Open Access Article
Yufang
Wang
a,
Jianzhu
Wang
a,
Mingshuang
Sun
a,
Jiyan
Zhang
b and
Yanping
Bi
*a
aSchool of Pharmaceutical Sciences, Shandong First Medical University, China. E-mail: biyanpingtsmc@163.com
bTai An TSCM Hospital, China
First published on 6th January 2022
Escaping from the immune system to achieve a long circulation time is an essential prerequisite for targeting liposomes. Monomethoxy-poly(ethylene glycol)–distearoylphosphatidylethanolamine (mPEG–DSPE) is the most commonly used stealth polymer for long circulating liposomes. With its monomethoxy end moving freely on the liposomal surface, the linear PEG chains of mPEG–DSPE construct a hydration layer to repel complement proteins and thus evade immune clearance. We describe in this work a new kind of PEG derivative whose two ends were grafted with cholesterol (cholesterol–PEG–cholesterol, CPC). According to the in vitro and in vivo results, the presence of CPC in liposomes was shown to reduce the uptake by phagocyte cells while extending the circulation time. The stealth performance of CPC liposomes is closely related to the molecular weight of PEG moieties. CPC6k performed better than CPC2k, CPC4k and the commonly used mPEG2k–DSPE. CPC on the liposomal surface would not let the free end of PEG act as the immune recognition site, meanwhile, the PEG chain of CPC tends to adopt a twisted ring-like conformation rather than a linear conformation, which is considered to be associated with the stealth effect. This finding adds to the range of stealth liposomes and may be valuable for developing new drug carriers.
PEG chains repel proteins due to their high hydrophilicity and flexibility, so an intact PEG hydration layer with enough thickness on the nanoparticle surface is essential for preventing the adsorption of plasma proteins. The length (molecular weight, MW), density and conformation of PEG chains, which correlate with each other on the nanoparticle surface, strongly affect the circulation time of nanoparticles. A reasonably higher MW of PEG chains leads to a thicker hydration layer on the nanoparticle surface and thus a lower level of opsonization.2,8,9 A low ratio of surface coverage may bring about the interaction between the proteins and exposed surface.
The PEG chains on the particle surface could show a “mushroom” or “brush” conformation depending on their grafting density. In order to achieve a better stealth-like behavior, the PEG conformation needs to be optimized between the “mushroom” and “brush” because the over-high coverage ratio and density, which result in a “brush” conformation, may reduce the flexibility of PEG chains.1,2 In addition, there is easily overlooked relevance between the end-group of PEG chains and MPS uptake. Compared with hydroxyl- or mannoside-terminated PEG, methoxy-terminated PEG can protect nanocarriers from MPS recognition more effectively,10 which implies that the end group of PEG is an important recognition site for MPS clearance.
PEGylated liposomes have been widely used as a kind of long circulating nanocarrier for drug targeting especially after the approval of Doxil® by the FDA. It is necessary for a PEG chain to anchor at least one of its two ends onto the surface of liposomes, so that a stable hydration layer can be preserved. In previous reports, the other end of the PEG, usually capped with a methoxy group or a targeting ligand, can move freely within the hydration layer. For example, monomethoxy-poly(ethylene glycol)–distearoylphosphatidylethanolamine (mPEG–DSPE), the most commonly used stealth polymer for stealth liposomes,11 could be fastened to a liposome by inserting its distearoyl group into a phospholipid bilayer. As compared to its homologues, PEG2k–DSPE attracts more attention due to its low toxicity and stabilization effect on liposomes.12–14 The superiorities of the PEG2k–DSPE unit in fabricating stealth liposomes are rooted in its suitable hydrophile–lipophile balance (HLB) value which is decided by the MW ratio of PEG to DSPE. That is to say, extending the PEG chain might not bring about a better stealth effect but cause unpredictable toxicity or self-assembly of mPEG–DSPE.
If the other end of mPEG–DSPE was also grafted with a lipophilic group, the MW of the PEG chain could be doubled with the HLB value remaining unchanged. From a thermodynamics perspective, both ends of the lipophilic groups tend to insert into a liposomal membrane to construct a ring-like PEG chain (Fig. 1). The unique ring-like conformation of the PEG chain would endow liposomes with improved properties. Cholesterol can be a suitable alternative to anchoring into liposomal membranes,15 so in this work, cholesterol molecules were attached to both ends of PEG to obtain cholesterol–PEG–cholesterol (CPC). Subsequently, CPC-containing liposomes were prepared and their physicochemical properties, cellular uptake and pharmacokinetic behaviors were also studied.
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| Fig. 1 Schematic representation of linear (left) and ring-like (right) conformations of PEG moieties on the liposomal surface. | ||
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1.5
:
0.1, v/v/v).
In the second step, PEG diacids (2 mmol), cholesterol (8 mmol), DMAP (1.955 g) and DCC (3.3 g) were dissolved into 60 mL of anhydrous dichloromethane. The mixture was stirred under nitrogen at room temperature for 24 h and then filtered. The filtrate was washed with 0.1 M HCl, 1% aqueous ammonia and distilled water in turn until pH = 7, then was dehydrated using anhydrous sodium sulfate for 24 h and re-precipitated using petroleum ether to obtain CPC. The detailed synthetic scheme is illustrated in Fig. 2.
Fourier transform infrared (FT-IR) spectra of CPC samples were recorded using a Shimadzu IRAffinity-1 spectrometer at frequencies ranging from 400 to 4000 cm−1 with a 4 cm−1 resolution. Typically, 1 mg of each sample was mixed with 20 mg KBr and compressed into tablets before determination. 1H and13C nuclear magnetic resonance (NMR) spectra of samples in DMSO-d6 were recorded on a Bruker Avance NEO400 at frequencies of 400 MHz at 298 K.
:
1) before 1000 μL of Cou-6 solution (100 μg mL−1) in dichloromethane was added. The organic solvent was removed in a rotary evaporator to yield a thin lipid film. Then the film was hydrated with 10 mL of physiological saline and treated with a high pressure homogenizer at 10
000–15
000 psi for 5 min.
The size, polydispersity index (PDI) and zeta potential of liposomes were analyzed with a Malvern Zetasizer Nano ZSE. For each test, 100 μL of liposomal suspension was mixed with 1.000 mL of ultrapure water at 25 °C. A JEM-1200 EX II transmission electron microscope (TEM, JEOL Ltd.) was used to observe the morphology of liposomes. Before observation, about 5 μL of diluted liposomal suspension was dripped onto a carbon-film-coated copper grid and dried in a vacuum, and then stained with 2.0% (w/w) phosphotungstic acid solution for 2 min.
000 rpm for 10 min before loading into the HPLC system.
The concentration of Cou-6 was calculated using a standard curve. In the range of 0.08–16 ng mL−1, the concentration of Cou-6 (Y, ng mL−1) correlated well with its peak area (X): Y = 1.3469X + 0.0358 (R2 = 0.9999). Three samples of Cou-6 at concentrations of 0.4, 4.0 and 8.0 ng mL−1 were selected for methodology validation. The recovery of this method ranges from 97% to 105% and the relative standard deviation (RSD) is smaller than 2% for 48 h.
Before acetonitrile pretreatment and HPLC analysis (see 2.4), the samples of liposomes were centrifuged at 3000 rpm for 5 min and diluted with ultrapure water 1000 times.
In order to investigate the leakage of Cou-6 in cell culture media, the dialysis test was conducted at 37 °C in a horizontal diffusion cell. The donor and receptor compartments were separated by a dialysis membrane (3.5 kD) and filled with 2.0 mL of liposomes and 7.0 mL of culture media, respectively. After magnetic stirring (100 rpm) for 24 h, 100 μL of the culture media was withdrawn and mixed with 400 μL of acetonitrile for HPLC determination. The leakage rate was calculated by the following equation:
C stretching vibrations of the cholesterol moiety at 1655 cm−1 appeared in the FT-IR spectra of CPC2k, CPC4k and CPC6k (Fig. 3). In the 1H-NMR spectra (Fig. 4) of CPCs, the characteristic peaks of the cholesterol moiety appeared at 5.34 ppm (C
C) and 0.5–2.1 ppm (CH3– and –CH2–), while the methylene groups of the SA moiety were found at 2.54 ppm. In the 13C-NMR spectra (Fig. 5), signals of the two carbonyl groups of succinic acid moieties were observed at 172.49 and 171.67 ppm while signals of the unsaturated carbons of cholesterol moieties were observed at 139.95 and 122.35 ppm.
| Number | Formulation | Hydrodynamic size (nm) | PDI | Zeta potential (mV) | Drug loading (%, w/w) |
|---|---|---|---|---|---|
| 20 mg of lecithin and 100 μg of Cou-6 were used within a total volume of 10 mL for F1–F4; 100 mg of lecithin and 100 μg of Cou-6 were used within a total volume of 10 mL for F5–F8. | |||||
| F1 | Cholesterol, 2.5 mg | 97.17 ± 1.39 | 0.180 ± 0.011 | −18.17 ± 1.92 | 85.93 |
| F2 | mPEG2k–DSPE, 4.00 mg (1.426 μmol) | 92.44 ± 2.35 | 0.244 ± 0.008 | −13.06 ± 1.41 | 86.78 |
| F3 | CPC2k, 4.24 mg of (1.426 μmol) | 120.23 ± 5.07 | 0.178 ± 0.024 | −14.50 ± 0.81 | 89.76 |
| F4 | CPC4k, 7.09 mg (1.426 μmol) | 121.36 ± 3.57 | 0.140 ± 0.008 | −13.80 ± 0.98 | 88.31 |
| F5 | CPC6k, 9.94 mg (1.426 μmol) | 135.30 ± 4.69 | 0.222 ± 0.008 | −16.23 ± 1.75 | 86.68 |
| F6 | mPEG2k–DSPE, 10 mg | 75.10± 1.25 | 0.262 ± 0.007 | −13.63 ± 0.45 | 87.76 |
| F7 | CPC2k, 10 mg | 130.80 ± 4.32 | 0.525 ± 0.118 | −13.80 ± 0.98 | 84.07 |
| F8 | CPC4k, 10 mg | 116.00 ± 4.06 | 0.457 ± 0.036 | −15.23 ± 0.37 | 87.41 |
| F9 | CPC6k, 10 mg | 91.75 ± 3.283 | 0.238 ± 0.013 | −15.70 ± 3.50 | 90.60 |
Naked liposomes, which were prepared without CPC, possessed a zeta potential of −18.17 mV while CPC liposomes, as well as mPEG2k–DSPE, displayed only a slightly lower value. This kind of minor variation in charge density may result from the addition of non-ionic polymers of CPC. However, the variation of PEG moieties in weight or MW did not induce the change in the zeta potential of liposomes.
From a thermodynamics perspective, both cholesterol moieties in a CPC molecule tend to anchor into the lipid bilayer so that the Gibbs energy of the whole system is minimized. If so, PEG chains would present a ring-shaped, specifically speaking, twisted-ring-shaped rather than linear conformation (Fig. 1). A double shell structure, which might be attributed to the lipid membrane and PEG layer, respectively, can be seen in CPC6k liposomes but not in other kinds of liposomes (Fig. 6). Under a given resolution of TEM, it is possible that the PEG layer could not be observed unless it is thick enough. Unfortunately, neither the TEM image nor any other widely used spectrum method is adequate to directly differentiate the ring-like conformation from that of linear type.
With Cou-6 as the fluorescent probe, different kinds of liposomes (F1–F5 in Table 1) were investigated for cellar uptake and the results are presented in the form of fluorescence intensity of cells in Fig. 7. Compared with the naked liposome (F1), the mPEG2k–DSPE liposome did not show significant difference in cellular uptake until 12 h passed, while CPC liposomes demonstrated a lower cellular uptake than naked liposomes at 1 h (p < 0.05) and extremely significant differences at 4 h and 12 h (p < 0.01). The degree to which CPC liposomes evade cellular uptake relied on the MW of the PEG moiety. Under the given molar amount of CPC, the cellular uptake efficiency of CPC liposomes was negatively correlated with the MW of PEG moiety at 12 h, which is consistent with previous reports on mPEG derivatives.1,5,16 An increase in size usually enhances the cellular uptake. However, the CPC6k liposome, even with a larger size than that of mPEG2k–DSPE, performed better in evading cellular uptake, which implied its superior surface properties for long circulation.
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| Fig. 7 Mean fluorescence intensity of different kinds of liposomes in RAW264.7 cells. Comparison was made with the mPEG2k–DSPE group (*p < 0.05; **p < 0.01; ***p < 0.001). | ||
| mPEG2k–DSPE liposome (F6) | CPC2k liposome (F7) | CPC4k liposome (F8) | CPC6k liposome (F9) | |
|---|---|---|---|---|
| *Represents the comparison with mPEG2k–DSPE liposomes. *p < 0.05; **p < 0.01; ***p < 0.001. | ||||
| T 1/2 (h) | 2.112 ± 0.8173 | 1.770 ± 0.6300 | 1.728 ± 0.4969 | 2.799 ± 0.3772 |
| AUC (ng L−1 h−1) | 11244 ± 1860 | 8657 ± 2792 | 15622 ± 7871 | 36563 ± 22284* |
| MRT (0-t) | 0.8992 ± 0.1006 | 1.317 ± 0.2098** | 1.577 ± 0.2700*** | 1.789 ± 0.3630** |
| CL | 3.125 ± 0.6687 | 4.267 ± 1.478 | 2.562 ± 1.126 | 0.9878 ± 0.4452*** |
| V | 9.006 ± 1.009 | 11.31 ± 6.402 | 6.232 ± 3.541 | 4.050 ± 1.874** |
It is the repetitive units of oxyethylene that endowed PEG chains with hydrophilicity and the resulting stealth capability, which would undoubtedly remain even when the PEG chains were folded into rings. Considering the end group of the PEG chain being the recognition site of MPS uptake, the possible mechanism by which CPC takes effect lies not only in the twisted ring-like conformation but also in the both hidden ends of the PEG chain. CPC could provide a new alternative for stealth liposomes to be drug carriers or imaging agents.
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