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Characterizations on the Stability and Release Properties of #-ionone Loaded Thermosensitive Liposomes (TSLs) Ling Chen, Rong Liang, Yihan Wang, Wallace Yokoyama, Maoshen Chen, and Fang Zhong J. Agric. Food Chem., Just Accepted Manuscript • DOI: 10.1021/acs.jafc.7b06130 • Publication Date (Web): 30 May 2018 Downloaded from http://pubs.acs.org on May 30, 2018
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Journal of Agricultural and Food Chemistry
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TITLE HEADER
2
Characterizations on the Stability and Release Properties of β-ionone Loaded
3
Thermosensitive Liposomes (TSLs)
4 5
Ling Chena,b, Rong Liangc, Yihan Wange, Wallace Yokoyamad, Maoshen Chena,b, Fang Zhong*a,b
6 7
a
8
Jiangnan University, Wuxi 214122, China
9
b
Key Laboratory of Synthetic and Biological Colloids, Ministry of Education,
School of Food Science and Technology, Jiangnan University, Wuxi 214122, China
10
Jiangnan University, Wuxi 214122, P.R. China
11
c
12
of Chemical and Material Engineering, Jiangnan University, Wuxi 214122, P.R. China
13
d
Western Regional Research Center, ARS, USDA, Albany, CA 94710, USA
14
e
Zhejiang Institute for Food and Drug Control, Zhejiang 310000, P.R. China
Key Laboratory of Synthetic and Biological Colloids, Ministry of Education, School
15 16 17 18 19 20 21 22 23 24 25 26 27 28
* To whom correspondence should be addressed. Tel: +86(510)85197876, Email:
29
[email protected]. 1 ACS Paragon Plus Environment
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ABSTRACT:
31
Liposomes with phase transition temperatures, Tm, near pathogenic site
32
temperature are potential chemoprophylactic delivery vehicles. We prepared and
33
characterized the thermal properties of liposomes composed of DPPC and HSPC
34
incorporating β-ionone with Tm at 42℃. Liposomes with β-ionone/lipid ratio (wt/wt)
35
of 1:20 and 1:8 had the necessary stability and released most of the β-ionone. The
36
molecular architecture surround Tm was studied by fluorescent probes, Raman
37
spectroscopy and DSC. β-ionone was found to be preferentially located in the deep
38
regions of lipid bilayer (toward the long chain alkyl of the lipid) at moderate loading.
39
The results showed that β-ionone encapsulated liposomes have a superior release at
40
higher loading amount. Increasing β-ionone leads to disorder in the liquid crystalline
41
state and accelerates the release rate. These studies provide information on the
42
membrane structural properties of β-ionone loaded liposomes that guide rational
43
bioactive molecular delivery systems designing for health product.
44 45
Key words: Thermosensitive liposomes (TSLs), β-ionone, microviscosity, DSC,
46
Raman spectroscopy
47
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Journal of Agricultural and Food Chemistry
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INTRODUCTION
49
Chemoprevention is effective in treating cancer and inflammation to promote
50
human health. However, a major obstacle is systemic toxicity accompanying effective
51
chemotherapy at target tissues necessitates high delivery concentration of bioactive
52
molecules
53
anticancer component during delivery through the circulatory system while producing
54
a burst release only at the diseased tissue has been a goal of many laboratories.
55
Thermosensitive liposomes (TSLs) that release their encapsulated drug by heat at the
56
tumor site have been demonstrated to be a valid approach to transport and release
57
anticancer drugs to solid tumors (4). This delivery system was first proposed by Yatvin
58
et al. in 1978 for use at sites of mild local hyperthermia
59
to transport a variety of drugs. Agarwal et al. reported a thermosensitive liposomal
60
nanocarrier that held doxorubicin (DXR) up to 24 h and release it at 43℃
61
Melphalan encapsulated TSLs with the phase transition temperature of 42.7℃ were
62
designed by Chelvi for hyperthermia-mediated targeted delivery to murine tumors
63
TSLs reported by Winter et al, were also characterized for delivering the anticancer
64
drug arsenic trioxide (ATO)
65
phospholipid (phosphatidyldiglycerol) based TSLs in a feline sarcoma study has been
66
reported by Zimmermann et al.(9) In addition, one clinical study using combinations of
67
hyperthermia
68
www.ClinicalTrials.gov site, with the Celsion phase I clinical trial for patients with
69
liver tumors been completed, and the phase III trial for treating hepatocellular
(1-3)
. Therefore, research to develop a delivery system that would retain its
and
TSLs
(5)
. Later, TSLs were applied
(6)
.
(7)
.
(8)
. Recently, a preclinical trial using a synthetic
(ThermoDox®)
has
been
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listed
on
the
NIH
Journal of Agricultural and Food Chemistry
70
carcinoma and phase II trial for breast cancer patients still in the progress (10).
71
β-ionone, one of the estimated 22,000 isoprenoid products of secondary plant
72
mevalonate metabolism, is widely found in algae, fruits, flowers and vegetables. It is
73
derived from the cleavage of the 9, 10 double bound of β-carotene by a dioxygenase
74
(11)
75
breast cancer and meningioma cells, through suppression of cell division and
76
initiation of apoptosis
77
mammary carcinogenesis via the downregulation of cyclin D1 and Bcl-2 expression
78
and upregulation of Bax expression
79
anticancer properties to gastric adenocarcinoma cells with the IC50 value of 89 µmol/L
80
(13)
81
chemopreventive and antitumor agent, few applications of β-ionone in an antitumor
82
delivery system were developed. It has been reported via numerous research studies
83
that liposome was an effective approach to encapsulate isoprenoids, such as
84
β-carotene, astaxanthin or coenzyme Q10 (17-19). β-ionone, a decomposition product of
85
β-carotene, possessing the similar hydrophobic properties and groups with β-carotene,
86
might has the potential to be incorporated by liposomes. The objective of this research
87
was to investigate the use of TSL as a delivery system for β-ionone to promote it
88
healthy benefits.
. β-ionone has been reported to inhibit the growth of melanoma, gastric cancer,
(12-15)
. For instance, β-ionone could suppress DMBA-induced
(16)
. Additionally, Liu et al. have also studied its
. Although recent research has found that β-ionone may be a potential
89
The precise phase transition temperature, Tm, is the most essential property of
90
TSLs. It is well known that liposomes remain stable and exhibit minimal drug release
91
below their Tm, but release their encapsulated material when the temperature reaches 4 ACS Paragon Plus Environment
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Journal of Agricultural and Food Chemistry
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the Tm (20). TSLs are distinguished from typical liposomes by possessing a narrow Tm.
93
TSLs ideally are selective and release therapeutic levels of drugs only at the targeted
94
temperature at the local tumor site without damaging peripheral noncancerous tissues.
95
Research suggests that Tm in the range of 39-43℃ is optimum to reduce pre-leakage
96
of
97
2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC, Tm = 41.3℃) and hydrogenated
98
soy phosphatidylcholine (HSPC, Tm = 52.7℃) have been used to prepare TSLs in this
99
Tm range
drugs
at
body
temperature
(37℃)
(21)
.
1,
(4, 22)
. Previous studies have suggested that the positively charged part of
100
HSPC interacts with the negatively charged part of DPPC by electrostatic interaction
101
resulting in a complex with a single phase transition
102
compositions of PCs, the amount of core material has been reported to affect the Tm as
103
well. The incorporation of temoporfin into liposomes composed of DPPC and
104
dipalmitoyl-phosphatidylglycerol (DPPG) resulted in a distinct decrease of the Tm (24).
105
These studies demonstrate the impact of proportion ratios of wall material and the
106
loading amount of encapsulated drugs on Tm and these properties will be discussed
107
later in detail. In addition, other requirements like the physicochemical stability
108
during storage, ultrafast drug release upon heating and the in vitro stability in serum
109
have been reported to be key roles for TSLs design as well(25, 26), so the storage
110
stability and the release behaviour in biological medium with serum would also
111
characterized in the following study.
(23)
. In addition to the
112
In this study, differential scanning calorimeter (DSC) was used to measure Tm as
113
a function of membrane composition and β-ionone loading. The stability and shelf life 5 ACS Paragon Plus Environment
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of β-ionone loaded TSLs were characterized by measuring changes in the Z-average
115
particle diameter, phospholipid profiles, TEM images and retention rate during
116
storage. The liposomal release properties were also characterized by in vitro release
117
tests with serum. Release behavior was further analyzed by fluorescence and Raman
118
spectra. The potential application of β-ionone loaded TSLs to deliver effective doses
119
of bioactive molecules, as well as the relationship between β-ionone release behavior
120
and liposomal structural properties were evaluated.
121
MATERIALS AND METHODS
122
Materials
123
HSPC (with the main component of DSPC, 97%) and DPPC were acquired from
124
Shanghai Advanced Vehicle Technology L.T.D. Co (Shanghai, China). β-ionone
125
standard was purchased from ANPEL laboratory Technologies Shanghai Inc
126
(Shanghai, China). The fluorescent probe 1-anilinonaphthalene-8-sulfonate (ANS, 98%
127
purity),
128
trimethylammonium-DPH (TMA-DPH, 98% purity) were obtained from Sigma
129
Chemical Co. (St. Louis MO, USA). Fetal Bovine Serum (FBS) was purchased from
130
Gibco (Grand Island, NY). Ultra-pure grade water purchased from A.S. Watson Group,
131
Ltd. (Hong Kong, China) was used for HPLC tests and other experiments. Tween 80
132
and other analytical grade reagents were from China Medicine (Group) Shanghai
133
Chemical Reagent Co. (Shanghai, China).
134
Preparation of β-ionone Liposomes
135
1,
6-diphenyl-1,
3,
5-hexatriene
(DPH,
98%
purity),
and
Liposomes of different PC composition were prepared by the thin film hydration 6 ACS Paragon Plus Environment
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Journal of Agricultural and Food Chemistry
(27)
136
method developed by Xia et al
. 200 mg of PCs (DPPC, HSPC or the mixture of
137
DPPC and HSPC at different molar ratios), 50 mg of Tween80 and a range of amounts
138
(0-200 mg) of β-ionone were dissolved in ethanol in a round bottom flask. The solvent
139
was evaporated with a rotary evaporator at 50℃ to form a thin film of dry lipid on the
140
wall of the flask. The film was then hydrated by adding 20 mL of phosphate buffer
141
solution (0.05 M phosphate buffer solution, 0.15 M NaCl, PBS, pH 6.8) under
142
vigorous stirring at 50℃ for 30 min to form multilamellar vesicles (MLV). The
143
liposomal suspension was formed by ultrasonic probe processing of the MLV in an ice
144
bath for 4 min at 20% amplifying strength with 1 s of sonication and 1 s rest.
145
Vesicle Size Measurement
146
Z-Average diameter of β-ionone liposomes were evaluated by dynamic light
147
scattering (DLS) with a Nano Particle Analyzer (ZetaPALS, Brookhaven Instruments
148
Ltd., USA), according to methods in our previous report
149
aliquots of liposomal dispersion were suspended in 5 mL of phosphate buffer (0.05 M
150
phosphate buffer solution, 0.15 M NaCl, PBS, pH 6.8) to avoid multiple scattering
151
phenomena due to interparticle interaction. The prepared β-ionone liposomes were
152
then transferred to polystyrene cuvettes, and the Z-Average diameter (𝐷𝑧) and PDI
153
were recorded by DLS using the Nano-Zeta PALS particle size analyzer with a He/Ne
154
laser (λ = 633 nm) and scattering angle of 90°. 𝛥𝐷𝑧 was used to evaluate the
155
physical stability during the storage, calculating by the function as follows:
156
𝛥𝐷𝑧 =
157
Determination of Tm by Differential Scanning Calorimetry (DSC)
(28)
. Briefly, dilute 100 μL
The average diameter after storage-The average diameter initially prepared The average diameter initially prepared
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158
DSC (NETZSCH Instrument Ltd., Germany) thermograms were evaluated to
159
determine the phase transition temperature (Tm) of the liposomes with different
160
HSPC/DPPC ratios and β-ionone/lipid ratios, using an empty aluminum crucible with
161
a lid as a reference
162
transfered to 40 μL aluminum pans, which was subsequently sealed and measured.
163
The samples were scanned from 20 to 60℃ at 5℃/min in duplicate to ensure
164
exemption of the thermal history of the specimens (30).
165
Retention Rate
(29)
. Briefly, 10 μL of the β-ionone liposomal suspension was
166
Total β-ionone in the liposomal suspension was released by completely breaking
167
vesicles with TritonX-100. The concentration of β-ionone was assayed by HPLC
168
(Waters2695, Waters, Milford, MA) at 304 nm compared to a β-ionone standard curve.
169
The retention rate (RR) was calculated by the percentage of total amount of β-ionone
170
after storage relative to the total amount of β-ionone initially prepared.
171
RR(%) = Total amount of β-ionone
172
HPLC Analysis of β-ionone
173
High-performance liquid chromatography (RP-HPLC) was conducted to determine
174
the concentration of β-ionone (Waters, Milford, MA) equipped with a UV-VIS
175
detector, based on the method reported by Waldmann et al (31). In short, sterile syringe
176
filters (0.22 μm) were used to remove particulate contaminants from each sample
177
prior to analysis. Chromatographic separation was performed on a Waters Symmetry
178
C18 (Lichrosphere, 5 mm, 250×4.6 mm, Waters, Milford, MA) column at 30℃. The
179
mobile phase was a mixture of acetonitrile and ultrapure water (70:30). The flow rate
Total amount of β-ionone after storage initially prepared
× 100%
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Journal of Agricultural and Food Chemistry
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was 1.0 mL/min. The detection wavelength was 304 nm and the sample volume was
181
20 μL.
182
HPLC-MS Analysis of Phospholipid Profile
183
HPLC-ESI-MS/MS technique was applied to analyze the decomposition (32)
Briefly, 1 μL
184
products of the phospholipids according to the method of Zhu et al.
185
lipid samples (with the phospholipid concentration of 1 mg/mL) were injected into a
186
Acquity UPLC Hilic column (2.1 × 100 mm, 1.7 μ m, Waters, Milford, MA) with
187
mobile phase flow rate of 0.3 ml/min. Solvent A and B were hexane and ammonium
188
acetate solution (20 mmol/L), respectively, with the analysis time of 10 min. The
189
thermostat column compartment was operated at 30°C, and the jet stream ESI source
190
was operated in the negative mode. Instrument parameters were set as follows: sheath
191
gas temperature of 100°C; sheath gas flow of 50 L/min; dry gas temperature of 250°C;
192
dry gas flow of 500 L/h; capillary entrance voltage of 3.5 kV; and kimmer voltage of
193
6 V. The MS scan data were collected in the range of m/z 782, 520 and 258. MS data
194
of phospholipids compositions were extracted by MassLynx Software (V4.1).
195
Transmission Scanning Electron Microscope TEM
196
The morphology of empty and β-ionone loaded liposomes were visualized via
197
transmission electron microscopy (TEM, H-7650, HITACHI, Japan) according to our
198
previously reported method.(33) A fresh copper mesh grid was placed onto droplets
199
containing pre-diluted liposomal suspension and excess liquid was removed with filter
200
paper after 4 minutes. Samples were air dried at room temperature, the morphology of
201
the liposomes was recorded by TEM at a voltage of 80 kV. 9 ACS Paragon Plus Environment
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202 203
In vitro Release Studies The release rate of β-ionone in vitro was determined according to the method of (34, 35)
204
Yang et al. and Comiskey with minor modification
205
liposome with its β-ionone /lipid ratio of 1:8 was put into a dialysis bag (MW cutoff
206
3000, Sinopharm Co., China), and then transferred to a 250 mL beaker with 200 mL
207
dialysis medium (20% ethanol with 10% serum). This dialysis device was stirred in a
208
thermostatted water bath at 200 rpm under different temperatures of 25, 35, 42 and
209
50℃. At predetermined time intervals (0, 10, 30, 60, 90, 120, 180 min), 200 μL
210
samples of the release medium were withdrawn and replaced with equal volume of
211
fresh release medium. The β-ionone concentration in release medium was analyzed by
212
HPLC, following the methods mentioned. To investigate the release behavior of
213
liposomes loaded with different amount of β-ionone, the release assay were carried
214
out with β-ionone /lipid ratio of 1:20 and 1:8 and the incubation temperature of 42℃.
215
Microviscosity of Liposomal Bilayer Membranes
216
. For the assay, 5 mL of
The liposomal membrane fluidity was measured according to the method of Xia (27, 36)
217
and Tan et al
. Microviscosity is inversely related to membrane fluidity. High
218
microviscosity or lower membrane fluidity values are an indication of higher
219
structural order (37). Microviscosity of the membrane adjacent to a fluorescent probe is
220
positively correlated to the fluorescence polarization of the probe and can be
221
calculated using the Perin-Weber’s equation
222
of the membrane was determined by different fluorescent probes. DPH (oriented in
223
the deep regions of the lipid bilayer), ANS (oriented toward the hydrophilic
(38)
. The microfluidity at different depths
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headgroup of the lipid) and TMA-DPH (oriented on the surface and glycerol side
225
chain region of the membrane) were fluorescence probes used to investigate the
226
molecular movement in the lipophilic core, superficial region and exterior membrane
227
surface, respectively
228
to a final concentration of 6×10-3 mol/L. The DPH stock solution was prepared by
229
dissolving DPH powder in tetrahydrofuran, followed by adjusting the concentration to
230
2×10-3 mol/L. The DPH stock was kept at 4℃ in the dark. Then, aliquots of DPH
231
stock solution (100 μL) were added to the 10 mL volumetric flask diluted by fresh
232
buffer solution (0.01 M PBS, pH 6.8) and used at room temperature. The final
233
concentration of DPH was 2×10-5 mol/L. TMA-DPH stock solution was prepared by
234
dissolving TMA-DPH powders in tetrahydrofuran/water (1:1, v/v) and the
235
concentration was adjusted to 10-2 mol/L. Aliquots of TMA-DPH stock solutions (100
236
μL) were added into 10 mL volumetric flasks and diluted by fresh PBS. The final
237
TMA-DPH concentration was 10-4 mol/L. When determining the microviscosity of
238
liposomal membranes, a small quantity of probe stock solution was mixed with
239
β-ionone liposomes with their drug/lipid ratios varying from 1:40 to 1:4 to give a
240
lipid/probe molar ratio of 300:1 at room temperature. For investigating the membrane
241
fluidity changing during heating process, the incubation temperature was rise from 35
242
to 50℃. Note that the ANS solution must be dried by nitrogen before analysis to
243
avoid the destruction of the membrane by ethanol
244
which is correlated to microviscosity (η) near the fluorescent probes was calculated
245
using the Perrin-Weber’s equation as follows: (41)
(39, 40)
. Briefly, the ANS probe was dissolved in ethanol solution
(27)
. Fluorescence polarization (P)
11 ACS Paragon Plus Environment
Journal of Agricultural and Food Chemistry
(I
-GI
)
I
Page 12 of 49
246
P = (I 0,0+GI0,90 ), G = I 90,0
247
η = 0.46-P
248
where I0,0 and I0,90 are the fluorescence intensities of the emitted light polarized
249
parallel and perpendicular to the excitation light, respectively, and G is the grating
250
correction factor(42). The fluorescence intensities were measured at a range of
251
temperature from 30 to 50℃ with a florescence spectrometer (F-7000, Hitachi Co.,
252
Ltd, Japan). The excitation and emission wavelengths were 350 and 450 nm,
253
respectively, and the slit widths for both excitation and emission were 5 nm.
254
Raman Spectroscopy
0,0
(3)
90,90
0,90
2P
(4)
255
Raman spectroscopy was used to predict the location of β-ionone in the bilayer
256
membrane and characterize the structural properties according to the method of
257
Gardikis et al
258
interval 2 cm-1 via a Raman spectrometer (LabRAM HR Evolution, HORIBA Jobin
259
Yvon S.A.S. France) equipped with a 633 nm frequency stabilized laser source. The
260
collection time was 30 s, and the laser output power was 400 mV. The ordinary
261
Raman spectrum was baseline corrected, and the Raman intensities were measured as
262
peak height. Liposomes with different β-ionone/lipid ratios from 1:40 to 1:4 were held
263
at 25℃ in order to assess the change of the interaction between PCs and β-ionone at
264
increasing amounts, while liposomes with β-ionone/lipid ratios of 1:20 and 1:8 were
265
further investigated from 35 to 50℃. SL represents the changes in both the
266
trans/gauche population ratio and the lateral packing of the chains. ST represents the
267
degree of longitudinal order of liposomes
(43)
. Raman spectra were recorded in the ranges of 600-3000 cm-1 with
(37)
. These parameters were calculated from
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268
Journal of Agricultural and Food Chemistry
the equations as follows:
269
SL =
270
ST =
ICH2(Sample) -0.7 1.5
, ICH2 =I2882 /I2847
𝐼1130 /𝐼1086
(5) (6)
1.77
271
where I2882 /I2847 is the height intensity ratios of the peaks at 2882 and 2847 cm-1, and
272
𝐼1130 /𝐼1086 is the height intensity ratios of the peaks at 1130 and 2086 cm-1.
273
Statistical Analysis
274
All the data are expressed as mean±standard deviation (SD). All measurements
275
were performed at least in triplicate. The results were subjected to statistical analysis
276
by one-way ANOVA followed by multiple comparison test with SPSS software (SPSS
277
Inc., (SPSS Inc., Chicago, IL, USA). Differences were considered to be significant
278
when p < 0.05.
279 280
RESULTS AND DISCUSSION
281
Effect of Phospholipid Composition on Tm
282
Tm as a function of membrane composition was determined by DSC. The DSC
283
profiles (Fig. 1) for pure DPPC (trace a), HSPC (trace f) and their mixtures (traces b-e)
284
show phase transitions from 41.30℃ to 53.12℃. HSPC had the highest and DPPC the
285
lowest Tm, agreeing with published data (44, 45). For liposomes composed of both HSPC
286
and DPPC, the greater proportion of HSPC led to higher Tm, which is attributed to the
287
longer acyl chain length and stronger interactions of HSPC (23, 46) This result is highly
288
consistent with that reported by Chen et al. that Tm would rise with increasing HSPC
289
content (with longer length of acyl chains) and decreased after adding DLPC (with
290
shorter acyl chain length) (23). The temperature peak width at half peak height, T1/2, is 13 ACS Paragon Plus Environment
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(47)
291
inversely proportional to the co-operativity of the phospholipid bilayers
. The
292
increase of HSPC caused progressive broadening of the temperature peak width as
293
shown in the DSC thermogram, suggesting decreased co-operativity of the transition
294
by increased HSPC concentrations (48). The same results were shown in the studies of
295
Chen’s et al
296
is observed, but as the ratio increases, a shoulder appears, indicating phase
297
segregation. The DSC results suggest that the molar ratio of DPPC: HSPC=8:2 meets
298
the requirements of Tm of 42℃ in target tissue and was selected for further study. This
299
result was consistent with various formulations developed by other research groups.
300
For instance, liposomal formulations composed of DPPC/DSPC/DSPE-PEG2000 in a
301
molar ratio of 80:15:5 reported by Li et al. and of DPPC/DSPC/DPPGOG in a molar
302
ratio of 7:2:1 developed by Lindner et al., with similar DPPC/DSPC ratios, showed
303
the same Tm of 42℃ (49, 50).
304
Effect of Encapsulated β-ionone on Tm
(4)
. Moreover, at lower HSPC/DPPC ratios only a single-phase transition
305
Incorporation of β-ionone in liposomes affects the thermal properties of the
306
bilayers possibly due to some intercalation into the bilayers, adsorption on the surface
307
of liposomes, or interaction with the polar head groups of the PC and was studied by
308
DSC
309
liposomes and liposomes (DPPC: HSPC=8:2) with varying β-ionone/lipid ratios (1:40
310
to 1:1) were characterized by DSC. A symmetrical peak was only occured in the
311
absence of β-ionone with Tm of 43.48℃. Incorporation of β-ionone at even 5 mg
312
(β-ionone/lipid ratio of 1:40) lowered the Tm and broadened the main transition
. Thermograms (Fig. 2) and the Tm and T1/2 (Table 1) of blank
(46, 51-53)
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313
temperature peak, with the peak showing asymmetry towards the lower temperature
314
side. Increasing β-ionone content amplified the asymmetry with a shoulder appeared
315
at 1:4 β-ionone/lipid ratio. Further increases of β-ionone to 100-200 mg
316
(β-ionone/lipid ratio of 1:2-1:1) resulted in the Tm shift to 37.38℃ with a larger
317
shoulder spanning 29-42℃, suggesting a phase segregation occurred with the
318
formation of a new membrane species, these liposomes were no longer stable (54).
319
According to the researches of Ichioma Onyesom, the reduction of transition
320
temperature is associated with partial embedding of molecules into the bilayer of lipid
321
or penetration into the core area of liposomes (46). Additionally, Bermudez et al. has
322
reported that molecules interacting with either the polar headgroups, lipophilic
323
hydrocarbon chains or both parts of the lipid bilayer constituents would exert a
324
significant influence on their phase behavior
325
researches as well as our study results inferred that β-ionone has been encapsulated
326
into the liposomal membranes and the embedding of β-ionone would cause the Tm
327
reducing. Further studies about the relationship between loading amounts and
328
liposomal stability were investigated as follows.
329
Storage Stability of β-ionone Loaded Liposomes
(55)
. Information presented in above
330
The stability of shelf life of liposomal vesicles during storage at 4℃ was evaluated
331
by the changes of Z-average diameter (ΔDz) and retention rate (RR) over time. As
332
shown in Fig. 3A, the Z-average diameter of blank liposomes more than tripled to
333
282.9 nm after 80 days storage, with its PDI value changing from 0.155 to 0.298. This
334
tendency to aggregate during storage or manufacture is a thermodynamic property of 15 ACS Paragon Plus Environment
Journal of Agricultural and Food Chemistry
335
liposomes(17). However, this instability was strongly inhibited by β-ionone
336
incorporation. The increases of DZ after 80 days were only 28.48, 8.74, 7.31 and 20.41%
337
at the β-ionone/lipid ratios of 1:40, 1:20, 1:8 and 1:4 (Fig. 3B), with their original
338
particle size of 132.6±2.8, 158.7±3.4, 192.6±1.2 and 203.5±3.1 nm, and PDI values of
339
0.183±0.006, 0.109±0.025, 0.110±0.016 and 0.135±0.012, respectively. These results
340
showed that β-ionone suppressed aggregation on the whole, compared with unloaded
341
ones and in a concentration-dependent manner when the β-ionone/lipid ratio was
342
below 1:8. However, higher β-ionone loading would reduce the suppression properties,
343
which might be attributed to the excess amounts of β-ionone present in the aqueous
344
phase yielding to disruption of the bilayer, thus reduce the dispersion stability of
345
liposomes.
346
The loss of encapsulated β-ionone during storage is shown in Fig. 3C.
347
Liposomes with relatively higher β-ionone/lipid ratios of 1:20 and 1:8 had a retention
348
rate of about 60% after 80 days storage, while samples with high β-ionone/lipid ratio
349
of 1:4 had retention rates of 43%, only. High loss of β-ionone in 1:4 drug/lipid ratio
350
liposomal delivery system might be attributed to the heavier coalescence of liposomes
351
during storage (combining with the results of particle size), which would further
352
destabilize the liposomal bilayers and thus lead to more severe leakage of β-ionone.
353
The initial PC composition of empty and β-ionone loaded liposomes as well as
354
after storage at 38℃ was presented in Table 4. As seen in Table 4, the content of
355
HSPC and DPPC after 4 weeks storage reduced for approximately 6% for all the
356
liposomal samples, but conversely, the lysophospholipids (LPC) content among all 16 ACS Paragon Plus Environment
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Page 17 of 49
Journal of Agricultural and Food Chemistry
357
those formulations increased. This result was consistent with the previous reports that
358
the liposomal phospholipids could hydrolyze to LPC during storage, which would
359
destabilize the bilayer structures
360
liposomal formulation was negligible, which would not cause a significant damage to
361
the bilayer structure. In addition, the similar degradation rate of empty liposomes and
362
β-ionone loaded liposomes indicated that the incorporation of β-ionone would not
363
affect the bilayer decomposition.
(56)
. However, the generation of LPC in this
364
The morphology and vesicle shape of empty and β-ionone loaded liposomes were
365
observed by TEM. As presented in Fig. 4A and B, blank liposomes possessed high
366
tendency to aggregate compared with β-ionone loaded ones and the hydrophobic area
367
of β-ionone loaded liposomes were much larger than empty ones (marked with red
368
arrow, the light area surrounding the vesicles), indicating the incorporation of
369
β-ionone into liposomes. The vesicle size around 200 nm showed by TEM were
370
slightly larger than the results by DLS, which might due to the collapse of liposomal
371
vesicles during the progress of taking photos. The variations of vesicle size and shape
372
before and after storage for liposomes with different drug/lipid ratios were shown in
373
Fig. 4C. The size changes of empty and β-ionone loaded samples matched well with
374
the results of DLS presented in Fig. 3A and B, with empty liposomes doubled after
375
storage for about 30 d, while β-ionone loaded liposomes merely changed little.
376
Effect of β-ionone Incorporation on Membrane Fluidity
377
Fluorescence polarization and Raman spectra were utilized to investigate the
378
structural properties of the bilayer membranes when β-ionone was incorporated. The 17 ACS Paragon Plus Environment
Journal of Agricultural and Food Chemistry
379
microviscosity for DPH and TMA-DPH with β-ionone loading is shown in Fig. 5.
380
Low β-ionone/lipid ratios from 1:40 to 1:20 increased the microviscosity of the
381
membrane surrounding both probes indicating β-ionone enhanced membrane rigidity.
382
Further increases in β-ionone to 1:8 did not increase the microviscosity of DPH and
383
TMA-DPH remained constant implying that the hydrophobic interactions had reached
384
saturation. At high loading, with the drug/lipid ratio of 1:4, the hydrophobic core and
385
exterior surface region of the membrane had lower microviscosity or were more
386
highly fluid, compared with 1:20 or 1:8 ones. Over high β-ionone in the bilayer may
387
interfere with acyl chain and/or head group interactions and destabilize the bilayer.
388
The microviscosity measured by the ANS surface probe barely changed at low
389
loading (Fig. 5), suggesting that β-ionone is oriented in the deep regions of the lipid
390
bilayer when incorporated at low levels. The microviscosity for ANS increased with
391
the β-ionone/lipid ratio up to 1:8 followed by a slight decrease at higher concentration.
392
The microviscosity results suggest that β-ionone moves to the surface and may affect
393
the ionic interactions between the polar headgroups at higher β-ionone/lipid ratio
394
(above 1:8). The carbonyl group of the β-ionone molecule has a slight ionic character
395
and may interact with the polar head group of the phospholipid. The location of
396
β-ionone in liposomal bilayers interpreted by our data is shown in Fig. 6.
397
Fluorescence measurements demonstrated that liposomes with β-ionone/lipid
398
ratios of 1:20 or 1:8 are more stable because they had higher microviscosity and lower
399
membrane fluidity (lower ΔDz and higher RR) than other liposomes.
400
Effect of β-ionone Incorporation on the Order Parameters of Lipid Bilayer 18 ACS Paragon Plus Environment
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Journal of Agricultural and Food Chemistry
401
Raman spectroscopy has been widely used to determine structural changes at the
402
molecular level of liposomal hydrocarbon chains in membranes by drugs that change
403
molecular conformation and vibrational modes
404
corresponding to inter- and intra- molecular membrane order are shown in Fig. 7.
405
Changes in peak intensities in Raman scattering spectra relate to membrane order (58).
406
The characteristic peaks in Fig. 7A at 2847 and 2882 cm-1 show the symmetrical and
407
asymmetrical vibration of the methylene C-H stretching, respectively
408
calculated from the ratio of peak intensities, I2882/I2847, is associated with the changes
409
in both the lateral interaction between chains and the trans-gauche population ratio (59).
410
The changes of relative peak intensity and SL are shown in Table 3. The data shows
411
that the SL increased with increasing β-ionone/lipid ratio from 1:40 to 1:8 and
412
indicates that the lateral packing and inter-chain order between lipid molecules
413
increased. Nevertheless, SL decreased with further increases in β-ionone to 1:4 ratio.
414
These observations are consistent with the fluorescence microviscosity measurements
415
that β-ionone would incorporate into the membrane at high concentration.
(57)
. Spectra of wavelength range
(43)
. SL,
416
The bands at 1130 cm-1 are associated with the all-trans stretching vibrations of
417
the alkyl C-C bonds, while bands at 1086 cm-1 correspond to the gauche rotations of
418
hydrocarbon chains Fig. 7B. Some researchers found a positive correlation between
419
the longitudinal order and the number of all-trans bonds
420
from the ratio I1130/I1086 may be a sensitive measure of the order in the longitudinal
421
interaction between alkyl chains. The calculated results are in Table 4. The ratios
422
were similar at all β-ionone levels, which might due to the weak intensity of the peaks 19 ACS Paragon Plus Environment
(60)
. Therefore, ST derived
Journal of Agricultural and Food Chemistry
423
that hard to be calculated accurately to ST from the Raman spectra.
424
Release Behavior of β-ionone Loaded Liposomes
425
The release behavior of β-ionone loaded liposomes may be the most important
426
property as an anticancer delivery vehicle and was evaluated using an in vitro release
427
test at incubation temperatures of 25, 35, 42 and 50℃, using the liposomes with the
428
β-ionone/lipid ratio of 1:8. According to the results in Fig. 2 and Table 1, Tm of the
429
liposomes with β-ionone/lipid ratios of 1:20 and 1:8 were all around 42℃, one is of
430
42.32±0.35℃ and another is of 41.24±0.12℃. For the purpose to further clear the
431
differences between these two samples, their release behaviors were also investigated
432
in this study. As shown in Fig. 8A, very little β-ionone was released at 35℃, and
433
almost no release at 25℃. A large release of β-ionone occurs at 42℃, and increases at
434
50℃. Loading amount also affects release as shown in Fig. 8B. Liposomes with
435
β-ionone/lipid ratio of 1:8 were more stable than 1:20 at 42℃. The differences in the
436
release behavior might be attributed to lower Tm at 1:8 ratio, which would be further
437
studied in the following sections.
438
Effect of Heating Temperatures on Membrane Fluidity
439
In order to understand phase transition at the molecular level as a function of
440
temperature, the acyl chain vibration during in vitro release were investigated. The
441
temperature dependence of DPH fluorescence polarization for pure liposome and
442
liposomes with β-ionone/lipid ratios of 1:20 and 1:8 are presented in Fig. 9. The
443
fluorescence polarization of pure liposomes is constant until about 41℃ when there is
444
a sudden decrease at 41-45℃ and then remains constant at temperatures above 45℃. 20 ACS Paragon Plus Environment
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Page 21 of 49
Journal of Agricultural and Food Chemistry
445
Liposomes loaded with β-ionone showed similar polarization behavior, but the phase
446
transition temperature was reduced to 39-42℃. On the other hand, the microviscosity
447
of bilayer membranes in the gel state increased when the mole fraction of β-ionone
448
enhanced with the drug/lipid ratio changing from 1:20 to 1:8. The liquid crystalline
449
state decreased with β-ionone loading. The higher microviscosity lowers fluidity of
450
membranes and indicates that the packing density at β-ionone/lipid ratio of 1:8 was
451
lower in the liquid crystalline state, thus β-ionone would release more rapidly. This
452
phenomenon was used to account for the release behavior in previous studies.
453
Effects of Heating Temperatures on the Order Parameters of Lipid Bilayer
454
The order properties of lipid molecules transition from solid to the
455
liquid-crystalline phases were studied with increasing temperature. The phase
456
transition temperature can be measured by the peak height intensity ratio
457
ratio I2882/I2847 in the C-H stretching region and the ratio I1130/I1086 in the C-C
458
stretching region, respectively, as a function of temperature were monitored for
459
liposomes with β-ionone/lipid ratios of 1:20 and 1:8. (Fig. 10). The ratios I2882/I2847
460
and I1130/I1086 remained almost constant below 40℃, followed by an abrupt decline at
461
40-45℃, and remained constant again above 45℃. The phase transition of liposomes
462
with β-ionone/lipid ratio of 1:20 usually took place at 39-40℃ (Fig. 10B and 10D).
463
The incorporation of β-ionone at the drug/lipid ratio of 1:8 resulted in a lower initial
464
transition temperature from 41.43 to 40.50℃ (Fig. 10A) or 41℃ (Fig. 10C). These
465
transition temperatures are very close to the results derived from DSC. The peak ratio
466
at 1:8 β-ionone/lipid ratio was higher than that at 1:10 in the gel state and supports our 21 ACS Paragon Plus Environment
(61, 62)
. The
Journal of Agricultural and Food Chemistry
Page 22 of 49
(63)
467
other data. These ratios correspond to the disorder/order among the chains
. This
468
parameter is further verification that β-ionone increases the disorder in the liquid
469
crystalline state and explains why liposomes at β-ionone/lipid ratio of 1:8 possess
470
superior release properties than those at 1:20.
471
In summary, the release behavior and phase transition mechanisms upon heating
472
of β-ionone loaded thermosensitive liposomes (TSL) were studied in this research.
473
The phase transition temperature, Tm, of β-ionone loaded liposomes composed of
474
DPPC and HSPC was inversely related to the molar ratio of these two PCs and the
475
loading amount of β-ionone. β-ionone incorporation improved the storage stability of
476
liposomes, and those liposomes with β-ionone/lipid ratios of 1:20 and 1:8 were more
477
stable by decreasing membrane fluidity and increasing lateral inner-chain order. The
478
release of β-ionone occurred in the ideal range, 39-43℃. These findings suggest that
479
β-ionone loaded TSLs may be a potential useful delivery system for nutritional
480
supplement or chemopreventive agents.
481
Acknowledgments
482
This research was supported by the National Key R&D Program of China
483
(2016YFD0400801,2016YFD0400802), the National Natural Science Foundation of
484
China (No. 31571891,31401533), The research is also supported by program of
485
“Collaborative Innovation Center of Food Safety Quality Control in Jiangsu
486
Province”, China.
487
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Figure Captions Fig. 1 DSC thermograms of liposomes with different DPPC/HSPC ratios (a, pure DPPC; b, DPPC: HSPC=9:1; c, DPPC: HSPC=8:2; d, DPPC: HSPC=6:4; e, DPPC: HSPC=5:5; f, pure HSPC). Fig. 2 DSC thermograms of liposomes (DPPC/HSPC=8:2) at varying β-ionone/lipid ratios (a, 0; b, 1:40; c, 1:20; d, 1:8; e, 1:4; f, 1:2; g, 1:1). Fig. 3 Changes in z-average diameter (ΔDz/%) of (A) pure liposomes and (B) β-ionone encapsulated liposomes with different drug/lipid ratios during storage at 4℃ in the dark for 80 d; Changes in the (C) retention rate (RR) of β-ionone liposomes with different drug/lipid ratios during storage at 4℃ in the dark for 80 d. Fig. 4 TEM morphology of (A) empty and (B) β-ionone loaded liposomes with the drug/lipid ratio of 1:8 (magnification 10000× and 30000×); the TEM images of (C-1) empty liposomes (magnification 80000×), (C-2) liposomes with drug/lipid ratio of 1:20 (magnification 100000×) and (C-3) liposomes with drug/lipid ratio of 1:8 (magnification 60000×) before (left) and after (right) storage for 4 weeks. Fig. 5 Microviscosity (η) in liposomes for ANS, TMA-DPH and DPH as a function of β-ionone/lipid ratios from 0 to 1:4. Fig. 6 Schematic representation of the main patterns about the localization of β-ionone molecules in liposomal vesicles. Fig. 7 Raman spectra in the range from (A) 2800 to 3000 cm−1 and (B) from 1000 to 1200 cm−1 of pure liposomes and liposomes loading with different β-ionone/lipid
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ratios from 0 to 1:4. Fig. 8 The release curve of β-ionone loaded liposomes (A) at different incubation temperatures from 25 to 50℃; (B) with different β-ionone/lipid ratios of 1:20 and 1:8 at 42℃. Fig. 9 Relationship between fluorescence polarization of DPH and temperature for (A) pure liposomes and (B) liposomes with different β-ionone/lipid ratios of 1:20 and 1:8. Fig. 10 I2882/I2847 vs. temperature graph for liposomes at β-ionone/lipid ratios at (A) 1:8 and (B) 1:20; I1130/I1086 vs. temperature graph for liposomes at β-ionone/lipid ratios at (A) 1:8 and (B) 1:20.
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Table Captions Table.1 Tm and △T1/2 of liposomes with different β-ionone/lipid ratios. PC composition (mol/mol)
80%DPPC+20%HSPC
β-ionone/lipid Tm(℃)
△T1/2(℃)
0
43.48±0.20a
1.80±0.12a
1:40
42.33±0.13b
2.40±0.09a,b
1:20
42.32±0.35c
2.76±0.21b
1:8
41.24±0.12d
3.52±0.18c
1:4
40.07±0.86e
5.09±0.07d
1:2
38.57±0.08e
5.60±0.92d
1:1
37.20±0.08f
7.28±0.30e
ratios (wt/wt)
Data are presented mean ±SD, n = 3. Different letters in the same row indicate significant difference (P < 0.05, Duncan analysis)
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Table.2 Phospholipid composition of liposome dispersions with different β-ionone/lipid ratios during storage. β-ionone/lipid ratios (wt/wt)
0
1:20
1:8
Peak Area
Storage time at 38℃ (d)
PC
LPC
0
1208
110
14
1194
122
28
1180
134
0
1232
117
14
1196
139
28
1148
168
0
1286
84
14
1247
123
28
1232
137
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Table.3 Order parameters of pure liposomes and liposomes with different β-ionone/lipid ratios and variations percent as deduced from Raman spectra in the range between 1000 to 1200 cm−1. β-ionone/lipid ICH2(I2882/ I2847)
SL
(SL-SL.0)/SL.0
0
1.0675
0.245
-
1:40
1.0852
0.2568
4.82%
1:20
1.0941
0.2627
7.24%
1:8
1.1396
0.2931
19.63%
1:4
1.0836
0.2557
4.38%
ratios (wt/wt)
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Table.4 Order parameters of pure liposomes and liposomes with different β-ionone/lipid ratios and variations percent as deduced from Raman spectra in the range between 2800 to 3000 cm−1. β-ionone/lipid IC-C(I1130/ I1086)
ST
(ST-ST.0)/ST.0
0
0.9374
0.5296
-
1:40
0.918
0.5186
-2.07%
1:20
0.9594
0.542
2.35%
1:8
0.9751
0.5509
4.02%
1:4
0.9681
0.5469
3.28%
ratios (wt/wt)
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Figure graphics
Fig. 1
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Fig. 2
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Fig. 6
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Fig. 8
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Fig. 9
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Fig. 10
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Graphic Abstract
Thermosensitive liposomes was fabricated to rapidly release the bioactive molecule β-ionone at certain temperature of 42℃
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