Emma L.
Talbot
,
Jurij
Kotar
,
Lorenzo
Di Michele
and
Pietro
Cicuta
*
Department of Physics, Cavendish Laboratory, University of Cambridge, JJ Thomson Avenue, Cambridge, CB3 0HE, UK. E-mail: pc245@cam.ac.uk; Tel: +44 (0)1223 337462
First published on 25th January 2019
We demonstrate experimental control over tubule growth in giant unilamellar vesicles with liquid–liquid phase coexistence, using a thermal gradient to redistribute lipid phase domains on the membrane. As studied previously, the domains of the less abundant phase always partition towards hotter temperatures, depleting the cold side of the vesicle of domains. We couple this mechanism of domain migration with the inclusion of negative-curvature lipids within the membrane, resulting in control of tubule growth direction towards the high temperature. Control of composition determines the interior/exterior growth of tubules, whereas the thermal gradient regulates the length of the tubule relative to the vesicle radius. Maintaining lipid membranes under non-equilibrium conditions, such as thermal gradients, allows the creation of thermally-oriented protrusions, which could be a key step towards developing functional materials or artificial tissues. Interconnected vesicle compartments or ejected daughter vesicles as transport intermediaries towards hot/cold are just two possibilities.
Protuberances from a membrane can be highly curved, enabling the sorting of lipids. For example, regions of higher curvature in tubules pulled from aspirated vesicles were found to be enriched in the liquid-disordered phase.10 The curvature preference of some lipid phases over others, based on differences in bending modulii, also presents a method for curvature-induced domain patterning.11 Indeed, some proteins induce (or stabilise) curvature themselves, e.g. BAR (Bin, Amphiphysin, Rvs) domains,12–14 enabling lipid selectivity. Such proteins (or protein networks) may work via scaffolding – offering a curved surface for interaction with the lipid membrane, or by directly inserting into part of the membrane (e.g. the top half of a bilayer) and acting as a wedge that locally deforms the membrane.12 For example, the lateral separation of curvature-inducing membrane proteins mediates endocytosis.15 Conversely, the selection of lipids in highly curved tubules offers the potential to expel known composition daughter vesicles from a membrane, or to deliver other moieties that prefer the tube phase, e.g. surfactants/proteins.
Giant unilamellar vesicles (GUVs) share various properties with biological cell membranes whilst reducing the complexity significantly, and they provide an ideal chassis for “artificial cells”, enabling compartmentalisation of functional material within a surrounding bilayer membrane.17 Vesicle networks with compartmentalisation are capable of step-wise synthetic chemistry reactions,18 mimicking organelles or functioning towards artificial tissue. These nano-reactors can trigger the release of chemicals/cargo when exposed to external stimuli.19 Directed growth of membrane extensions is therefore a relevant feature with potential to advance synthetic biology. GUVs with a ternary composition of a saturated lipid, an unsaturated lipid, and a sterol can form domains of coexisting liquid phases (liquid-ordered, Lo, and liquid-disordered, Ld) below a mixing transition temperature, Tt.20–22 The most common morphology, minimising the line tension, is circular domains. The phase forming domains are the minority phase and thus depend on the composition of the vesicle, and on the phase diagram (particularly the tie lines of the mixture).23 For example, at a higher concentration of saturated lipid, domains will be of the liquid-ordered phase.24
Directed growth of tubules via a non-invasive method can provide the first stage towards developing interconnected vesicle compartments with “communication” for creating artificial tissue. Alternatively, directed growth of tubules as transport intermediaries would allow the expulsion of daughter vesicles towards hot/cold for thermally targeted delivery. Current methods for tubule growth from GUVs are either invasive (micro-manipulation,25 optical tweezing of a bead attached to the membrane,26,27 and hydrodynamic flows on immobilized vesicles28) or do not offer control over the direction of tubule growth (motor-proteins,29 curvature-inducing proteins,12,30 and inclusion of wedge-shaped lipids31). So far, only confinement methods,32 aqueous phase separation,33,34 and chemically-triggered ejection35 offer a route to spontaneously grow tubules in a defined direction, but the second needs a specific interior solution, and the latter requires local injection of a chemical.
In this paper, we explore the non-equilibrium conditions induced by thermal gradients as an unobtrusive method for directed tubule growth in GUVs towards hot or cold. This thermal method is of relevence to the intracellular environment, as the temperature difference between organelles can vary up to around 0.7 K.36 We use ternary GUVs as a model system, formed from lipids with a composition chosen to exhibit liquid-disordered/liquid-ordered phase coexistence with circular lipid domains.20 There are three main concepts that we bring together to achieve control over the spontaneous and directed growth of the tubules. First, we control the relative area fractions of liquid ordered and liquid disordered phases, which in turn relates to subtle regulation of vesicle shape and thereby controls internal/external monolayer areas. Second, we include “wedge-shaped” lipids with negative curvature that can stimulate tubule growth from a bilayer, due to a temperature-change induced imbalance in wedge-lipids across the bilayer leaflets. These wedge-lipids enable randomly-oriented tube growth from the vesicle when no thermal gradient is applied,12,31 and they stabilise those tubes due to their innate curvature. Third, we implement the recently revealed migration of lipid domains seen in thermal gradients16 to reposition lipid domains on the surface of the GUV. Domains migrate towards higher temperatures to reduce their line interface energy closer to mixing.16 Following migration of the domains to higher temperatures, tubule growth is induced, giving directed growth on the hot side. This technique could be extended to the directed expulsion of daughter vesicles of known composition, containing moieties segregated into the tube phase.
GUVs with liquid-disordered (Ld)/liquid-ordered (Lo) phase coexistence were formed from mixtures of DOPC, DPPC, and chol with a fluorescent probe. Molar ratios of DOPC:DPPC:chol were chosen that formed circular lipid domains of the Ld phase (or Lo phase) with a near equal area to that of the background phase.20 For circular Ld domains, we used DOPC:DPPC:chol with a composition of 30:30:40 mol%, and for circular Lo domains, we used 35:35:30 mol%. Other compositions with the same domain type (Ld or Lo as the minority phase) behave much in the same manner.
Fig. 1 GUVs are held in a thermal gradient and imaged in epifluorescence. Tubules nucleate from phase domains, which migrate towards the hot cap. (a) The schematic shows the custom-made imaging cell used to impose a thermal gradient: the copper holder dimensions are 54 mm × 86 mm × 34 mm. Sapphire windows ensure no lateral convection. The vesicle sample sits inside the hole in the silicone spacer, which ensures a sample thickness of 200 μm. The range of ∇T between the hot and cold plates in this work is typically 0–0.33 K μm−1. (b) As in a previous work,16 we observe that the cold cap is depleted of domains (here, Ld in DOPC:DPPC:chol 30:30:40 mol% GUV). Scale bars are 10 μm. In this time series, the thermal gradient was ∇T = 0.1 K μm−1 with cap T as indicated. (c) Schematic of domain migration and coalescence from the cold to the hot side, as in a similar system.16 (d) Schematic of the directed and position controlled tubule growth observed in this study. Controlled tubule growth results from a two step process. Step 1: circular lipid phase domains of the liquid-disordered phase migrate towards higher temperatures as shown previously.16 When present, the wedge-shaped lipid DOPE preferentially partitions into the liquid-disordered phase and is transported with the domains towards higher temperatures. Step 2: tubules grow from domains on the hot side of the vesicle while GUVs are still phase separated when DOPE is present. |
Prior to applying a temperature ramp, we heated GUVs above their transition temperature for 5 min and cooled them again to ensure lipids within the membrane fully mixed to present a starting point where domains were not already coalesced on the membrane.
During imaging, the cold plate of the thermal-cell was typically held at 278 K to begin with. For a temperature ramp with ∇T ≠ 0, the hot plate was then ramped from 278 K up to 343 K in intervals of 1 K (∇T ≠ 0) while the cold plate was maintained at 278 K throughout. The temperature of the cell was allowed to equilibrate for 1 minute between each step. Whereas, for a temperature ramp with ∇T = 0, the hot plate was fixed at the same temperature as the cold plate (i.e. 278 K to start with), and then both were increased together in 1 K steps, i.e. both to 279 K and equilibrated for 1 minute, until both plates reached 343 K.
When no wedge lipid is included in the membrane, we observe tubule growth from the GUVs occurring upon heating and crossing above the transition temperature, Tt. For our choice of ternary compositions, the systems with Ld circular domains exhibit a transition temperature, Tt, slightly lower than the systems with Lo domains (Fig. 2(a)), and they also grow tubules at lower temperatures. For vesicles that originally have Ld domains, tubule growth is external to the vesicle. In contrast, for vesicles that originally have Lo domains, tubules grow into the interior of the vesicle. Examples of each type of growth are shown in Fig. 2(c and d).
The growth of internal tubules from vesicles with Lo domains plateaus after a given temperature above the initialisation temperature, with normalised tubule lengths comparable for both ∇T = 0 and ∇T ≠ 0 (Fig. 3(a)). The comparable growth suggests that tubule length depends on the increase in temperature of the vesicle, and not on the thermal gradient. In comparison, the outwardly extending tubules grown from vesicles with Ld domains exhibit an initial stage of growth followed by a stage of shrinking (Fig. 3(b)). In the first stage of growth, the diameter of the vesicle remains fairly constant, whereas the stage in which the tubule shrinks corresponds to a swelling of the vesicle diameter. Lastly, a new interior tubule sprouts and grows as the vesicle shrinks in size once more. The external-growth/shrink/internal-growth behaviour of these membrane tubules imposes a thermal limit for external tube growth and switch over to internal tube growth, which has potential use as a trigger to introduce a “switch off temperature” after which external tubes will no longer grow to heat but instead go inside the vesicle.
The tubule growth above Tt can be explained by considering the excess area of the bilayer. As the temperature of the membrane increases, the relative area density of each leaflet of the bilayer changes due to the larger change in area of the outer leaflet from thermal expansion, which, for geometric reasons,39 leaves an excess area in the outer leaflet (lipid flip-flop might equilibrate this excess over a long period of time). Excess area in the outer leaflet would always promote growth of external tubes on heating. Additionally, as the transition temperature is approached, the lipid compositions of the two phases are brought closer, reducing the ordering of acyl chains in the Lo phase. The reduction in packing of the lipid tail-groups can increase the excess area of the vesicle (for both leaflets).40 So, the average interfacial area of the lipids can increase at higher temperatures, contributing to an increase in the excess area.24 For example, a DPPC lipid molecule has an average interfacial area of 47.9 Å2 at 293 K41 and 64 Å2 at 323 K41 (Tm = 314 K20). These factors all couple to result in external tubule growth above Tt, to relieve the imbalance in excess membrane area. However, another important aspect is the vesicle shape in the presence of domains, which has been considered in various studies.24,42 The disordered phase has a lower bending modulus, and therefore domains of that phase tend to bud out of the majority ordered phase. In contrast, domains of the ordered phase tend to be flat in the background of a disordered majority phase. As the temperature is increased towards melting, the vesicle approaches a spherical shape (this can be through non-monotonic changes in the diameter24), and at this point, a vesicle that started with Ld domains will have reduced overall curvature, whereas a vesicle that started with Lo domains will have increased curvature. The two conditions lead to opposite excess areas across the bilayer, which can be balanced by forming external and internal tubules, respectively.
When no thermal gradient is applied, tubule growth is initiated at ∼Tt, whereas when a thermal gradient is applied, tubule growth is initiated when the temperature of the hot side of the cell has far surpassed the transition temperature (Fig. 3(a)). The high T tubulation transition for ∇T ≠ 0 could indicate that a large enough proportion of the membrane must reach temperatures above Tt to give a significant enough increase in the excess area for tubule formation. Indeed, the mean normalised temperature at which tubule growth begins in a thermal gradient is close to the point the mean vesicle temperature reaches Tt (Fig. 3(a)). Tubule growth above Tt (when no wedge lipids are present) prevents the use of lipid phase domains to position the tubes, since domains disappear above Tt.
Note that the fluorescent dyed lipid, TX-DHPE, has an innate curvature, hence its preference for one phase over the other: as a control, we checked that tubule growth is still initiated at temperatures high above the transition temperature when this dye is not included in the membrane and there are no wedge lipids either (Fig. 2(c and d)).
We also attempted an experiment to test if the tube has a clear lumen accessible to the vesicle interior. Fluorescein dye was included within the vesicle compartment. We could not observe the fluorescein dye signal from the tubule, leaving an open question as to whether the external tubules are bilayer tubes or composed of the outer leaflet only.
When no thermal gradient is applied, the DOPE:DOPC:DPPC:chol vesicles with Ld domains deform from spherical and then grow tubules external to the vesicle as Tt is exceeded. As the temperature is increased above Tt, there is a local increase in excess area, predominantly of the Lo background phase, which makes the vesicle floppy (see Fig. S1a, ESI†) and enables randomly orientated tubule formation. Similar to the vesicles without the wedge lipid, external tubules grew and then shrank, before becoming internal tubules instead. Vesicles with Lo circular domains containing the wedge lipid grow internal tubules, also initiated after Tt has been exceeded for ∇T = 0 (Fig. S1b, ESI†). At higher temperatures, tubule growth is enhanced independent of the phase of the domains, which is explained by the increase in excess area with temperature.
For GUVs with Ld domains, the DOPE is concentrated within these disordered domains, favouring negative curvature of the inner leaflet and leading to the formation of external tubes. If instead, the GUVs have Lo domains, then the DOPE is more spread out in the background phase. In this case, the increased excess area of the GUV is mostly local to the domains and lowers the internal pressure, and an invaginated tubule forms to relax the negative pressure.
If tubule growth occurs before domains have fully migrated to the hot cap, then tubules can grow from both caps of the vesicle (e.g. Fig. S2, ESI†). This situation can occur if the temperature across the vesicle becomes high enough to cause tubule growth before the domains have fully migrated onto the hot cap. Similarly, if the temperature is increased above Tt such that extended tubules grow, which remain intact upon quenching below Tt, then those tubules do not necessarily associate with Ld domains and move around the vesicle (Fig. S2, ESI†), so these tubules can remain on the cold side. To control tubule position, it is therefore important to ensure that tubule growth is only initiated after domain formation and their migration to the hot side.
By changing the composition of the GUV, Lo circular domains are formed on a Ld background phase, which still migrate around from the cold cap to the hot cap when a thermal gradient is applied (Fig. S3a, ESI†). As the temperature approaches Tt, tubule growth begins, but it is interior to the vesicle (Fig. S3b, ESI†), persisting above Tt to lengthen the tubules (Fig. S3c, ESI†). In this case, the temperature gradient does not provide useful directed growth of the tubules from the hot or cold cap, rather the tubules coil inside the vesicle as they extend.
Independent of which phase forms the circular domains, tubule growth in a thermal gradient occurs before passing through the mixing transition temperature for GUVs containing DOPE (Fig. 5). This contrasts with the observations for ∇T = 0, where tubule growth was only initiated from the vesicle after Tt was exceeded (Fig. 5), and it is likely in part due to the stabilisation effect of wedge lipids on tubule growth. At a uniform temperature, GUVs containing the wedge lipid grow tubules above the transition temperature with similar growth behaviour to membranes without the wedge lipid (Fig. 5).
For directed tubule growth via domain migration, tubules must form below Tt, which is only possible when wedge lipids are included in the membrane and a thermal gradient is applied. The thermal gradient concentrating DOPE by the domain migration mechanism could therefore be a key factor in tubule growth below Tt and in the shrink/growth behaviour.
For vesicles in a thermal gradient with bright Ld domains, the tubule growth external to the GUV attains longer tubule lengths (compared to the vesicle radius) than vesicles with dark Lo domains that grow internal tubes (Fig. S4a, ESI†). The longer growth relates to the larger proportion of the Lo phase in GUVs with bright domains that is responsible for the largest increase in excess area above Tt. For all GUVs, the tubule length initially grows with increasing temperature of the hot side of the vesicle. Tuning the temperature gradient therefore enables control over the length of the tube. In addition, normalised tubule lengths were longer for GUVs containing the wedge lipid when a thermal gradient was applied compared to growth at a uniform temperature.
For GUVs including DOPE, there is then a stage where the tube length shrinks after passing above Tt (Fig. 5). In the case of GUVs with Lo domains, the internal tubules then re-grow following this regime of shrinking. For GUVs with Ld domains, shrinking occurs further above Tt and external tubules shrink before internal tubules grow. Tubule shrinkage could occur on passing above Tt due to phase mixing. Below Tt, the DOPE is partitioned between each phase with higher concentrations in the Ld phase (from which tubules grow for either GUV composition). The DOPE stabilises tubule growth, which is initiated from the line interface between domains in phase separated GUVs. On mixing, the DOPE spreads out in the membrane, locally reducing the concentration of wedge lipid in regions that were previously the Ld phase, including the tubules. The tubules are then less stable and shrink.
To determine whether the existence of phase domains has a significant contribution to selecting whether tubules grow inward/outward and if they shrink after an initial growth period, vesicles were made with the same composition ratio as GUVs forming Lo domains but with DOPC replacing all DPPC (i.e. DOPE:DOPC:DPPC:chol 2:68:0:30 mol%). These GUVs do not have phase domains and they grow external tubules, despite having the same concentration of wedge lipid and cholesterol as GUVs with Lo domains that have internal tubes. The growth of these external tubes is very similar to growth from GUVs with bright Ld domains (Fig. 5). This tubule growth plateaus without shrinkage (Fig. 5), suggesting phase domains and subsequent phase mixing are necessary for tubule shrinkage. Additionally, the length of tubules grown either internally or externally correlates positively with an increase in GUV radius, suggesting a strong link with the membrane area (Fig. S4a, ESI†).
The phase transition temperature was significantly decreased on addition of more wedge-shaped lipids. For vesicles with circular domains formed from the liquid-ordered phase, tubule growth was interior to the vesicle. However, for vesicles with circular domains formed from the liquid-disordered phase, tubules grew outwards from the vesicle's surface and to longer lengths (compared to the GUV radius). In the latter case, tubule growth was induced following the migration of domains to the hot side of the vesicle by raising the temperature of the hot cap. The result was the directed growth of tubules from the hot side of the vesicle. Hence, material concentration of wedge-shaped lipids within domains and the subsequent redistribution of those domains through thermally-induced migration provide a route for the directed growth of protuberances, offering significant potential to advance avenues of synthetic biology.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8sm01892h |
This journal is © The Royal Society of Chemistry 2019 |