomerization rate constant of
p(DMAEMAm-b-AZOMn) in the film than in the H2O/
THF suspension indicates the rotational mechanism of the
isomerization of p(DMAEMAm-b-AZOMn). Apart from
that, p(DMAEMAm-b-AZOMn) can be potentially used in
the drug delivery system and the determination of BSA.
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FIG. 7. Resonance light scattering (RLS) spectra of p(DMAEMA79-b-
AZOM2) microspheres-BSA system. (1) 1.4 3 1026 mol L21 BSA;
(2?6) c(microspheres) ¼ 2.04 3 1027 mol L21; c(BSA)(31026 mol
L21): 0, 0.2, 0.6, 1, 1.4.
1668 POLYMER ENGINEERING AND SCIENCE—-2011 DOI 10.1002/pen