Systematic surface energy modifications to glass substrates can induce nucleation and improve crystallization outcomes for small molecule active pharmaceutical ingredients (APIs) and proteins. A comparatively broad probe for function is presented in which various APIs, proteins, organic solvents, aqueous media, surface energy motifs, crystallization methods, form factors, and flat and convex surface energy modifications were examined. Replicate studies (n ≥ 6) have demonstrated an average reduction in crystallization onset times of 52(4)% (alternatively 52 ± 4%) for acetylsalicylic acid from 91% isopropyl alcohol using two very different techniques: bulk cooling to 0 °C using flat surface energy modifications or microdomain cooling to 4 °C from the interior of a glass capillary having convex surface energy modifications that were immersed in the solution. For thaumatin and bovine pancreatic trypsin, a 32(2)% reduction in crystallization onset times was demonstrated in vapor diffusion experiments (n ≥ 15). Nucleation site arrays have been engineered onto form factors frequently used in crystallization screening, including microscope slides, vials, and 96- and 384-well high-throughput screening plates. Nucleation using surface energy modifications on the vessels that contain the solutes to be crystallized adds a layer of useful variables to crystallization studies without requiring significant changes to workflows or instrumentation.
Systematic surface energy modifications to glass substrates can induce nucleation and improve crystallization outcomes for small molecule active pharmaceutical ingredients (APIs) and proteins. A comparatively broad probe for function is presented in which various APIs, proteins, organic solvents, aqueous media, surface energy motifs, crystallization methods, form factors, and flat and convex surface energy modifications were examined. Replicate studies (n ≥ 6) have demonstrated an average reduction in crystallization onset times of 52(4)% (alternatively 52 ± 4%) for acetylsalicylic acid from 91% isopropyl alcohol using two very different techniques: bulk cooling to 0 °C using flat surface energy modifications or microdomain cooling to 4 °C from the interior of a glass capillary having convex surface energy modifications that were immersed in the solution. For thaumatin and bovinepancreatic trypsin, a 32(2)% reduction in crystallization onset times was demonstrated in vapor diffusion experiments (n ≥ 15). Nucleation site arrays have been engineered onto form factors frequently used in crystallization screening, including microscope slides, vials, and 96- and 384-well high-throughput screening plates. Nucleation using surface energy modifications on the vessels that contain the solutes to be crystallized adds a layer of useful variables to crystallization studies without requiring significant changes to workflows or instrumentation.
The isolation
of crystalline
materials continues to be a foundational aspect of chemical characterization,
purification, and manufacturing.[1,2] In the field of pharmaceutical
development, the cost-effective purification and predictable performance
of a crystalline solid are much sought after for small molecule active
pharmaceutical ingredients (APIs),[2−4] and X-ray crystal structures
of biological macromolecules are fundamental to both the structure–function
understanding and structure-based drug design.[5,6] Despite
over a century of detailed investigation, the crystallization of new
chemical entities is still largely an empirical process that often
requires tens to thousands of screening experiments. The advent of
96- and 384-well plates and automated high-throughput screening (HTS)
instrumentation have enabled probabilistic approaches to crystallization
that involve screening large numbers of conditions to produce crystalline
“hits”.[7] By example, various
structural biology groups have developed sophisticated automated HTS
crystallization workflows over the last 15 years in order to alleviate
the “crystallization bottleneck” in protein structure
determination by crystallographic methods.[8,9] Despite
careful optimization, the greatest attrition still occurs at the crystallization
step, in which the average success rate for isolation of diffraction
quality crystals hovers in the 5–7% range.[10] Only for a few sophisticated laboratories do success rates
reach 15–20%,[8,11] and these confoundingly low crystallization
success rates underscore the need for rational methods to improve
crystallization outcomes for proteins. Advances can be expected to
have a significant impact in structural biology, as >80% of the
costs
associated with structure determination are incurred after the proteins
have been purified.[12]The identification
of solid form variants including polymorphs,
solvates, and hydrates continues to be an important and regulated
aspect of small molecule API development because these different solids
can have very different dissolution characteristics that can affect in vivo drug performance.[1−4,13,14] The needs for such crystal form screening are broad-based
and will persist given that ≈90% of APIs are crystalline materials[13,15] and that ≈50–80% of small molecule APIs exhibit polymorphism
at some point from discovery through manufacturing.[16−18] The many unpredictable
aspects of polymorphism, and of solid form variation in general, underpin
the need for rational approaches to improving crystallization outcomes
for small molecule APIs, and advances here can be anticipated to help
minimize the costly economic penalties incurred from untimely polymorphic
transformations (e.g., Norvir, Avalide, etc.). As importantly, enhanced
crystal nucleation can create value in the form of new intellectual
property for commercially relevant API compositions and by making
solid form screening more complete and time efficient. For example,
eliminating just one month from development of a $5B blockbuster drug
to yield an additional month of sales under patent can be worth more
than $400M.Crystallization is often divided into the two sequential
processes
of nucleation and crystal growth,[1,2] with nucleation
representing the best opportunity to rationally influence crystallization
success rates because the thermodynamic drivers have not yet been
fixed by the emergence of a crystal lattice. As the solutes in a supersaturated
solution undergo the molecular recognition, aggregation, and preorganization
processes that shuttle impurities, solvent, etc., out of the prenuclear
aggregate, this species becomes a heterophase and presents a new surface
to the supersaturated solution that interfaces with other aggregates,
solvent, adventitious solids, and with the vessel or surface that
contains the supersaturated solution. Vessels and other surfaces in
contact with supersaturated solutions are well-known to lower the
energy required to achieve heterogeneous primary nucleation,[1,11,19−21] and thus, the
fluxional and growing solute aggregates can be predisposed to nucleation
using appropriate solid substrates. A variety of surface coating strategies
using organosilanes or self-assembled monolayers[22] has been used in crystallization; for example, the bifunctional
self-assembled monolayers use directed chemical interactions with
the solutes to be crystallized to give small particle sizes, narrow
size distributions,[23−25] and even polymorph control.[26−28] An interesting
complementary strategy that is independent of directed chemical interactions
is to systematically alter the substrate surface (e.g., by etching,
ablation, additive manufacturing, etc.) to give a continuum of surface
energy characteristics that can facilitate nucleation through interactions
between the vessel surface, the supersaturated solution, and the fluxional
prenuclear aggregates therein. Such physical alterations are well-known
to affect various surface properties including wettability and, by
extension, the surface energy.[29−32] Considering that a supersaturated solution relieves
the metastable condition by forming a suitably sized aggregate to
achieve primary nucleation and recognizing that surface energies are
important in aggregate formation and growth, the convenient and systematic
manipulation of surface energies in heterogeneous primary nucleation
is potentially of significant utility in improving crystallization
outcomes.The promise of this platform approach derives from
the ubiquity
of a vessel (or substrate surface) to contain the liquid sample of
the solute to be crystallized; the recognition that this surface may
interact with the prenuclear solute aggregates in solution; and that
the surface energy modifications can be conveniently varied and systematically
produced with automated manufacturing methods to give a broad spectrum
of surface energies useful in crystal nucleation. By using engineered
surface energy modifications to induce nucleation without the need
to alter the screening chemistry, experimental workflow, or HTS equipment,
this slot-in approach to enhancing nucleation promises to add a meaningful
layer of variables that improve crystallization outcomes for drug
development, structure-based drug design, and manufacturing. This
communication presents the initial probe for function using surface
energy modifications to induce nucleation and reports reproducible
improvements in crystallization outcomes based on replicate investigations
of various APIs, proteins, organic solvents, aqueous media, surface
energy motifs, crystallization methods, form factors, and flat and
convex surface energy modifications.Table shows microscopy
images from the initial proof of concept studies with acetylsalicylic
acid (ASA; frequently used to study new crystallization techniques[25]), in which the crystals (shown as white specks)
form preferentially in the surface-energy-modified features as compared
to the random distribution on the unmodified control surfaces. For
the crystallization onset time studies of Table , solvent controls were used to rule out
effects from adventitious impurities or solids (e.g., microcrystalline
ASA, vessel surfaces, etc.) and surface controls (i.e., unmodified
soda-lime glass microscope slides) were used to isolate effects from
either the surface of the slides or the factory cut edges. For these
proof of concept studies, a microscope slide serving as a control
surface or one with a 20 mm surface-energy-modified nucleation site
array was immersed in ≈40 mL of 150 mg/mL ASA in 91% isopropyl
alcohol, the 120 mL vial sealed, and immediately quenched to 0 °C in
an ice/H2O bath inside a refrigerator maintained at 3 °C.
As reported in Table , the solvent controls showed no evidence of ASA crystallization
to at least 242 min, whereas the surface controls showed crystallization
at 118(91) min (alternatively 118 ± 91 min) on average. Analysis
of the crystallization onset time data for grids with 1.8, 0.6, and
0.5 mm square islands (i.e., G18, G6, and G5, respectively, in Table ) and concentric circles
(i.e., CC5; decrement of ≈0.5 mm between circles) shows an
average 56% reduction in crystallization onset times (n = 6) and supports an expanded probe of this approach to nucleation.
Table 1
Average Crystallization Onset Times
(min) for 150 mg/mL Acetylsalicylic Acid (ASA) in 91% Isopropyl Alcohol
at 0 °C for Solvent and Surface
Control Systems and for 20 mm Engineered Nucleation Features on Flat
Glass Surfaces Immersed in Solution
Avg = average.
esd = estimated standard deviation.
Avg = average.esd = estimated standard deviation.Table shows average
crystallization onset times for the protein thaumatin (n = 15) on 20 mm grid and circular surface energy modifications using
sitting drop vapor diffusion (see Supporting Information for details). The unmodified control surface produced thaumatin
crystals on average at 44(12) h, with the CC5 motif of concentric
circles producing little apparent reduction in crystallization time
with a similar value of 39(14) h. The grid-based surface energy modifications
gave progressively faster crystallization onset times of 37(14), 33(16),
and 32(15) h for G5, G6, and G18, respectively, affording a reproducible
maximum reduction of 27% in crystallization onset times for the G18
surface.
Table 2
Average Crystallization Onset Times
(h) for Thaumatin on 20 mm Engineered Nucleation Features at 22 °Ca
Protein solution:
20 mg/mL thaumatin
in 25 mM HEPES at pH 7.0. Precipitant solution: 0.5 M K/Na tartrate,
0.1 M sodium citrate at pH 6.3. A 10 μL total drop size with
1:1 ratio of protein:precipitant was used in sitting drop vapor diffusion.
Protein solution:
20 mg/mL thaumatin
in 25 mM HEPES at pH 7.0. Precipitant solution: 0.5 M K/Na tartrate,
0.1 M sodium citrate at pH 6.3. A 10 μL total drop size with
1:1 ratio of protein:precipitant was used in sitting drop vapor diffusion.Tables and 2 provide an
initial glimpse into how the different
surface energy modifications may impact crystallization of different
solutes; for example, the grid motif G18 shows the largest decreases
in crystallization onset times of 66% for the small molecule ASA and
27% for the protein thaumatin, whereas CC5 gives a 49% decrease for
ASA and just an 11% decrease in crystallization onset time for thaumatin.
While the latter is not compelling, the onset time for CC5 compares
favorably to that of the surface control and is a reflection of care
in the experimental approach. These data suggest that different surface
energy modifications may exhibit different nucleation behavior for
different solutes, and this is an important area of investigation
in our laboratories.Similarly, by analyzing the crystallization
onset times for the
protein bovinepancreatic trypsin (BPT; n = 17) in Table , it can be seen that
the surface controls produced crystals at 41(14) h and that the CC5
substrate again shows little improvement in crystallization onset
time at 41(13) h vs control. The grid motifs G5, G18, and G6 show
decreasing crystallization onset times of 34(16), 30(12), and 27(12)
h, respectively, and the surface energy profile of G6 produces the
largest overall reduction in crystallization onset times for BPT of
34%.
Table 3
Average Crystallization Onset Times
(h) for Bovine Pancreatic Trypsin (BPT) on 20 mm Engineered Nucleation
Features at 22 °Ca
Protein
solution: 20 mg/mL BPT
in 25 mM HEPES at pH 7.0, 10 mM CaCl2, and 10 mg/mL benzamidine-HCl.
Precipitant solution: 0.1 M (NH4)2SO4, 20% (w/v) PEG 8000. A 10 μL total drop size with 1:1 ratio
of protein:precipitant was used in sitting drop vapor diffusion.
Protein
solution: 20 mg/mL BPT
in 25 mM HEPES at pH 7.0, 10 mM CaCl2, and 10 mg/mL benzamidine-HCl.
Precipitant solution: 0.1 M (NH4)2SO4, 20% (w/v) PEG 8000. A 10 μL total drop size with 1:1 ratio
of protein:precipitant was used in sitting drop vapor diffusion.These promising preliminary
results with 20 mm surface energy modifications
and 10 μL drop sizes, which are comparatively large for structural
biology studies, led to the next prototype iteration resulting in
surface energy modifications of 2.5 mm to accommodate a more relevant
drop size of 2 μL. Figure shows crystals or groups of
crystals (blue circles) of BPT on the 2.5 mm surface energy motifs,
and it provides an example of the naming convention: multiplexed (M),
grid (G), concentric circle (CC), concentric square (CS), concentric
triangle (CT), and asterisk (AST), where any trailing digit is an
average (n = 3) distance between major features (peaks)
in the motif. Figure shows three separate crystallization trials for BPT in which one
or more crystals (in blue circles) is observed on all surfaces after
40 h. More importantly, Figure illustrates that the larger number of nucleation sites on
the engineered surfaces results in more crystals and that these crystals
are most often in contact with (i.e., adjoining or on top of) the
engineered nucleation features.
Figure 1
Sitting drop vapor diffusion crystallization
of bovine pancreatic
trypsin (BPT) on 2.5 mm surface energy modifications after 40 h at
22 °C. Protein drop: 20 mg/mL BPT in 25 mM HEPES at pH 7.0, 10
mM CaCl2, 10 mg/mL benzamidine-HCl. Precipitant drop: 0.1
M (NH4)2SO4, 20% (w/v) PEG 8000.
Total drop size of 2 μL with 1:1 ratio of protein/precipitant.
Sitting drop vapor diffusion crystallization
of bovinepancreatic
trypsin (BPT) on 2.5 mm surface energy modifications after 40 h at
22 °C. Protein drop: 20 mg/mL BPT in 25 mM HEPES at pH 7.0, 10
mM CaCl2, 10 mg/mL benzamidine-HCl. Precipitant drop: 0.1
M (NH4)2SO4, 20% (w/v) PEG 8000.
Total drop size of 2 μL with 1:1 ratio of protein/precipitant.The smaller footprint of the 2.5
mm nucleation site motifs allows
for their convenient organization into multiplexed arrays, as shown
in Figure for microscope
slides and various HTS plate formats for manual or automated crystallization
screening. Figure (right) also shows the variables examined in assessing the utility
of using surface energy modification to affect crystallization outcomes.
As shown, this probe for function is comparatively broad and is rigorous
in using replicate studies. In a boundary probe of the experimental
space, a series of experiments was conducted that migrated away from
flat form factors (Tables –3 and Figure ) to the convex external surface of a glass
capillary (Figure , bottom center). This boundary study also allowed for concurrent
testing of a microdomain thermal perturbation to induce nucleation
in a full immersion, batch crystallization technique. This microdomain
approach to cooling from the “interior of the solution”
while the bulk is held at a separate temperature (≈22 °C
in these studies) by virtue of a heat sink is one interesting approach
to overcoming protein solubility issues that arise during bulk cooling
protocols. Microdomain cooling effectively increases the supersaturation
ratio through localized cooling, and when performed in proximity to
a nucleation surface, it may promote nucleation at lower solute concentrations,
which is important in structural biology where the small quantities
of purified protein are often quite precious (e.g., membrane proteins). Figure shows the experimental
apparatus used in these preliminary studies, and results for ASA crystallization
from 40% ethanol are shown in Figure . Here, ASA crystals are evident on the borosilicate
glass capillary (left) having a linear array of surface energy nucleation
sites, as compared to the control surface (right). Table shows the results of replicate
quantitative studies (n = 7) for crystallization
onset times for ASA in 91% isopropyl alcohol using the apparatus shown
in Figure . These
data show a 47% reduction in crystallization onset times from 38 to
20 min compared to control, in rigorously controlled and replicated
studies. A comparison of the data in Table showing an acceleration in crystallization
onset times of 47% for ASA using convex surface energy modifications
and a microdomain cooling approach at 4 °C with the data of Table showing a 56% improvement
in crystallization onset times using flat surface energy modifications
and bulk cooling to 0 °C shows remarkably good agreement across
these very different form factors and cooling approaches.
Figure 2
Left: Examples
of surface energy modifications on various form
factors including microscope slides, vials, glass capillaries, and
96- and 384-well HTS plates for crystallization. Right: Variables
examined in challenging the approach.
Figure 3
Apparatus constructed to investigate nucleation and crystallization
using surface energy modifications on convex surfaces with microdomain
cooling. A single 20 AWG Cu wire is fashioned into two adjacent probes
and is attached to a thermoelectric device so that the thermal effect
for the experimental and control surfaces is identical.
Figure 4
Left: Acetylsalicylic acid (ASA) crystallization from
40% ethanol
on a borosilicate glass capillary with a linear array of surface-energy-modified
nucleation sites. Right: Unmodified capillary as control surface.
Image taken at 120 min through a H2O heat sink at 22 °C.
Table 4
Average Crystallization
Onset Times
(min) for Acetylsalicylic Acid (ASA) in 91% Isopropyl Alcohol in Contact
with Unmodified Capillaries as Control Surfaces and Capillaries Having
a Linear Array of 19 Hemicircumferential Nucleation Motifsa
Each capillary
was cooled to
4 °C using the device in Figure , while the vials were immersed in a H2O
heat sink at 22 °C.
Left: Examples
of surface energy modifications on various form
factors including microscope slides, vials, glass capillaries, and
96- and 384-well HTS plates for crystallization. Right: Variables
examined in challenging the approach.Apparatus constructed to investigate nucleation and crystallization
using surface energy modifications on convex surfaces with microdomain
cooling. A single 20 AWG Cu wire is fashioned into two adjacent probes
and is attached to a thermoelectric device so that the thermal effect
for the experimental and control surfaces is identical.Left: Acetylsalicylic acid (ASA) crystallization from
40% ethanol
on a borosilicate glass capillary with a linear array of surface-energy-modified
nucleation sites. Right: Unmodified capillary as control surface.
Image taken at 120 min through a H2O heat sink at 22 °C.Each capillary
was cooled to
4 °C using the device in Figure , while the vials were immersed in a H2O
heat sink at 22 °C.Figure shows a
time sequence in which the appearance of hen egg white lysozyme crystals
became evident (white circles) with microscopic digital image capture,
and these crystals largely formed and settled on the side of the capillary
having the hemicircumferential surface energy modifications. The appearance
of lysozyme crystals was consistently 30% faster (n = 10) on the surface-energy-modified capillaries
cooled to 4 °C as compared to controls.[33] This microdomain cooling technique is under continued development
as a means of locally increasing supersaturation to facilitate nucleation
of proteins and other molecules with challenging solubilities and/or
crystallization behaviors.
Figure 5
Time sequence showing crystallization of lysozyme
on control surfaces
(top) and capillaries with hemicircumferential surface energy modifications
(bottom) using the apparatus in Figure .
Time sequence showing crystallization of lysozyme
on control surfaces
(top) and capillaries with hemicircumferential surface energy modifications
(bottom) using the apparatus in Figure .The use of physical surface
energy modifications to create a conveniently
and systematically controlled spectrum of surface energies to facilitate
nucleation in bulk solutions or in drops has been investigated in
carefully controlled and replicated studies. This communication and
the associated reports[33,34] discuss several tangible benefits
of using surface energy modifications to induce crystal nucleation:For ASA as a model
small molecule
API, bulk and microdomain cooling using very different approaches
and form factors (i.e., flat vs convex nucleation features) gave good
agreement and an average 52(4)% reduction in crystallization onset
times as compared to control surfaces.For the proteins thaumatin and BPT,
maximum decreases in crystallization onset times of 27% and 34%, respectively,
were observed as was an increase in the number of crystals formed
per experiment, many of which formed on the surface-energy-modified
nucleation arrays.Microdomain cooling in proximity to
engineered surface energy modifications was shown to accelerate nucleation
and appearance of crystals for ASA and lysozyme by 47% and 30%, respectively.Systematic surface energy modifications
can have beneficial effects
on nucleation and crystallization outcomes, as demonstrated in this
comparatively broad and rigorous probe for function that includes
carefully controlled studies and n = 6–26 replicate crystallization trials for
different small molecule APIs, proteins, organic solvents, aqueous
conditions, surface energy modifications, crystallization methods,
form factors, and flat and convex nucleation features. Given that
nucleation relieves the metastable condition of supersaturation and
that solid surfaces in contact with supersaturated solutions are known
to reduce the energies needed to achieve nucleation,[1,11,19−21] the use of
surface energy modifications applied to the vessel surface may be
a promising new tool for use in small molecule API solid form and
polymorph screening; structural biology in support of structure-based
drug design; and potentially in improving the productivity and robustness
of manufacturing-scale crystallization processes. Future studies with
a more diverse set of APIs and proteins will allow a more quantitative
assessment of the breadth and benefits of using surface energy modifications
to rationally impact nucleation and improve crystallization success
rates.
Authors: Tan Pham; Denton Lai; David Ji; Wirote Tuntiwechapikul; Jonathan M Friedman; T Randall Lee Journal: Colloids Surf B Biointerfaces Date: 2004-04-01 Impact factor: 5.268
Authors: Konstantin O Zamuruyev; Hamzeh K Bardaweel; Christopher J Carron; Nicholas J Kenyon; Oliver Brand; Jean-Pierre Delplanque; Cristina E Davis Journal: Langmuir Date: 2014-08-12 Impact factor: 3.882
Authors: Sahir Khurshid; Lata Govada; Hazim F El-Sharif; Subrayal M Reddy; Naomi E Chayen Journal: Acta Crystallogr D Biol Crystallogr Date: 2015-02-26