Preservation of the integrity of macromolecular higher-order structure is a tenet central to achieving biologic drug and vaccine product stability toward manufacturing, distribution, storage, handling, and administration. Given that mRNA lipid nanoparticles (mRNA-LNPs) are held together by an intricate ensemble of weak forces, there are some intriguing parallels to biologic drugs, at least at first glance. However, mRNA vaccines are not without unique formulation and stabilization challenges derived from the instability of unmodified mRNA and its limited history as a drug or vaccine. Since certain learning gained from biologic drug development may be applicable for the improvement of mRNA vaccines, we present a perspective on parallels and contrasts between the emerging role of higher-order structure pertaining to mRNA-LNPs compared to pharmaceutical proteins. In a recent publication, the location of mRNA encapsulated within lipid nanoparticles was identified, revealing new insights into the LNP structure, nanoheterogeneity, and microenvironment of the encapsulated mRNA molecules [Brader et al. Biophys. J. 2021, 120, 2766]. We extend those findings by considering the effect of encapsulation on mRNA thermal unfolding with the observation that encapsulation in LNPs increases mRNA unfolding temperatures.
Preservation of the integrity of macromolecular higher-order structure is a tenet central to achieving biologic drug and vaccine product stability toward manufacturing, distribution, storage, handling, and administration. Given that mRNA lipid nanoparticles (mRNA-LNPs) are held together by an intricate ensemble of weak forces, there are some intriguing parallels to biologic drugs, at least at first glance. However, mRNA vaccines are not without unique formulation and stabilization challenges derived from the instability of unmodified mRNA and its limited history as a drug or vaccine. Since certain learning gained from biologic drug development may be applicable for the improvement of mRNA vaccines, we present a perspective on parallels and contrasts between the emerging role of higher-order structure pertaining to mRNA-LNPs compared to pharmaceutical proteins. In a recent publication, the location of mRNA encapsulated within lipid nanoparticles was identified, revealing new insights into the LNP structure, nanoheterogeneity, and microenvironment of the encapsulated mRNA molecules [Brader et al. Biophys. J. 2021, 120, 2766]. We extend those findings by considering the effect of encapsulation on mRNA thermal unfolding with the observation that encapsulation in LNPs increases mRNA unfolding temperatures.
The spectacular advent
of mRNA vaccines as a rapid response to
the COVID-19 pandemic has ushered in a new front line in vaccinology.
These vaccines combine the informational sophistication of the mRNA
molecule with the physicochemical architecture of lipid nanoparticles
to create a tunable drug delivery platform with great potential for
broadly versatile medical applications.[2−5] Understandably, the COVID-19 pandemic has
focused much attention on the practical details of vaccine shelf life,
storage conditions, supply, and distribution,[6] while also highlighting that, well prior to this pandemic, poor
vaccine thermostability[7,8] coupled with supply chain logistics
challenges[9] had already been regarded as
an Achilles heel of efforts to globally vaccinate against deadly infectious
diseases. The goal of achieving more robust vaccine products connects
directly to the understanding of the underlying molecular interactions
and ultimately translating this knowledge into rational formulation
design strategies.[10] These connections
have been well-developed for therapeutic proteins; however, for mRNA
vaccines, structural details of the conformational state and physicochemical
environment of the mRNA within the lipid nanoparticle (LNP) formulation
are only beginning to emerge. The central drug delivery challenge
of mRNA is more formidable than for proteins because the mRNA molecule
must be delivered intracellularly whereas pharmaceutical proteins
remain limited to druggable targets outside the cell. An addition
to this challenge is the intrinsic rapid biodegradability of mRNA.
Although this is a favorable attribute from a safety and pharmacokinetic
perspective,[11] unfortunately, it also confers
susceptibility to degradation in vitro. A more detailed understanding
of the pathways specifically relevant to mRNA pharmaceutical instability
is currently emerging.[12] Similarly, although
lipid nanoparticles have been studied as drug carriers for about 30
years,[13] the first approved product using
this technology occurred only recently with ONPATTRO (patisiran) in
2018.[14]To create perspective, it
is intriguing to consider the current
state of mRNA biomedical technology relative to therapeutic protein
biotechnology and the advances made preceding and following FDA’s
approval of the first recombinant DNA drug product, human insulin
(Humulin), in 1982.[15] This milestone was
well preceded by the crystal structure of pig insulin in 1969[16] with an elegant description of the underlying
factors governing correct protein folding well-articulated by the
early 1970s.[17] A pathway to improved protein
pharmaceuticals then unfolded (no pun intended), leveraging regulatory
precedent and an understanding of the underlying structure and folding
to create improved sequences conferring greater pharmaceutical stability
and/or improved therapeutic properties.[18] The approval of Humalog in 1996 provided a striking example of the
latter, showing how even a subtle amino acid sequence modification
could be engineered to dramatically alter insulin pharmacokinetics
via a physicochemical mechanism,[19,20] thereby addressing
a therapeutic need. These biomedical milestones stand on the shoulders
of historic advancements in recombinant DNA technology, protein engineering,
and structural biology at atomic resolution serving to emphasize that
the route to better biomedical products is based firmly on understanding
the fundamental interrelationships among higher-order structure, biological
activity, and biomedical implementation, aka the molecular pharmaceutics.
The
RNA Molecule
mRNA was discovered in 1961, and an indication
of its biomedical
potential was demonstrated in 1990 when protein production was shown
from reporter gene mRNAs injected into mice.[21] Historically, structural studies of RNA in the 1960s were part of
a frenzy to understand their function in decoding genetic information.
The ensuing discovery of catalytic RNA in the early 1980s was a major
milestone in RNA science with the recognition that its 3-dimensional
structure is intrinsically related to its function.[22,23] Up until that time, X-ray crystallographic studies of RNA had focused
predominantly on transfer-RNA (due in part to limitations of preparative
methodologies for adequate quantities of other RNA types) and then
ribosomal-RNA motivated by the fascination with its central role in
protein biosynthesis.[24] Early therapeutic
proteins were more convenient to study. As relatively stable, naturally
occurring molecules, they could be isolated from animal or human tissues
in large quantities. For example, insulin could be purified in gram
quantities and had been used therapeutically since the 1920s. Large-scale
global production was achieved within a few years of its discovery,
and commendably, advanced pharmaceutical formulations had been developed
by the 1930s.[25] The biomedical potential
of insulin and the full knowledge of its 3-dimensional structure had
thus been thoroughly established well before its launch as the first
biosynthetic human protein drug in 1982. In fact, structurally, biochemically,
medically, and pharmaceutically, insulin was one of the most thoroughly
studied protein molecules in history by that time.In contrast
to proteins, the concept of mRNA as a drug or vaccine
is relatively recent, one that faced formidable drug delivery challenges
and was not preceded by a long history of applicable pharmaceutical
sciences research. A 3-dimensional structure of our mRNA molecule
is not available, and an understanding of the interrelationships among
higher-order structure, protein translational efficiency, and chemical
stability is only beginning to emerge.[26−30] Indeed, it is amusing to note that as late as the
mid 1990s RNA scientists practically lamented the reverence that protein
scientists held toward the delicacy of higher-order structure,[31] apparently reflecting the more contemporary
appreciation of RNA folding. mRNAs are large molecules (typically
≈1000–4000 nucleotides): three nucleotide units code
for each amino acid of the protein for which they encode, and each
nucleotide has a mass of about 330 Da versus the average amino acid
mass of 110 Da. The incorporation of ribose sugars into RNA as opposed
to deoxyribose sugars for DNA makes RNA more suitable for its short-lived
purpose in vivo,[32] whereas DNA (the information
storage molecule) is highly stable to the extent of boasting an impressive
521-year half-life.[33] Chemical modifications
to the mRNA molecule including cap structures and modified nucleosides
have played a key role in overcoming challenges of immunogenicity,
achieving prolonged stability and potent, accurate protein expression
in vivo.[5,34] These advancements have been central to
enabling exogenous mRNA delivery; however, the achievement of the
ideal target product profiles for mRNA vaccines and therapeutics will
require further innovative approaches.mRNA is a single stranded
molecule that can form double stranded
structures by folding over on itself, forming hairpin stem-loops and
pseudoknots stabilized by the intramolecular hydrogen bonds formed
through complementary pairing of contiguous bases. These secondary
structures fold into 3-dimensional tertiary structures as illustrated
in Figure .
Figure 1
Representations
of RNA higher-order structure showing how secondary
structures formed from complementary base pairing fold into 3-dimensional
tertiary structures. (A) RNA secondary structure; (B) 3-dimensional
tertiary structure showing water and ions; (C) the incorporation of
specific secondary structural elements into the tertiary structure.
Figure adapted from Dawson, W. K.; Bujnicki, J. M. Computational modeling
of RNA 3D structures and interactions. Curr. Opin. Struct.
Biol.201637, 22 (ref (90)) under the terms of creative
Commons license http://creativecommons.org/licenses/by/4.0/.
Representations
of RNA higher-order structure showing how secondary
structures formed from complementary base pairing fold into 3-dimensional
tertiary structures. (A) RNA secondary structure; (B) 3-dimensional
tertiary structure showing water and ions; (C) the incorporation of
specific secondary structural elements into the tertiary structure.
Figure adapted from Dawson, W. K.; Bujnicki, J. M. Computational modeling
of RNA 3D structures and interactions. Curr. Opin. Struct.
Biol.201637, 22 (ref (90)) under the terms of creative
Commons license http://creativecommons.org/licenses/by/4.0/.RNA is a polyanion with complex conformational and charge
interaction
behaviors in solution. The negative charges on the chain repel each
other causing the RNA molecules to stretch out in solution. However,
this stretching lowers the conformational entropy so that the molecule
arrives at an optimum between minimizing the repulsive potential of
like charges by stretching out as much as possible while keeping the
entropy sufficiently positive. In the presence of an electrolyte,
the charges will be shielded, and the molecule will relax electrostatically
and shrink in size. Consequently, the folding of RNA into stable tertiary
structures is extremely sensitive to counterions[35] or, in the parlance of the pharmaceutical scientist, expected
to be highly formulation dependent. Although Ca2+ and Mg2+ play important roles in the stabilization of RNA folding
in vivo by participating in the ionic microenvironment as diffuse
ions or directly bound at high affinity sites, divalent cations also
promote cleavage of RNA.[36,37] Large RNA molecules
in solution are generally considered to be more extended and diffuse
than globular proteins but still adopt diversely complex sequence-dependent
higher-order structures.[38] While much progress
has been made in the prediction of the secondary structure from the
sequence, the proverbial “rugged energy landscape” makes
the prediction of the tertiary structure a formidable problem, especially
for the very large mRNA molecule.[39] Both
proteins and RNA exhibit secondary and tertiary structures dependent
on the primary sequence; however, protein higher-order structures
are driven primarily by the burial of the hydrophobic side chains
whereas RNA folding is a hierarchical process driven predominantly
by base stacking, hydrogen bonding, and electrostatic stabilization.[40] Although there is a superficial parallel between
protein- and RNA-higher-order structures, the analogy breaks down
upon deeper consideration of structure–function interrelationships.
For mRNA specifically, Crick’s classic metaphor of mRNA as
an audio tape running through the reading head of a tape recorder
emphasizes the significance of the primary sequence as the central
basis of its function, carrying the genetic code from DNA to ribosomes
that unwind the folded mRNA molecule to decode the message. In contrast,
it was the 3-dimensional folded structure of proteins that historically
held such fascination and is most associated with launching the field
of structural biology. It follows that the preservation of the integrity
of a therapeutic protein’s folded structure has always been
synonymous with achieving good pharmaceutical stability, whereas fundamental
details of how mRNA folding relates to its biological activity are
still emerging.[30]The comparison
of the crystallization behavior highlights the physicochemical
differences. The crystallization process is a form of molecular recognition,
making its manifestation a visible outcome of the underlying structural
and interfacial phenomena. In a comparison of proteins with RNA molecules,
the differing chemical nature of the repeating units in these two
types of biopolymers results in quite different propensities for molecular
ordering and crystallization. Many pharmaceutical proteins crystallize
well because the molecular characteristics and solution conditions
that favor crystallization also favor pharmaceutical integrity and
stability (purity, chemical homogeneity, conformational homogeneity,
and solubility). Indeed, their crystallization conditions can provide
useful clues for the identification of optimal pharmaceutical formulation
conditions because the crystallization process is sensitive to multiple
pharmaceutical quality attributes.[41] In
contrast, large RNA molecules are highly dynamic and are characterized
by extensive conformational heterogeneity with poorly differentiated
molecular surfaces that offer few tertiary contacts to favor lattice
formation. The very large size of mRNA molecules further compounds
the difficulty of achieving a well-ordered crystal lattice, as evident
from the description by Gopal et al. of the long RNA molecule in solution
as “a statistical object whose properties are derived from
an ensemble of possible structures”.[42] Although many RNA structures have been reported in the structural
biology literature and open databases, these predominantly correspond
to comparatively short sequences, tRNA, and/or RNA in complexes with
proteins.[43] In contrast, many therapeutic
proteins, including monoclonal antibodies, have X-ray crystal structures
defining their 3-dimensional structures. Prospects for mRNA structures
with atomic level precision are poor because, in practice, NMR and
X-ray crystallographic methods are restricted to relatively small
sequences (<≈200 nucleotides).[44]
Lipid Nanoparticles for mRNA Delivery
Due to their size,
polyanionic nature, and hydrophilicity, the
intracellular delivery of mRNA molecules cannot generally rely on
passive diffusion across cell membranes. Furthermore, nucleic acids
are rapidly degraded by endogenous nucleases in physiological fluids.
To overcome these challenges, LNPs incorporating ionizable lipids
have been developed as delivery vehicles for siRNA and mRNA, serving
both to protect the delicate cargo from degradation in vivo and to
enable delivery into the cell. LNPs for mRNA delivery generally comprise
a zwitterionic phospholipid, cholesterol, a polyethylene glycol (PEG)
lipid, and an ionizable lipid.[45,46] Engineering the lipid
structure[47] and particle surface has thus
been pursued as a strategy to enhance cellular uptake and endosomal
escape[48,49] while specific nanostructural features of
the LNP, such as nonlamellar lipid phases, have also been suggested
to affect delivery efficiency.[50] LNP interfacial
interactions with the cell membrane initiate the internalization of
the mRNA; then, inside the cell, the more acidic environment protonates
the ionizable lipid, reversing the electrostatic interactions to release
the RNA cargo for translation and subsequent protein expression. This
is of course an oversimplified description, and the reader is directed
to some excellent recent reviews that address these intracellular
aspects in more detail.[45,51] The LNP morphology,
lipid packing, and microenvironment of the encapsulated mRNA are thus
plausibly connected to the delivery efficiency, emphasizing the central
significance of higher-order structure associated with both the mRNA
and LNP.The challenges of LNP preparative scale-up and large-scale
processing
represent another interesting point of distinction between mRNA-vaccines
and biologic drugs. While LNPs may be prepared at bench-scale using
pipets and simple manual mixing,[52] their
cGMP scale-up for clinical/commercial use employs finely controllable
rapid-mixing platforms involving multiple processing steps.[53,54] In contrast, the large-scale production of many biologic drugs can
be based on relatively simple thaw–filter–fill drug
product production processes. On the other hand, the operational simplicity
of the drug product is offset by the complexity of biologic drug substance
production processes, which are based on microbial fermentation or
mammalian cell culture. mRNA is produced synthetically at large scale
using the in vitro transcriptase reaction.[55]Although cryo-EM images of mRNA-LNPs reported in the literature
often appear as relatively featureless gray circles, we were intrigued
by the diversity of mRNA-LNP morphologies in some published images
where spherical and nonspherical morphologies are apparent, including
blebs (cavernous protrusions) of varying size, sometimes showing resolved
striations indicative of annular arrangements.[56−58] The literature
indicates there are many processing and compositional factors that
can influence the outcome of the nanoprecipitation reaction, and it
is also apparent that the chemical nature of the component lipids
can affect the LNP morphology,[48] even to
the extent of producing distinctive faceted particle geometries.[50] The siRNA-LNP literature reflects a fairly concordant
description of the LNP assembly supported by biophysical studies.
Presumably, due to their small size (≈20 nucleotides) and double
stranded character, the siRNA molecules can be more readily accommodated
within a structural arrangement directed predominantly by preferences
of the lipids. The much larger mRNA molecules evidently require a
different accommodation. A direct comparison of LNP formation using
siRNA versus mRNA under the same LNP preparative scheme showed that
mRNA formed LNPs with very large bleb features, whereas the siRNA-LNP
counterpart were devoid of these.[56] When
one recognizes that cryo-EM mass density in the blebs can be assigned
to mRNA, it follows that the nature of the encapsulated RNA molecule
itself can influence LNP morphology and the degree of lipid association.
Clearly, the encapsulation of large mRNA molecules is more complex
than common representations of the LNP as a sphere with RNA lipid-bound
in the core.[59] On the basis of our recent
study pinpointing the location of mRNA within the LNP,[1] we suggest that LNPs may be better represented as a continuum
of states corresponding to varying degrees of mRNA-lipid association
as shown in Figures and 3.
Figure 2
Cryo-EM characterization of the representative
mRNA-LNP preparations.
When the mRNA was highlighted with a permeating cationic dye, it became
evident that LNPs may form morphological arrangements corresponding
to different states of mRNA-lipid association. Panels A and B show
extremes of highly spherical versus nonspherical morphologies where,
in the latter, mRNA is dissociated from the solid lipid body of the
nanoparticle to reside in a bleb compartment. Panel C shows the significant
degree of nanoheterogeneity that can be present including states of
mRNA-lipid association intermediate between panels A and B. Figure
adapted from Brader et al. Encapsulation state of messenger RNA inside
lipid nanoparticles. Biophys. J.2021, 120 (14), 2766–2770 (ref (1)) under the terms of Creative
Commons license http://creativecommons.org/licenses/by/4.0/.
Figure 3
Schematic representation of mRNA-LNP morphologies. At the far left,
a spherical particle with mRNA and the lipid fully associated is depicted.
The formation of a bleb involves the creation of a protrusion on the
LNP characterized by a darkened, thicker periphery consistent with
enrichment of the DSPC as the most mass dense component present. This
aqueous compartment can occur to varying degrees and may or may not
be occupied by mRNA (blue depicts aqueous; mottled surface depicts
mRNA). In the extreme of dissociation, at right, mRNA-loaded or unloaded
liposomes may also be formed as minor components.
Cryo-EM characterization of the representative
mRNA-LNP preparations.
When the mRNA was highlighted with a permeating cationic dye, it became
evident that LNPs may form morphological arrangements corresponding
to different states of mRNA-lipid association. Panels A and B show
extremes of highly spherical versus nonspherical morphologies where,
in the latter, mRNA is dissociated from the solid lipid body of the
nanoparticle to reside in a bleb compartment. Panel C shows the significant
degree of nanoheterogeneity that can be present including states of
mRNA-lipid association intermediate between panels A and B. Figure
adapted from Brader et al. Encapsulation state of messenger RNA inside
lipid nanoparticles. Biophys. J.2021, 120 (14), 2766–2770 (ref (1)) under the terms of Creative
Commons license http://creativecommons.org/licenses/by/4.0/.Schematic representation of mRNA-LNP morphologies. At the far left,
a spherical particle with mRNA and the lipid fully associated is depicted.
The formation of a bleb involves the creation of a protrusion on the
LNP characterized by a darkened, thicker periphery consistent with
enrichment of the DSPC as the most mass dense component present. This
aqueous compartment can occur to varying degrees and may or may not
be occupied by mRNA (blue depicts aqueous; mottled surface depicts
mRNA). In the extreme of dissociation, at right, mRNA-loaded or unloaded
liposomes may also be formed as minor components.
Conformational
Stability and Pharmaceutical Stability
The lipidic environment
of encapsulated mRNA involves several chemical
components, creating the possibility that each pharmaceutical raw
material may adversely affect the mRNA stability profile.[12] Structural effects of the encapsulation itself
on the mRNA 3-dimensional fold may also conceivably influence stability
by exposing or burying labile regions. The mRNA molecule within the
LNP is thus expected to possess a distinct stability profile relative
to naked RNA. It is worth emphasizing at this point that the term
“stability” is often used in different scientific contexts
across the pharmaceutical sciences and biological sciences fields.
It has been described basically as the potential of a pattern to survive
over time,[60] and in the context of a biological-based
medicinal product, the relevant pattern may be categorized broadly
as either conformational or compositional. Denaturation, unfolding,
self-association, and aggregation relate to the former, whereas processes
creating new chemical entities such as cleavage, enzymatic degradation,
oxidation, and covalent adducts[12] are examples
of the latter. The preservation of correct higher-order structures,
specifically secondary, tertiary, and quaternary structures, represents
a central focus of biologic product development and characterization[61] for which the close connection between conformational
stability and chemical stability is well recognized.[62] Interfacial stresses associated with large-scale production,
filling, shipping, storage, handling, and administration create formidable
challenges to preserving these delicate higher-order structures necessary
for biological activity.[63] Signatures of
thermal unfolding can thus provide some basis for understanding how
pharmaceutical conditions impact the intrinsic structural stability
with a view to identify solution conditions robust to large-scale
processing and pharmaceutical stresses while also enabling a convenient
comparison of sequence variants in discovery phases of drug development.[64] A prediction of the shelf life of proteins from
accelerated data remains largely aspirational, nevertheless, gaining
predictive insights into the overall pharmaceutical stability of formulated
drug products by screening thermal unfolding signatures featured prominently
in protein developability workflows within the biotechnology industry.[65−67] Similarly, there is evidence that the secondary structure affects
the chemical stability of RNA.[68] We were
interested in exploring the impact of encapsulation on the thermal
folded stability of the mRNA molecule with a view to understand its
potential relevance to pharmaceutical stability.
Thermal Unfolding
Thermal melting techniques for RNA are well-developed and have
been applied extensively to studying nucleic acid folding and stability.[69] These approaches utilize optical or calorimetric
readouts to detect conformational change as the molecule unfolds.
Much historical impetus for this work has come from the goal of understanding
biologically relevant conformational transitions, as these occur via
breakage and formation of base pairing interactions. The thermal stability
of secondary structural elements in mRNA has received additional attention
recently due to emerging evidence that this attribute relates to actual
function (protein expression).[27,70] We applied differential
scanning calorimetry (DSC)[66] to a free
mRNA to produce the thermogram shown in Figure A.
Figure 4
Differential scanning calorimetry thermograms:
(A) an unencapsulated
mRNA; (B) same mRNA encapsulated in LNP, both in 20 mM Tris, 8% sucrose,
and pH 7.4 buffer; (C) bovine serum albumin in 5 mM sodium citrate,
pH 6.5 buffer; (D) mRNA-LNP sample from (B) reheated (after it had
been heated to 95 °C and then cooled back to room temperature).
In each panel, the experimental data is shown as the black line together
with the mathematical fit in red. Gaussian components of the fit are
shown as a color gradient together with the midpoint temperatures
of each transition. Data were recorded using a MicroCal PEAQ-DSC capillary
differential scanning microcalorimeter (Malvern-Panalytical, Malvern,
United Kingdom) with a scanning rate of 1.5 °C/min.
Differential scanning calorimetry thermograms:
(A) an unencapsulated
mRNA; (B) same mRNA encapsulated in LNP, both in 20 mM Tris, 8% sucrose,
and pH 7.4 buffer; (C) bovine serum albumin in 5 mM sodium citrate,
pH 6.5 buffer; (D) mRNA-LNP sample from (B) reheated (after it had
been heated to 95 °C and then cooled back to room temperature).
In each panel, the experimental data is shown as the black line together
with the mathematical fit in red. Gaussian components of the fit are
shown as a color gradient together with the midpoint temperatures
of each transition. Data were recorded using a MicroCal PEAQ-DSC capillary
differential scanning microcalorimeter (Malvern-Panalytical, Malvern,
United Kingdom) with a scanning rate of 1.5 °C/min.A complex thermogram requiring multiple Gaussian components
to
produce an adequate fit indicative of a complex thermal unfolding
pathway is evident. As an illustrative comparator, we also recorded
the DSC of bovine serum albumin (BSA), a “model globular protein”
(Figure C). BSA exhibits
a much simpler thermal profile even though its 3-dimensional structure
comprises 3 domains containing significant proportions of an α-helix,
β-sheet, and random coil.[71]Figure B shows the DSC signature
of the same mRNA formulated as LNPs, revealing that significant changes
in the thermal profile occurred together with an overall shift of
the mRNA signal to higher temperatures. The data of Figure A,B show that, unencapsulated,
the mRNA thermogram required 7 Gaussian fitting components, whereas
encapsulated, the profile could be fit with only 2. When the mRNA-LNP
sample corresponding to Figure B was rescanned after cooling back down to room temperature,
the thermogram shown in Figure D was obtained, which is different from both free mRNA and
mRNA in LNP, exhibiting transitions that have shifted to lower temperature
relative to mRNA in LNP. This again suggests a protective effect of
encapsulation within the LNP that is abolished when the LNP structure
is denatured by heat. DSC unfolding of free mRNA is characterized
by the existence of many closely spaced and rather sharp transitions,
probably corresponding to many similar, but different size, structural
elements. When encapsulated in the LNP, those structural elements
are transformed into a smaller number of more stable “superstructures”.To further evaluate the DSC results using a different biophysical
technique, we applied circular dichroism (CD) spectroscopy, which
can be applied to the characterization of the conformation of nucleic
acids in solution.[72] CD spectra of nucleic
acids are mostly dependent on the sequence and stacking geometry of
the bases, and in the case of short RNA sequences, it is possible
to distinguish A-form, B-form, and Z-form helices.[73] The CD spectrum of mRNA at 25 °C, shown in Figure A, is qualitatively
indicative of the A-form helix with two negative bands (210 and 295
nm) and one positive band (265 nm). This profile is similar to spectra
reported previously for mRNA and tRNA.[74,75] CD spectra
of this mRNA recorded at 5 °C temperature increments from 25
to 95 °C are also shown in Figure A. It is apparent that the spectrum changes in a complex
way with different wavelength regions shifting relative to one another,
a tell-tale sign that the effect of heating is not simply to produce
a change in the proportions of two states (folded and unfolded). Instead,
the result suggests a complex mix involving multiple conformations.
This interpretation is also apparent from monitoring the CD change
at a series of specific wavelength regions corresponding to the CD
bands, each of which resulted in distinctly different unfolding trajectories
(Figure B). We infer
that different regions of the mRNA molecule are affected by heat in
unique ways, and as a result, the unfolding of these regions occurs
along different pathways. This type of interpretation has been postulated
previously from CD melt experiments on RNA.[76]
Figure 5
(A)
Circular dichroism spectra of mRNA recorded on a Jasco J1500
spectrometer at successively increasing temperatures of 5 °C
increments from 25 to 95 °C. (B) Thermal unfolding trajectories
measured from integrated areas of the three wavelength regions indicated,
which correspond to distinct CD spectral bands. (C) CD spectra of
mRNA-LNP recorded at successively increasing temperatures in 5 °C
increments from 25 to 95 °C. (D) Thermal unfolding of mRNA measured
by monitoring the CD spectral area in the region of 264–268
nm. Shown in blue is the unfolding curve of free mRNA (in buffer).
The red data corresponds to the unfolding trajectory of the same mRNA
encapsulated in LNP. The gray curve corresponds to the same mRNA-LNP
sample cooled from 95 °C and then heated again from 25 °C.
Experimental averages and standard deviations are based on 3 independent
experiments. Normalized data, y, were fit with the
Hill equation, y = 1/[1 + (Tm/T)Hill] where the superscript
“Hill” refers to the Hill coefficient. Tm and Hill coefficient values are presented in Table .
(A)
Circular dichroism spectra of mRNA recorded on a Jasco J1500
spectrometer at successively increasing temperatures of 5 °C
increments from 25 to 95 °C. (B) Thermal unfolding trajectories
measured from integrated areas of the three wavelength regions indicated,
which correspond to distinct CD spectral bands. (C) CD spectra of
mRNA-LNP recorded at successively increasing temperatures in 5 °C
increments from 25 to 95 °C. (D) Thermal unfolding of mRNA measured
by monitoring the CD spectral area in the region of 264–268
nm. Shown in blue is the unfolding curve of free mRNA (in buffer).
The red data corresponds to the unfolding trajectory of the same mRNA
encapsulated in LNP. The gray curve corresponds to the same mRNA-LNP
sample cooled from 95 °C and then heated again from 25 °C.
Experimental averages and standard deviations are based on 3 independent
experiments. Normalized data, y, were fit with the
Hill equation, y = 1/[1 + (Tm/T)Hill] where the superscript
“Hill” refers to the Hill coefficient. Tm and Hill coefficient values are presented in Table .
Table 1
Transition Midpoints (Tm) and Hill Coefficients (Hill) Obtained from the CD Data
at 3 Spectral Bands Shown in Figure
CD spectral
band
208–212 nm
264–268 nm
294–298 nm
sample
Tm (°C)
Hill
Tm (°C)
Hill
Tm (°C)
Hill
free mRNA
53.0 ± 0.2
–6.3 ± 0.4
58.4 ± 0.8
–6.2 ± 0.1
49.6 ± 0.5
–9.2 ± 0.3
mRNA in LNP
71 ± 1
–11 ± 1
60.7 ± 0.4
–5 ± 1
mRNA in LNP reheated
64 ± 3
–6.7 ± 0.7
63 ± 4
–11 ± 6
The effect of encapsulation on the thermal melting of mRNA was
also characterized using the CD signal. The CD spectrum of encapsulated
mRNA recorded at 5 °C increments is shown in Figure C. From these spectra, the
ellipticity of the 264–268 nm region was monitored upon heating
(thereby avoiding interference from cholesterol CD, which coincides
with the 208–212 nm band). The comparison of encapsulated versus
free mRNA showed a similar effect to the DSC results (Figure ) with the thermal unfolding
profile shifted to significantly higher temperatures as a result of
encapsulation. Intriguingly, when the heated mRNA-LNP solution was
cooled to room temperature and then reheated, the resulting mRNA profile
had shifted significantly to become much more comparable to the melt
of the unencapsulated mRNA. This result suggests that it is the specific
nanostructured encapsulation state (which was destroyed upon heating
to 95 °C) that enhances mRNA folded stability.For proteins,
the assignment of CD bands to specific secondary
structural elements has been well-established on the basis of the
far-UV CD of the peptide bond.[77] The determination
of the protein structure from the CD spectra is possible because the
far-UV CD arises from the intrinsic CD of the protein backbone. In
contrast, much of the nucleic acid CD originates from the stacking
geometry and sequence-dependent base pair content, making the relationship
between the nucleic acid secondary structure and CD spectral shape
more convoluted than is the case for proteins, especially in the case
of a large single-stranded mRNA. With this caveat, we offer some interpretations
of the spectral features present in Figure A. Published experimental results indicate
that the strong negative band observed at 210 nm is the result of
nearest-neighbor interactions and base stacking.[78,79] Studies on DNA have found that a particularly large spectral effect
originates from guanine–guanine stacking, which makes an important
contribution to the formation of helix duplexes, leading to the strong
positive band at 265 nm.[80] In general,
a positive band in the 260–280 nm region suggests the formation
of a right-handed helix.[72] A dominant positive
band at 260 nm and a sharp negative band at 210 nm characterize the
CD spectra of A-form helix RNA.[81] The weak
band observed at 295 nm has been identified as the result of the nearest-neighbor
interactions.[78] In thermal melting experiments,
CD changes are primarily caused by base destacking, leading to the
loss of interaction between neighboring bases, which manifests as
a decreased magnitude of CD bands. In the free mRNA spectrum of Figure A, the most thermally
susceptible region appears to be the 295 nm band followed by the 210
nm band. A simplistic interpretation, the unstacking of the single
weakest neighboring bases, is the first event observed during mRNA
heating (295 nm), leading to further unzipping of longer sequences
observed as melting at 210 nm. These events lead into a major helix
to coil transition, affecting the whole double helical structure evident
at 265 nm. The Hill coefficient has been calculated from sigmoidal
CD melting curves as an indication of cooperativity of RNA global
unfolding.[82] The Hill coefficient values
obtained from the curves of Figure D are given in Table . These values indicate
that cooperativity of mRNA unfolding within the LNP is significantly
higher than that of mRNA in solution or in the reheated LNP. We can
infer that mRNA encapsulated in the LNP is structured differently
and more compact than mRNA in solution or in heat denatured LNP.A comparison of events occurring in free versus encapsulated
mRNA
leads to the conclusion that mRNA becomes thermally more stable in
its encapsulated form, more effectively preserving its basic CD signature
during heating. This observation parallels a pharmaceutical stabilization
strategy used for proteins whereby enhanced folded stability may be
conferred by favorable formulation conditions.[67] Here, we show that some degree of analogy exists regarding
LNP encapsulation conferring enhanced conformational stability to
the mRNA molecule. The achievement of the overall pharmaceutical stability
of lipid nanoparticles will also require consideration of colloidal
stability. This raises some further interesting analogies and contrasts
to proteins as net attractive or repulsive forces between molecules
or particles can influence pharmaceutical stability. With the advent
of monoclonal antibodies (mAbs) as a prominent class of therapeutics
and the frequent need to deliver them at high dose and high concentration,
favorable colloidal properties have become increasingly critical to
achieve overall pharmaceutical stability and deliverability.[83] It is not uncommon to formulate mAbs at >100
mg/mL under which condition the distance between van der Waals surfaces
of the molecules is on the same order of magnitude as the size of
the molecules themselves.[84] Consequently,
solubility, stability, and viscosity become strongly influenced by
intermolecular networks that form in solution.[85] These networks have a complicated dependence on the subtleties
of surface morphology, dipole character, and patchiness of the electrostatic
and hydrophobic surfaces. Although monoclonal antibodies are large
molecules with hydrodynamic diameters in the vicinity of ≈5–7
nm, this size is considerably smaller than the ≈100 nm size
of the lipid nanoparticles used to deliver RNA. Consequently, colloidal
aspects can be expected to play a key role in their formulation. While
LNPs may be cartoonishly represented as uniform spheres, the images
in Figure show potential
for significant complexity of size, shape, surface composition, surface
electrostatics, solvation, and proximity energies.[1,86]
Conclusions
Early descriptions of mRNA emphasized its instability. Titles of
the landmark publications announcing its discovery referred to the
molecule as “An unstable intermediate...”[87] and “Unstable ribonucleic acid...”.[88] While these descriptions were certainly not
made with pharmaceutical applications in mind, they were an indicator
of the unique stability profile relative to other biopolymers. Because
mRNA science has not evolved with a central emphasis on biomedical
applications, the interrelationships among primary sequence, higher-order
structure, biological activity (protein expression), and pharmaceutical
stability have only relatively recently become the focus of intense
research. The accelerated thermal degradation of proteins has been
studied extensively throughout biopharmaceutical history[89] as a means of connecting fundamental thermodynamic
measurables to the ultimate practical resilience of the intended therapeutic
product. While there is clearly a unique set of challenges associated
with stabilizing mRNA vaccines, the observation that encapsulation
within LNPs significantly enhances the folded stability of mRNA strikes
a familiar and optimistic note.
Authors: Duane T Brandau; Latoya S Jones; Christopher M Wiethoff; Jason Rexroad; C Russell Middaugh Journal: J Pharm Sci Date: 2003-02 Impact factor: 3.534
Authors: Heidrun Steinle; Andreas Behring; Christian Schlensak; Hans Peter Wendel; Meltem Avci-Adali Journal: Stem Cells Date: 2016-06-20 Impact factor: 6.277
Authors: Ozan S Kumru; Sangeeta B Joshi; Dawn E Smith; C Russell Middaugh; Ted Prusik; David B Volkin Journal: Biologicals Date: 2014-07-01 Impact factor: 1.856