PARK SUNGWAN (US)
KIM SEYOUNG (US)
FESENMEIER DANIEL JAMES (US)
PRF Ref. No.69925-02/SLW 1165.135WO1 What is claimed is: 1. A composition comprising: dried amphiphilic block copolymer micelles having a mean hydrodynamic diameter in the range of about 5 nm to 1,000 nm in the original hydrated state, wherein the original micelle structure in an aqueous medium is preserved without aggregation or transformation during the drying process, wherein the drying is done substantially without using any excipients, wherein the original aqueous amphiphilic block copolymer micelle solution is prepared by initially forming amphiphilic block copolymer micelles in a medium containing an organic cosolvent and subsequently dialyzing the micelle solution against an aqueous reservoir. 2. The composition of claim 1, wherein the amphiphilic block copolymer comprises a hydrophobic block comprising a monomer selected from the group consisting of lactic acid or lactide (LA), glycolic acid or glycolide (GA), caprolactone (CL), styrene (S), methacrylate (MA), acrylate (Ac), butadiene (BD), and isoprene (IP), and a hydrophilic block comprising a monomer selected from the group consisting of ethylene glycol (EG), ethylene oxide (EO), vinyl alcohol (VA), oxazoline (OZ), and acrylamide (AM). 3. The composition of claim 1, wherein the amphiphilic block copolymer comprises a hydrophobic block comprising a styrene (S) monomer unit and a hydrophilic block comprising an ethylene glycol (EG) or ethylene oxide (EO) monomer unit. 4. The composition of claim 1, wherein the amphiphilic block copolymer comprises a poly(styrene) (PS) block having a number-average molecular weight in the range of 0.5 – 500 kDa and a poly(ethylene glycol) (PEG) block having a number-average molecular weight in the range of 0.5 – 500 kDa. 5. The composition of claim 1, wherein the corona-forming hydrophilic block of the amphiphilic block copolymer has a hydrophilic end group. 6. The composition of claim 1, wherein the end group of the hydrophilic block of the amphiphilic block copolymer is a hydroxyl group. 7. The composition of claim 1, wherein the micelles have a high dimensionless corona chain grafting density ıcorona^^ZKHUHLQ^ıcorona is defined as the projected area PRF Ref. No.69925-02/SLW 1165.135WO1 of the hydrophilic block segment in its unperturbed state divided by the micelle core surface area per hydrophilic segment. 8. The composition of claim 7, wherein the ıcorona is about 5 or greater. 9. A kit comprising the composition of claim 1 in a first container. 10. The kit of claim 9, wherein the kit further comprises an aqueous liquid in a second container. 11. A method of treating a pulmonary disorder in a subject, the method comprising administering to said mammal a therapeutically effective amount of the composition of claim 1 in the dried state or after reconstitution in an aqueous medium. 12. The method of claim 11, wherein the pulmonary disorder is caused by deficiency and/or deactivation of endogenous lung surfactant in the subject. 13. The method of claim 11, wherein the subject is a mammal. 14. The method of claim 11, wherein the subject is a human. 15. A method comprising: (a) dissolving an amphiphilic block copolymer in a mixed water-organic cosolvent mixture; (b) conducting a single-step dialysis against an aqueous reservoir to form a kinetically frozen monodisperse micelle polymer lung surfactant system in an aqueous solution; and (c) drying the aqueous polymer lung surfactant micelle solution to produce dried polymer lung surfactant micelles; wherein the aqueous polymer lung surfactant solution comprises substantially no excipients before the drying process. 16. The method of claim 15, wherein the amphiphilic block copolymer comprises a hydrophobic block comprising a monomer selected from the group consisting of lactic acid or lactide (LA), glycolic acid or glycolide (GA), caprolactone (CL), styrene (S), methacrylate (MA), acrylate (Ac), butadiene (BD), and isoprene (IP), PRF Ref. No.69925-02/SLW 1165.135WO1 and a hydrophilic block comprising a monomer selected from the group consisting of ethylene glycol (EG), ethylene oxide (EO), vinyl alcohol (VA), oxazoline (OZ), and acrylamide (AM). 17. The method of claim 15, wherein the amphiphilic block copolymer comprises a hydrophobic block comparing a styrene (S) monomer unit and a hydrophilic block comprising an ethylene glycol (EG) or ethylene oxide (EO) monomer unit. 18. The method of claim 15, wherein the amphiphilic block copolymer comprises a PS block having a number-average molecular weight in the range of 0.5 – 500 kDa and a PEG block having a number-average molecular weight in the range of 0.5 – 500 kDa. 19. The method of claim 15, wherein the corona-forming hydrophilic block of the amphiphilic block copolymer has a hydrophilic end group. 20. The method of claim 15, wherein the end group of the hydrophilic block of the amphiphilic block copolymer is a hydroxyl group. 21. The method of claim 15, wherein the step of dissolving comprises: (a) dissolving block copolymers in a water-organic cosolvent mixture at an initial water composition between about 10 and 90% (v/v); and (b) sonicating or mechanically agitating or heating the solution; (c) keeping the solution quiescently or under mild stirring for at least about ten minutes for equilibration. 22. The method of claim 15, wherein the step of single-step dialysis comprises: (a) dialyzing the solution using a dialysis bag against an aqueous reservoir for at least about ten minutes; and (b) replacing the aqueous reservoir with a fresh aqueous medium at least once during the dialysis period. 23. The method of claim 15, wherein the drying process comprises: (a) freezing the aqueous polymer lung surfactant micelle solution; (b) sublimating crystalized water from the polymer lung surfactant micelle solution until no further water sublimation is detected; and PRF Ref. No.69925-02/SLW 1165.135WO1 (c) desorbing and vaporizing the supercooled water adsorbed to the polymer lung surfactant nanoparticles (micelles). 24. The method of claim 23, wherein the freezing rate is about -2°C/min. 25. The method of claim 23, wherein the rate of temperature increase between the freezing and the primary drying steps is about 1°C/min. 26. The method of claim 23, wherein the rate of temperature increase between the primary drying and the secondary drying steps is about 1°C/min. 27. The method of claim 23, wherein the dried polymer lung surfactant micelles can be used as a therapy in dry powder form to treat acute respiratory distress syndrome, acute lung injury or neonatal respiratory distress syndrome. 28. The method of claim 23, wherein the dried polymer lung surfactant micelles can be used as a therapy after reconstitution in an aqueous medium to treat acute respiratory distress syndrome, acute lung injury or neonatal respiratory distress syndrome. 29. A method of reconstituting dried polymer lung surfactant micelles, the method comprising: (a) dissolving the dried polymer lung surfactant micelles of claim 1 in an aqueous medium; and (b) shaking or vortexing or mechanically agitating or sonicating the dissolved polymer lung surfactant micelles. |
PRF Ref. No.69925-02/SLW 1165.135WO1 [0051] wherein m (the degree of polymerization of the hydrophilic PEG block) is an integer in the range between about 11 and 11,000 and n (the degree of polymerization of the hydrophobic block) is an integer in the range between about 5 and 5,000. For example, each n can, independently, be an integer from about 5 to about 5,000. Alternatively, or in addition, each m is, independently, an integer from about 11 to about 11,000. For example, m can be from about 11 to about 2,200. In another example, n can be from about 5 to about 1,000. For example, m can be from about 11 to about 2,200. In another example, n can be from about 5 to about 1,000. For example, m can be from about 11 to about 5,500. In another example, n can be from about 5 to about 2,500. PLS Formulation and Characterization [0052] Block copolymer micelles with differing chemistry and sizes were prepared via a two-step solvent exchange technique termed as equilibrium nanoprecipitation (ENP) method. Each polymer (50 mg) was dissolved in a 5-mL mixture of acetone and Milli-Q water at varying solvent compositions (namely, the volume fraction of water, ij w,ENP), and each solution was sonicated for complete homogenization and subsequently equilibrated at ambient temperature for 24 hours. During the equilibration, block copolymers self-assemble into spherical micelles close to equilibrium whose size generally grows with ij w,ENP probably owing to a greater selectivity of the solvent quality. To completely remove the acetone from the PRF Ref. No.69925-02/SLW 1165.135WO1 solution after the equilibration, the solution was transferred to a dialysis bag (Spectra/Por 7, 50 kDa molecular weight cutoff) in 1 L of water reservoir, and the dialysate was changed three times with fresh water over 48 hours. The final concentration of the aqueous micelle dispersion was adjusted to 5 mg/mL by adding fresh Milli-Q water. [0053] Micelles formulated by the ENP method were characterized by transmission electron microscopy (TEM) using a 200-kV Tecnai T20 instrument. Diluted suspensions in Milli-Q water (0.1 mg/mL) were negatively stained by mixing in 1:1 ratio (v/v) with 1% aqueous uranyl acetate and then dried on a carbon-coated grid which was pre-treated by a glow discharge. The average diameter of micelles measured from the TEM images were regarded as the apparent core diameter (Dc), from which a non-dimensional grafting density of PEG (VPEG = pRg,PEG 2 /Dc 2 ), defined as the ratio of the cross-section area of a PEG chain (ʌR g,PEG 2 ) to the interfacial area per chain in the micelle (ʌD c 2 /p), was calculated. R g,PEG is the radius of gyration of an unperturbed PEG chain in water and is a function of weight- averaged PEG molecular weight. The term p = (ʌD c 3 /6)(M n,core /N A ^ core ) –1 is the aggregation number (where Mn,core is the number-averaged molecular weight of the hydrophobic core block), NA the Avogadro number, and ^core the density of the core block. [0054] The hydrodynamic size (Dh) distribution, the z-average hydrodynamic size (<Dh>), and the polydispersity index (PDI) of micelle formulations before (“pristine”) and after the lyophilization-and-reconstitution process (“reconstituted”) were measured by dynamic light scattering (DLS) using a Brookhaven NanoBrook 90Plus instrument. The nanoparticle solution was diluted to 0.5 mg/mL in Milli-Q water and filtered using a poly(tetrafluoroethylene) (PTFE) syringe filter (pores of ^^^^^^P^^^7KH^'/6^PHDVXUHPHQW^ZDV^SHUIRUPHG^DW^D^VFDWWHULQJ^ DQJOH^RI^^^^^DQG^ a laser wavelength of 640 nm. The micelle characteristics are summarized in Table 2.
) d A 6 3 7 1 9 0 5 4 3 8 S . 0 2 . 0 8 . 0 8 . 0 0 . 0 3 . 0 2 4 5 3 . ~ 0 1 . ) 0 1 . 0 1 . 0 4 . c 0 . y i ) t c sn F 9 8 0 6 8 1 2 5 6 6 9 4 e . I S 7 . 2 4 . 4 9 . 1 9 . 1 6 . 5 1 . 5 . 1 . 8 . 8 . 9 . 8 . d y t g i l i r 6 5 1 4 5 3 1 e i n b t f t f a l i a n a r av d o i e t g t a 8 8 G a e u t z I i 5 4 15 66 14 19 07 12 98 88 33 2 E c t i l i D 1 1 . 1 . 1 . 1 . 1 0 1 1 1 1 1 2 a s h P 0 0 0 0 . 0 . 0 . 0 . 0 . 0 . 0 . 0 . P f r n p 0 o d u o y e zi S c L l ) e ad R ) n . i s h m 6 . 1 7 . 3 1 2 . 9 7 . 9 1 . 2 6 . 9 . 5 . 5 . 9 . 6 . 2 . o s e l l n e D n ( 0 8 3 5 2 9 8 e i c 1 31 5 6 51 61 51 91 51 51 01 61 i m d m n e o n i t ) Ns b i r . p d o o t I h s 0 0 2 D 0 2 8 21 77 89 92 09 81 41 28 48 t e e l l P 3 . 2 . 0 . 1 . 1 . 0 . 0 . 1 . 2 . 1 . 0 . 2 e 0 0 0 0 0 0 0 0 0 0 . m 0 0 ) i c P m Nd 2 E e t e l ) ( n u t ba mn 1 . 7 4 . 9 2 . 1 6 . 5 8 . 6 3 . 6 8 . 8 1 . 8 0 . 1 . 5 . 2 . o i i t t sn T (h 4 2 3 3 2 2 2 6 2 6 7 1 a o 1 3 2 2 9 i t i c e D p n c e r i t e r f s i r ) p o o o P b n i t G E 1 . 0 . 2 . 0 3 . 1 0 . 8 9 . 9 2 . 0 5 . 0 8 . 7 3 . 8 4 . 9 1 . a a 7 9 1 n r r V P 1 1 1 1 1 m e t u i e ) r b m i a 7 m i l i d 1 n ( 3 0 3 3 8 u c . 3 . D 1 7 . . . 4 . 9 . 5 . 5 . 4 . 9 . 3 . q i c 1 91 12 41 81 81 91 61 71 91 32 e e m h a )a t n P n y N i d E , w 2 . 0 3 . 0 5 . 0 6 . 0 1 . 0 2 . 0 3 . 0 5 . 0 1 . 0 2 . 0 3 . 0 5 . d o 0 e r d s y ij u r h e t , . a e . i w f , r o o t c 3 n a H - o i t f g H C G c i n O O E a r s r - - e P f a G G - e e r m E E A 3 mc l y P - P - M H l u n i o S S B t C o e P P P P O ) V a i z S PRF Ref. No.69925-02/SLW 1165.135WO1 Lyophilization and Reconstitution [0055] Each micelle formulation (2 mL) was transferred into a 10-mL lyophilization vial equipped with a rubber stopper. A total of 12 vials (3 polymers × 4 ENP conditions) were placed together in the chamber of a small-batch lyophilizer (MicroFD, Millrock Tech) with programmable thermal trajectories. The lyophilization process followed a typical sequence; the solutions were rapidly cooled from 25°C to the target shelf temperature (T shelf ) and then allowed to equilibrate for 3 h (the freezing stage). Subsequently, the frozen water (ice) was sublimated at a T shelf below the “collapse” temperature of the PEG/water system (– 18°C) until the chamber vapor pressure (P) reached the target pressure of 70 mTorr (the primary drying stage). Finally, the bound water was dried at a Tshelf above the triple point of water (0.01°C) until the target pressure of P = 70 mTorr was achieved again (the secondary drying stage). Two different operating methods with distinct ramping rates and target Tshelf values were utilized, and the specific operational parameters can be found in Table 3. Throughout the lyophilization process, Tshelf, P, and the heat flux between the vials and the shelf were continuously monitored in real-time. In reconstitution, 2 mL of Milli-Q water was added to each vial containing lyophilized samples, followed by gentle shaking for 3 min and sonication for 3 min.
) c 5 9 0 r F I . 4 . e S 1 2 t f a no d i e t t a u t z i I D 8 i t l i P 1 . 7 0 1 . 0 s h n p o o c y e L R >h ) Dm 5 . 9 3 . 2 < n ( 6 8 g n i f l ) b e y h r s ) C 52 52 D T ° ( y e r g ad a t n S ) n i oc R m ) 1 1 e / a C + + S ° ( g f l ) b e n i hs ) 0 C 3 53 y T ° ( – – 3 r e l D eg ba y r a t T a S ) . m n r i o t i r R m ) a 2 1 ca P / C + + f ° ( g i n sa e r c ) n f l b i e e g hs ) 06 0 e 5 i z a t T C ° S ( – – ) S c 9 . 11 g e n i r O z ) u t W e n i a r 53 e r R m ) a 2 1 ep 1 . F / – – C 56 ° m ( e t 1 l f 1 e W n ) h S L o L S / i ) t m b . 2 a l ( e 8 2 e t 0 - u 3 1 a 52 m r m r g 9 o u l n F o 9 i t 6 V a . e o h N r . f o d g e n R o i h l o F t e A B o R M ) C P a PRF Ref. No.69925-02/SLW 1165.135WO1 Dynamic Light Scattering (DLS) [0056] An aqueous BCP micelle solution (0.5 mL of a 5 mg/mL) was diluted by adding 2.5 mL of Milli-Q-purified water. The diluted solution was filtered using a poly(tetrafluoroethylene) (PTFE) filter with 0.45 µm pore size twice to remove dusts, bubbles, etc. The filtrate was transferred to a polystyrene disposable cuvette for DLS measurement. The mean hydrodynamic diameter, polydispersity, and zeta potential of the BCP micelles were determined by DLS using a NanoBrook ZetaPALS instrument (Brookhaven, illumination with a 659 nm laser, detection at 90° scattering angle). Transmission Electron Microscopy (TEM) [0057] A TEM specimen was prepared as follows. For negative staining, 5 PL of a 1 mg/mL aqueous BCP micelle solution was mixed with 5 PL of a 1% aqueous uranyl acetate solution. The mixed solution was placed on a carbon-coated copper TEM grid (treated with O 2 plasma to make the surface hydrophilic). After 30 seconds, the solution was blotted using filter paper and dried. The resulting specimen was imaged using a 200-kV Tecnai T20 TEM instrument. The TEM images were analyzed using Gatan DigitalMicrograph software. Surface Pressure–Area Isotherms (Surface Mechanical Analysis) [0058] The surface pressure–area (Ȇ–A) isotherms of the micelle monolayers were measured using a Langmuir trough (KSV 5000, Biolin scientific) with two symmetric barriers attached at each end. The trough and two barriers were initially cleaned with ethanol and water three times. Water (1.4 L of Milli-Q purified water) was poured in the trough, and filter paper was used as a Wilhelmy plate to measure the surface tension. Before each measurement, the water surface was aspirated to remove any interfacial contaminants so that the surface pressure of pure water at the maximum compression (A = 71 cm 2 ) did not exceed 0.2 mN/m. [0059] Onto the clean surface of water at the maximum area (782 cm 2 ), 100 µL of the “pristine” or “reconstituted” micelle solution (5 mg/mL) was spread using a microsyringe. Droplets of a few microliter was formed on a tip of the syringe needle and carefully contacted on the water surface to spread the sample on the water. For the Ȇ–A isotherm measurements of the PLS with added excipients, excipients were added to the pristine solutions to reach a 10% w/v excipient concentration before the spreading. For the Ȇ–A isotherms of the solid lyophilizates, 1.5 mg of the foamy solid was carefully placed piecewise on the clean water surface using a dressing forcep. Differential Scanning Calorimetry PRF Ref. No.69925-02/SLW 1165.135WO1 [0060] Freezing and melting of the micelle formulations were analyzed using differential scanning calorimetry (DSC; DSC 4000, Perkin Elmer). The micelle concentration of ~100 mg/mL (i.e., ~20 times higher than the concentration of standard formulations) was used to precisely evaluate the amount of bound water to the PEG brushes. To increase the concentration, each of pristine micelle formulation (0.5 mL, 5 mg/mL) was placed in a pre-rinsed centrifugal dialysis membrane tube (Amicon Ultra–0.5, MWCO 10 kDa) and centrifuged at 14,000 rpm for 20 min. The micelle concentration post centrifugation was measured using GPC by taking an aliquot of the concentrated micelle suspension. The GPC intensity peak area was converted to the concentration based on a calibrated data (a standard solution of predetermined polymer concentration). The actual concentrations of micelle suspensions used in DSC are reported in Table 4. [0061] A concentrated solution (8 PL) was transferred to a hermetic DSC pan and tightly sealed. A DSC cycle of cooling from 30°C to –50°C and reverse heating back to 30°C was performed with a ramp rate of 5°C/min. The mass of eutectic PEG (m PEG,eu ) was calculated from the measured endothermic peak area (Q eu ) at the eutectic point according to: Qeu = meuǻHeu = (mPEG,eu/wPEG,eu)ǻHeu (1) ZKHUH^ǻHeu = 142 r 1 J/(g eutectic mixture) was evaluated by linear fits of the enthalpies of fusion of the PEG/water eutectic mixtures and w PEG,eu = 0.47 is the mass fraction of PEG at the eutectic point (Teu = –19°C). Given that a portion of PEG segments are dehydrated to cover the surface of hydrophobic core, only the rest (e.g., hydrated PEG segments) can form a eutectic mixture with nearby water. The fraction of hydrated PEG, fhyd = mPEG,eu/mPEG, was evaluated from eq 2: ¨+eu:PEG = Qeu/mPEG = [mPEG,eu/(wPEG,eumPEG)]ǻHeu = (fhyd/wPEG,eu)ǻHeu , (2) where mPEG is the total mass of PEG in the sample, and ¨+eu:PEG is the enthalpy of fusion at the eutectic point per total mass of PEG.¨ +eu:PEG and fhyd for each sample are reported in Table 4. ) f ) 3 . f m C 7 . 4 . n T ° ( 8 8 ) e d 2 9 y f h 1 . 0 0 . 0 0 0 0 0 0 0 0 0 c o c i n e p hg s t da ) t i d ) i n n e n l t e l r e mg s G G e m e e l l E P : E 8 8 0 4 0 01 6 4 mk 7 0 5 l y a s e G i c ue P 3 2 5 8 1 6 1 0 0 4 oe m H g / p ¨ J ( f p E oc i t P f e o nc h t n o i t e t f o i t cu E o a a ) o i t g r ft d a e r g h . t r e g i g i n h ) A eo p t s g ) d 6 5 3 9 1 5 6 6 ) W b g i n a . r e t u ) . . . . . . . . C 5 6 6 5 5 5 4 5 . dz d e e a e T ° ( 1 – 1 – 1 – 1 – 1 – 1 – 1 – 1 – o e r n i f w h t e m ) F ed l k c , u ) . n b y o e P Nh i t p c h t E 4 ( a r a r f f o . ) l ng G t i n e o o t n o i ba ) i c t E o t T f ) 6 . C 5 1 . 1 5 7 . 1 3 6 . 1 2 3 . 1 3 4 . 6 . 0 . 1 . 7 . 5 . 8 . aa i t m P p a 1 21 91 81 71 3 0 9 i p o r d gg e t i n u i f T ° ( – – – – – – – – – 1 – 1 – 1 – ch e r c a r l t r t p d ene o i a y M n v H ) f c ad ne ) e . i a i . m v d ) m n m e t u m r e t s e r b i e r t s yap y l ) b an g ) g ) g ) g i l i e t e y s ud s e e r p a , p 0 1 . 8 0 . 9 0 . 6 0 . 3 0 . 2 0 . 4 0 . 1 0 . 8 0 . 9 0 . 7 0 8 q ) e h 0 e n h t t n ( 2 n 2 1 w 0 0 0 0 0 0 0 0 0 0 . 0 . 0 eo h i t n i i i o s O t a G ngu GEn E Pe W5 i 3 d i fr t P f l psu 1 e . s n a t e o o t s 5 u r c med61 i a a h e t 1 ) a P e t N a v r g t a r t WL E , w w 2 S . 3 . 5 . 6 . 1 . 2 . 3 . 5 . 1 . 2 . 3 5 f d e r o r e t nec / ij 0 0 0 0 0 0 0 0 0 0 . 0 . 0 o na p e n r un 2 op 0 - i t e r i o t i x o c5 3 cp s2 H a r ( u f m eh 9 f n f c i 9 3 C t t n6 . H O i - e o s o y c i so H C m G n l p e t u e l N O E l u oep a e l e . f r - O - e G G P -e ) Vs h t e i c m E E A a u s n e h t m R y P - P - M F l o S S B R P P P t P P 5 PRF Ref. No.69925-02/SLW 1165.135WO1 Results and Discussion Surface Mechanics of PS-PEG-OH Micelles in the Presence of Excipients [0062] Excipients are commonly added to prevent structural damage and irreversible aggregation of nanoparticulate drugs caused by freezing and drying stresses, which result from ice crystallization and solvent evaporation, respectively, in conventional lyophilization processes. These excipients are typically hydrophilic molecules that can interact favorably with both water (through hydrogen bonding) and particle surface (through van der Waals interactions). However, due to this amphiphilic nature of excipients, they can have detrimental effects on the surface activity of block copolymer micelle formulations, either by modifying the surface energy of hydrophobic micellar cores or by competitively adsorbing at the air-water interface. To examine the effect of excipients on the surface mechanical behavior of the model PLS formulation prior to the lyophilization study, two saccharides (sucrose and HPȕCD) and two hydrophilic polymers (2 and 5 kg/mol PEG-OCH3) were selected as representative excipients. A concentration of 10% w/v, which falls within the typical range of 5–20% w/v for optimal protection, was used. [0063] FIG.1 compares the surface pressure–area (Ȇ–A) isotherms of PS-PEG- OH micelles formulated at ijw,ENP = 0.6 with and without excipients. Here, the surface pressure (Ȇ ^Ȗ0 – Ȗ^^^GHILQHG^DV^WKH^GHFUHPHQW^LQ^VXUIDFH^WHQVLRQ^IURP^ WKDW^ RI^ SXUH^ZDWHU^ ^Ȗ0 = 72 mN/m), is plotted against the trough area (A). The chosen model formulation exhibited the ability to achieve low suUIDFH^WHQVLRQ^^Ȗ^^^ 10 mN/m) upon compression of the surface, as demonstrated by the control isotherm. Strikingly, the addition of any excipient to the PS-PEG-OH formulation resulted in the loss of surface activity, preventing the attainment of high Ȇ values. While not wishing to be bound by any specific theory, it is speculated that saccharides and PEG-OCH 3 excipients reduce the surface activity of PS-PEG-OH micelles in different ways. Consistent with a previous study, the isotherms of the saccharide-containing formulations resemble the typical surface mechanical behavior of block copolymer micelles with weakly hydrophobic cores, such as poly(D,L-lactic acid-block-ethylene glycol) (PLA-PEG). This suggests a possible reduction in the interfacial tension between water and the hydrophobic PS core due to the mediating effect of saccharides, in line with literature on the favorable interactions between sucrose and globular proteins. [0064] On the other hand, PEG-OCH 3 excipients compete with the adsorption of PS-PEG-OH micelles at water surfaces. The maximum Ȇ values of PEG (2 and 4.6 kg/mol) monolayers formed by spontaneous adsorption from the subphase were 8 and 9 mN/m, respectively, which are nearly the same as the equilibrium PRF Ref. No.69925-02/SLW 1165.135WO1 spreading pressure of PS-PEG-OH micelles (10 mN/m). Thus, PEG-OCH 3 excipients (at a weight ratio of 20:1 to PS-PEG-OH micelles) likely occupy most of the available surface area and reduce the amount of adsorbed PS-PEG-OH micelles at the water surface. Apparently, it is difficult to use excipients as cryo- and lyoprotectants without causing the reduction in surface activity of PLS. Moreover, the removal of excipients from lyophilized samples requires complicated purification steps, such as prolonged dialysis, which is not clinically practical. Operation Parameters for Excipient-Free Lyophilization of PS-PEG-OH Micelles [0065] To avoid the problems in using excipients, an aim was to investigate the optimal operating conditions for excipient-free lyophilization. The same formulation as in the section entitled Surface Mechanics of PS-PEG-OH Micelles in the Presence of Excipients (PS-PEG-OH micelles formulated at ijw,ENP = 0.6) was used EHFDXVH^LW^H[KLELWHG^WKH^KLJKHVW^3(*^JUDIWLQJ^GHQVLW\^^ıPEG ) among all formulations in this study (Table 3; the effect of ıPEG will be discussed later). [0066] To identify the impact of process parameters on the quality of excipient- free lyophilization, two different methods were employed using a small-batch research-scale lyophilizer (MicroFD, Millrock Tech). Method A was designed to achieve more aggressive freezing compared to Method B, characterized by a faster cooling rate and a lower shelf temperature (Tshelf) during the freezing stage (refer to Table 3 for the operation parameters of Methods A and B). FIGS.2A and 2B depict the heat flux evolution between the shelf and the vial chamber along the initial freezing trajectory, where a negative peak in the heat flux corresponds to ice crystallization. The onset of the heat flux peak, indicating ice nucleation, occurred at a lower shelf temperature (–27.2°C) for Method A compared to Method B (– 21.4°C). The lower nucleation temperature leads to higher nucleation density and smaller crystallites, which can reduce the mechanical stress exerted by ice crystals and thus benefit nanoparticle preservation. Additionally, the interval between ice nucleation and the maximum rate of ice growth (indicated by shaded regions in FIGS.2A-2B was slightly shorter (9 min) for Method A compared to Method B (10 min), suggesting slightly faster crystallization when the cooling rate is doubled. [0067] On the other hand, during the primary drying stage, both Methods A and B underwent steady-state sublimation of water until complete evaporation. Since the T shelf values used in the primary drying stage were significantly lower than the eutectic temperature (T eu = –19°C) and the "collapse" temperature (–18°C) in both methods, the quality of lyophilization (as discussed below) is unlikely to be influenced by the differences in primary drying stage parameters. PRF Ref. No.69925-02/SLW 1165.135WO1 [0068] Consequently, Method A yielded better redispersibility and surface activity of the model formulations after reconstitution compared to Method B. The size increasing factor (SIF), defined as the ratio of the z-average hydrodynamic diameter (<D h >) of micelles after reconstitution to that before lyophilization, was lower for Method A (Table 3), indicating less pronounced irreversible aggregation. $GGLWLRQDOO\^^ WKH^ GLIIHUHQFH^ EHWZHHQ^ WKH^ Ȇ–A isotherms of pristine and reconstituted micelles from Method A (FIG.2C) was smaller than that from Method B (FIG. 2D), although both reconstituted micelles could achieve high surface SUHVVXUH^^Ȇmax # 70 mN/m) at maximum surface compression. Therefore, Method A was selected as the standard lyophilization procedure for the subsequent experiments. [0069] In polymer-grafted nanoparticles, the grafting density of hydrophilic SRO\PHUV^^ı PEG ) is a critical parameter to the colloidal stability of the formulations. $^ KLJKHU^ ı PEG leads to a thicker and denser PEG brush, promoting stable dispersion. This stabilizing effect of densely grafted polymer brushes is particularly relevant during the freezing stage, where ice growth reduces the available space for the particles and forces them to come into close proximity (referred to as "cryo- FRQFHQWUDWLRQ^^^^,Q^VXFK^VLWXDWLRQV^^D^KLJK^ıPEG is expected to protect the particles from irreversible aggregation by efficiently dampening the compressive stress. This is because the PEG brush remains partially hydrated and amorphous even below freezing temperature (see below for detailed discussion). [0070] It is noteworthy that Logie et al. have observed enhanced redispersibility following lyophilization, utilizing nonlinear (graft) copolymers that incorporate a higher number of PEG side chains, without the need for excipients. But, in the examples provided by Logie et al., the mean hydrodynamic diameters of the polymer micelles consistently exceeded approximately 85 nm. In contrast, as indicated in Table 2 above, the majority of the micelles described therein exhibited hydrodynamic diameters of less than approximately 50 nm. And there is evidence that the therapeutic effectiveness of micelles, particularly as polymer lung surfactants, can be compromised when the mean hydrodynamic diameter exceeded approximately 55 nm. See, e.g., Kim et al., ACS. Appl. Bio. Mater., 2018, (Figure 5), which is incorporated by reference as if fully set forth herein. Accordingly, the disclosure relates to micelles with a mean hydrodynamic diameter of less than about 90 nm, less than about 85 nm, less than about 80 nm, less than about 75 nm, less than about 70 nm, or less than about 60 nm; such as from about 1 nm to about 90 nm, about 10 nm to about 80 nm, about 10 nm to about 75 nm, PRF Ref. No.69925-02/SLW 1165.135WO1 about 20 nm to about 80 nm, about 15 nm to about 60 nm, or about 25 nm to about 90 nm. [0071] In the systems described herein^^WKH^ı PEG was systematically controlled by varying the number of block copolymer chains that constitute a micelle, also known as the aggregation number (N agg ). This control was achieved by applying the equilibrium nanoprecipitation (ENP) method with different qualities of a selective solvent. A higher water fraction in the ENP medium (ij w,ENP ) results in self-assembly with a higher N agg during the process of free energy minimization, leading to larger ı PEG . In this study, four micelle formulations were tested ZLWK^GLIIHUHQW^ı PEG values ranging from 7.1 to 11.3. These formulations were prepared using the identical starting polymer but at different ijw,ENP values (Table 2). The pristine micelles exhibited uniform sizes in all formulations, and the average core diameter (Dc) increased monotonically with ijw,ENP. However, the z-average hydrodynamic radius (<Dh>) of the pristine micelles did not follow a monotonic trend with ijw,ENP due to an outlier (ijw,ENP = 0.2) with the presence of significant amounts of large clusters (Table 2). [0072] The redispersibility of micelles after lyophilization and subsequent UHFRQVWLWXWLRQ^ VKRZHG^ D^ VLJQLILFDQW^ LQFUHDVH^ ZLWK^ ıPEG. Transmission electron microscopy (TEM) images of the reconstituted micelles revealed that clustered micelles were larger than 100 nm at ijw,ENP = 0.2 and 0.3, but decreased to approximately 50 nm at higher ijw,ENP values (FIGS. 3E-3H). Dynamic light scattering (DLS) analysis provided consistent results, as indicated by the unanimous increase in the z-average hydrodynamic radius (<Dh>) after lyophilization (Table 2). However, the size increasing factor (SIF), defined as the ratio of <Dh> of reconstituted micelles to pristine micelles, decreased with increasing ij w,ENP RU^^HTXLYDOHQWO\^^LQFUHDVLQJ^ı PEG . [0073] The surface activity of the reconstituted micelles exhibited a strong correlation with their redispersibility, indicating that it was preserved more HIIHFWLYHO\^ ZLWK^ KLJKHU^ ı PEG . FIGS. 4A and 4B demonstrate that the surface pressure (Ȇ) was significantly reduced at ij w,ENP = 0.2 and 0.3. This reduction can be attributed to the low availability of surface-active micelles, as clustered micelles with irregular shapes cannot expose their hydrophobic cores to the air efficiently and therefore are easily detached from the air/water surface. To quantify this effect, the concept of surface availability (SA) was introduced, which represents the multiplication factor required to overlap the pristine isotherm with the reconstituted isotherm (inset in FIG. 4A). For example, an SA value of 0.36 at ij w,ENP = 0.2 indicates that only 36% of surface-active micelles from the reconstituted PRF Ref. No.69925-02/SLW 1165.135WO1 formulation are available. As the micelles become more densely grafted with PEG, the Ȇ–A isotherms of the reconstituted formulations approach those of the pristine micelles (FIGS.4D-4E), resulting in an increase in SA close to unity (Table 2). This clearly demonstrates the feasibility of excipient-free lyophilization when the pharmaceutical formulation consists of densely PEG-grafted micelles. [0074] Furthermore, the lyophilized micelles in powder form could also be spread on the water surface and exhibited surface activity even without reconstitution. The Ȇ–A isotherms of solid lyophilizates were compared with those of the reconstituted formulations in FIGS.4A-4E. It was observed that the solid lyophilizates displayed comparable or even stronger surface activity, partially due to a larger amount of material deposited on the surface (approximately 1.5 mg of solid was deposited, theoretically three times greater than the mass of solute used in the pristine and reconstituted aqueous formulations). Nevertheless, the feasibility of directly spreading solid lyophilizates to achieve high surface pressure (Ȇ) is encouraging, as it may enable the delivery of PLS micelles to the alveolar space (deep inside the lungs) through inhalation, which is a more desirable approach than liquid instillation in clinical practice. Effects of End Group and Core Block Chemistry [0075] The study was expanded to include an analogous amphiphilic block copolymer, PS-PEG-OCH3, which has similar block molecular weights and high surface activity. The main difference between PS-PEG-OH and PS-PEG-OCH3 is the end group chemistry at the PEG block (Table 1). Similar to the PS-PEG-OH series, we prepared micelles from PS-PEG-OH and PS-PEG-OCH3 using the ENP method with four (4) different ijw,ENP. TEM images confirmed that all micelles were uniformly sized (FIGS.5A-5H) DQG^H[KLELWHG^KLJKHU^YDOXHV^RI^ıPEG with increasing ij w,ENP . However, DLS analysis revealed an unusually large <D h > for the ij w,ENP = 0.5 formulation, indicating the presence of supra-micellar aggregates (Table 2). Additionally, the micelles formulated at ij w,ENP = 0.5 showed minimal surface activity (FIG.6D), making them unsuitable as PLS. [0076] Reconstituted PS-PEG-OCH 3 micelles after lyophilization appeared as large chunks (>100 nm) in all samples (FIGS.5E-5H). DLS analysis showed higher size increasing factors (SIF) for PS-PEG-OCH 3 micelles (SIF > 5), except for the ij w,ENP = 0.5 formulation, which already had large, aggregated clusters in the pristine state. In comparison, the SIF values for PS-PEG-OH micelles were generally smaller (SIF < 5) (Table 2). These systematic differences indicate that a small change in the end group chemistry of the PEG block, from hydroxy to methoxy, leads to a significantly decreased stability. While not wishing to be bound PRF Ref. No.69925-02/SLW 1165.135WO1 by any specific theory, this may be attributed to the bridging effect of the hydrophobic methoxy (–OCH 3 ) end group, which promotes closer contact between the micellar cores, especially under cryo-condensed conditions. It is interesting to note that significant aggregation of all PS-PEG-OCH 3 micelles also occurred after centrifugation (at approximately 11,000×g for 20 min), whereas the centrifuged PS- PEG-OH micelles were easily redispersed (Table 4). Furthermore, both reconstituted and solid lyophilized forms of PS-PEG-OCH 3 micelles exhibited impaired surface activity (FIGS. 6A-6D), and the surface availability (SA) after reconstitution was less than 0.3 in all samples, except for the ij w,ENP = 0.5 formulation (Table 2). [0077] Next, another amphiphilic block copolymer, PtBMA-PEG-OCH3, with a different core block, was investigated for excipient-free lyophilization. In its pristine form, the PtBMA-PEG-OCH3 micelle formulation exhibited high surface activity, generating surface pressures as high as Ȇ = 68 mN/m in our recent study. TEM images confirmed that all PtBMA-PEG-OCH3 micelles formulated at 4 different ijw,ENP appeared as uniformly sized particles (FIGS. 7A-7D). However, for the ijw,ENP = 0.5 formulation, an unusually large <Dh> and the inability to generate high surface pressure upon compression indicated the presence of supra-micellar aggregates (Table 2 and FIGS.8A-8D). [0078] Due to the hydrophobic methoxy end group at the PEG chain of PtBMA- PEG-OCH3, the lyophilization results were similar to those of PS-PEG-OCH3 micelles. Reconstituted PtBMA-PEG-OCH3 micelles after lyophilization were observed as large chunks (>100 nm) (FIGS. 7E-7H). DLS analysis consistently showed size increasing factors (SIF) greater than 3 for reconstituted micelles, except for the ijw,ENP = 0.5 formulation where the pristine micelles already exhibited large superstructures (Table 2). Once again, the pronounced aggregation in PtBMA-PEG-OCH 3 micelles after excipient-free lyophilization can be primarily attributed to the bridging effect of the methoxy (–OCH 3 ) end group. Consequently, the surface activity of PtBMA-PEG-OCH 3 micelles in both reconstituted and solid lyophilized forms was compromised (FIGS. 8A-8D). Furthermore, the surface availability (SA) after reconstitution was below 0.2 in all samples, except for the ij w,ENP = 0.5 formulation (Table 2). However, there were slight differences in the lyophilization results between PS-PEG-OCH 3 and PtBMA-PEG-OCH 3 micelles (excluding all ij w,ENP = 0.5 formulations). The overall SIF values were smaller, and the solid lyophilizates exhibited higher surface activity in PtBMA-PEG-OCH 3 micelles. While not wishing to be bound by any specific theory, this may suggest that PtBMA-PEG-OCH3 micelles may be slightly more stable in maintaining PRF Ref. No.69925-02/SLW 1165.135WO1 colloidal dispersion. Similarly, the centrifuged PtBMA-PEG-OCH 3 micelles did not aggregate as strongly as the PS-PEG-OCH 3 micelles. However, the exact origin of this difference (in relation to the core block chemistry) is not yet fully understood. Differential Scanning Calorimetry (DSC) [0079] The stability of PS-PEG-OH micelles increased as the grafting density ^ı PEG ) grew, whereas no such effect was observed in PS-PEG-OCH 3 and PtBMA- PEG-OCH 3 micelles. To further investigate the impact of grafting density during the lyophilization cycle, we measured DSC thermograms of the aqueous micelle solutions. The solutions were cooled from 30°C to –50°C and subsequently heated to 30°C at a ramping rate of ±5 °C/min (FIGS.9A-9C). To accurately capture the PEG/water eutectic behavior (Teu = –19°C), the solution concentrations were increased through centrifugal dialysis. The polymer weight fraction after centrifugation (wp,analyte) ranged from 1% to 10% (Table 4). Notably, significant aggregation occurred in PS-PEG-OCH3 micelles formulated at ijw,ENP = 0.1, 0.2, and 0.5, resulting in a substantial loss of micelles in the concentrated suspensions. [0080] DSC thermograms provided insights into the nanoscopic changes of PEG- grafted micelles in the lyophilization medium (FIG. 10A). Typically, phase separation between PEG and water occurs after the bulk ice crystallization at the freezing point (Tf). However, as described in previous studies, not all PEG and water components separate into perfectly isolated crystals; instead, a substantial amount of amorphous PEG/water mixture remains even below Teu. Upon heating the system from –50°C to Teu, the crystallized portion of PEG and the adjacent water melt to form a eutectic mixture. This eutectic melting is displayed in the enlarged thermograms (insets of FIGS. 9A-9C). The Teu values were in close agreement (–15.5 ± 0.9°C), but the specific heat of fusion for the eutectic mixture ^¨H eu:PEG ) varied among the samples (Table 4). Moreover, PS-PEG-OCH 3 (ij w,ENP = 0.1) and PtBMA-PEG-OCH 3 (ij w,ENP = 0.1, 0.2, and 0.3) micelles did not exhibit eutectic melting. After surpassing T eu , the bulk ice finally melted at the melting point (T m ). Most of the samples showed very similar T m values and specific heat of melting. [0081] The eutectic melting was analyzed to evaluate the fraction of PEG segments that can freely interact with water, referred to as the hydrated PEG fraction (f hyd ). The distinction between hydrated and dehydrated PEG segments arises from the presence of a hydrophobic surface in block copolymer micelles. Previous studies have demonstrated that PEG brushes can form dense and nearly dehydrated layers at solid-water interfaces to reduce surface energy. It may be that strongly hydrophobic PS and PtBMA cores necessitate partial dehydration of PRF Ref. No.69925-02/SLW 1165.135WO1 PEG brushes to form a dense layer (FIGS. 10A-10C). The remaining PEG segments can be hydrated, and when a micellar suspension is frozen below T eu , a portion of the hydrated PEG crystallizes, while the other portion remains amorphous as a supercooled mixture with water. The measured heat of fusion at T eu ^¨H eu:PEG ) originates from the cooperative melting of the crystalline portion of PEG in contact with ice, and it is suppressed when the PEG brush is less hydrated, less hydrated PEG segments crystallize during the freezing stage, or the crystalline 3(*^VHJPHQWV^ORVH^FRQWDFW^ZLWK^ZDWHU^^7KHUHIRUH^^¨H eu:PEG provides an easy way to characterize the state of PEG brushes in the frozen micelle solution. [0082] In the reference system (an aqueous solution of homopolymer PEG), the empirical heat of melting per PEG/water eutectic mixture (ǻHeu) was 142 J/(g eutectic mixture). Note that this value is significantly lower than the theoretical limit of ~270 J/(g eutectic mixture) indicating imperfect crystallization. Owing to the similar DSC methods (rapid cooling) used in the present work and the reference (- 5°C/min), a comparable PEG crystallinity with the reference system can be assumed. Thus, we used eq.2 with ǻHeu = 142 J/(g eutectic mixture) to evaluate fhyd of the micelle samples. The results of fhyd (Table 4) show that, in most samples, the majority of PEG segments exists as a dehydrated film to cover the hydrophobic core surface (i.e., fhyd < 0.5). Nevertheless, it is rather surprising that PS-PEG- OCH3 (ijw,ENP = 0.3) and PtBMA-PEG-OCH3 (ijw,ENP = 0.1, 0.2, and 0.3) micelles lacks any signature of eutectic melting. While not wishing to be bound by any specific theory, it may be that freezing-induced massive aggregation in these samples isolated most of the PEG segments within the interior of aggregated micellar superstructure. Such an entrapping effect may have prevented the crystallized portion of PEG from eutectic melting with water. The correlation between f hyd and the size increase factor (SIF) obtained from the lyophilization experiment (FIGS. 9A-9D) supports this idea; generally, f hyd is lower when the sample has a greater SIF (e.g., intense aggregation). [0083] Regarding the effect of micelle structure, FIG.9E illustrates a clear trend of increasing f hyd ZLWK^KLJKHU^ı PEG . In PS-PEG-OH micelles, the hydrated fraction JUDGXDOO\^LQFUHDVHV^DV^ı PEG increases. Since the area per PEG chain required to cover the core surface decreases with iQFUHDVLQJ^ ı PEG , the PEG chains can allocate more segments to be hydrated after forming a dehydrated film (FIG.10B). &RQVHTXHQWO\^^PLFHOOHV^ZLWK^KLJKHU^ı PEG exhibit thicker amorphous layers, which can effectively mitigate freezing-induced stress during the freezing stage. Similarly, in PS-PEG-OCH 3 and PtBMA-PEG-OCH 3 micelles, the eutectic melting behavior LV^REVHUYHG^RQO\^DW^KLJKHU^ıPEG, indicating that the fraction of hydrated PEG is too PRF Ref. No.69925-02/SLW 1165.135WO1 ORZ^ DW^ ORZHU^ı PEG . However, due to the presence of hydrophobic methoxy end groups, the PEG chains now act as linkers between the cores, leading to irreversible aggregation (FIG. 10C). This suggests that block copolymers with a hydrophobic end group in the PEG block are susceptible to destabilization during lyophilization. Therefore, excipient-free lyophilization is feasible only if (i) the PEG grafting density is sufficiently high to form an amorphous layer which can dissipate the external freezing stress and (ii) the PEG end group does not induce bridging interactions. [0084] PEG grafting density and the endgroup at the PEG block simultaneously affect both the surface availability (SA) of the reconstituted micelles and the hydrated PEG fraction (fhyd). Indeed, FIG.9F reveals a strong correlation between fhyd and SA even if the thermal trajectories used in the two experiments (DSC and lyophilization) were not the same. Since SA is the most important property in terms of pharmaceutical surfactant formulation, this finding suggests that DSC can serve as an initial screening tool for evaluating the success of excipient-free lyophilization of PLS. Conclusions [0085] Although the use of excipients is a common practice in pharmaceutical lyophilization, there are instances where the removal of excipients becomes necessary. Polymer lung surfactant (PLS) are a case where commonly used excipients, such as saccharides and PEG, hinder the surface activity of PLS. Described herein are certain optimal conditions for excipient-free lyophilization, including material and operating parameters, using a small-batch research-scale lyophilizer. Micelles formulated through equilibrium nanoprecipitation (ENP) were tested using three different block copolymers and four incubating water fractions (ij w,ENP ). The reconstitution ability after excipient-free lyophilization was assessed through various techniques, including DLS hydrodynamic sizes, TEM images of the reconstituted micelles, and Langmuir force balance analysis (surface pressure–area isotherms) of both the solid lyophilizates and reconstituted micelles. It was found that a faster cooling rate during the freezing stage was advantageous, as it reduced the freezing stress by forming smaller ice crystallites. [0086] Among the variations in block copolymer chemistry, the PEG block end group was identified as a significant factor. The presence of a hydrophobic methoxy end group promoted irreversible aggregation of the micelles. In the case of PS-PEG-OH with a hydroxy end group, a decrease in the size increase factor (SIF) and an increase in surface availability (SA) with higher PEG grafting density were observed. This can be attributed to a higher fraction of hydrated PEG in the PRF Ref. No.69925-02/SLW 1165.135WO1 micelle formulation, as evidenced by the specific heat of melting at the eutectic point (T eu ). In the most successful lyophilization process, which involved PS-PEG- OH formulated at ij w,ENP = 0.5, the reconstituted suspension exhibited an SA of 87%, and the solid lyophilizate perfectly reproduced the isotherm of the pristine suspension. Based on these results, it is proposed that the amorphous mixture of PEG/water surrounding the micellar core plays a crucial role in dissipating the freezing stress, thereby preventing irreversible aggregation of the micelles. [0087] The above results suggest that BCP micelle PLS can even be delivered as a dry powder aerosol for treatment of lung disorders caused by lung surfactant dysfunction or deficiency, including ARDS, ALI, NRDS, etc. Aerosolized PLS in the form of dry powder or liquid droplets can be delivered to the lungs with the aid of a nebulizer, an inhaler or a mechanical ventilator. [0088] The following numbered statements are provided to further describe the scope of the disclosure: [0089] 1. A composition comprising: solid amphiphilic block copolymer micelles having a hydrodynamic diameter in the range of about 5 nm to about 1,000 nm, the micelles comprising substantially no excipients. [0090] 2. The composition of Statement 1, wherein the amphiphilic block copolymer comprises a poly(styrene) and a poly(ethylene glycol) block. [0091] 3. The composition of Statement 1, wherein the amphiphilic block copolymer comprises substantially the same number-average molecular weights of PS and PEG blocks. [0092] 4. The composition of Statement 1, wherein the PEG-end group of PS– PEG block copolymer is a hydroxyl group. [0093] 5. The composition of Statement 1, wherein the micelles have high PEG JUDIWLQJ^GHQVLW\^ı3(*^ [0094] 6. The composition of Statement ^^^ZKHUHLQ^WKH^ı3(*^LV^DERXW^^^RU^JUHDWHU^ [0095] 7. A kit comprising the composition of Statement 1 in a first container. [0096] 8. The kit of Statement 7, wherein the kit further comprises water in a second container. [0097] 9. A method of treating a pulmonary disorder in a subject, the method comprising administering to said mammal a therapeutically effective amount of the composition of Statement 1 reconstituted in water. [0098] 10. The method of Statement 9, wherein the pulmonary disorder is caused by at least one of a deficiency and the deactivation of functional lung surfactant in the subject. PRF Ref. No.69925-02/SLW 1165.135WO1 [0099] 11. The method of Statement 9, wherein the subject is a mammal. [00100] 12. The method of Statement 9, wherein the subject is a human. [00101] 13. A method comprising: (a) dissolving amphiphilic block copolymer in a mixed water-acetone cosolvent; (b) conducting a single-step dialysis against water to form kinetically frozen monodisperse micelle system in aqueous conditions to give polymer lung surfactant aqueous solution; and (c) lyophilizing the polymer lung surfactant aqueous solution to give polymer lung surfactant micelles; wherein the polymer lung surfactant aqueous solution comprises substantially no excipients before the lyophilization. [00102] 14. The method of Statement 13, wherein the amphiphilic block copolymer comprises a poly(styrene) and a poly(ethylene glycol) block. [00103] 15. The method of Statement 13, wherein the amphiphilic block copolymer comprises substantially the same number-average molecular weights of PS and PEG blocks. [00104] 16. The method of Statement 13, wherein the PEG-end group of PS-PEG block copolymer is a hydroxyl group. [00105] 17. The method of Statement 13, wherein the step of dissolving comprises: (a) dissolving PS-PEG block copolymers in a mixed cosolvent with initial acetone composition between 50% and 60% (v/v); (b) sonicating the solution; (c) mechanically agitating the solution; (d) heating the solution; and (e) leaving the solution quiescent overnight for the equilibration. [00106] 18. The method of Statement 13, wherein the step of single-step dialysis comprises: (a) dialyzing the solution using a dialysis bag against the water reservoir overnight; and (b) replacing the aqueous reservoir with clean water for at least three times. [00107] 19. The method of Statement 13, wherein the lyophilizing comprises: (a) freezing the aqueous polymer lung surfactant solution; (b) sublimating crystalized water from the polymer lung surfactant solution until no further water sublimation is detected; and (c) desorbing and vaporizing the supercooled water adsorbed onto the polymer lung surfactant nanoparticles. PRF Ref. No.69925-02/SLW 1165.135WO1 [00108] 20. The method of Statement 19, wherein the freezing rate is - 2°C/min. [00109] 21. The method of Statement 19, wherein the rate of temperature increase between the freezing and the primary drying steps is 1°C/min. [00110] 22. The method of Statement 19, wherein the rate of temperature increase between the primary drying and the secondary drying steps is 1°C/min. [00111] 23. The method of Statement 19, wherein the lyophilized polymer lung surfactant can be potentially used as the aerosolized therapy to treat acute respiratory distress syndrome. [00112] 24. A method of reconstituting lyophilized polymer lung surfactant, the method comprising: (a) dissolving lyophilized polymer lung surfactant of Statement 1 in water; (b) shaking the dissolved polymer lung surfactant; and (c) sonicating the dissolved polymer lung surfactant.