In biology, membrane fluidity refers to the viscosity of the lipid bilayer of a cell membrane or a synthetic lipid membrane. Lipid packing can influence the fluidity of the membrane. Viscosity of the membrane can affect the rotation and diffusion of proteins and other bio-molecules within the membrane, thereby affecting the functions of these molecules.
Factors determining membrane fluidity
Membrane fluidity can be affected by a number of factors. One way to increase membrane fluidity is to heat up the membrane. Lipids acquire thermal energy when they are heated up; energetic lipids move around more, arranging and rearranging randomly, making the membrane more fluid. At low temperatures, the lipids are laterally ordered and organized in the membrane, and the lipid chains are mostly in the all-trans configuration and pack well together. The composition of a membrane can also affect its fluidity. The membrane phospholipids incorporate fatty acids of varying length and saturation. Lipids with shorter chains are less stiff and less viscous because they are more susceptible to changes in kinetic energy due to their smaller molecular size and they have less surface area to undergo stabilizing van der Waals interactions with neighboring hydrophobic chains. Lipid chains with double bonds are more fluid than lipids that are saturated with hydrogen and thus have only single bonds. On the molecular level, unsaturated double bonds make it harder for the lipids to pack together by putting kinks into the otherwise straightened hydrocarbon chain. Membranes made with such lipids have lower melting points: less thermal energy is required to achieve the same level of fluidity as membranes made with lipids with saturated chains. Incorporation of particular lipids, such as sphingomyelin, into synthetic lipid membranes is known to stiffen a membrane. Such membranes can be described as "a glass state, i.e., rigid but without crystalline order". Cholesterol acts as a bidirectional regulator of membrane fluidity because at high temperatures, it stabilizes the membrane and raises its melting point, whereas at low temperatures it intercalates between the phospholipids and prevents them from clustering together and stiffening. Some drugs, e.g. Losartan, are also known to alter membrane viscosity. Another way to change membrane fluidity is to change the pressure. In the laboratory, supported lipid bilayers and monolayers can be made artificially. In such cases, one can still speak of membrane fluidity. These membranes are supported by a flat surface, e.g. the bottom of a box. The fluidity of these membranes can be controlled by the lateral pressure applied, e.g. by the side walls of a box.
Heterogeneity in membrane physical property
Discrete lipid domains with differing m composition, and thus membrane fluidity, can coexist in model lipid membranes; this can be observed using fluorescence microscopy. The biological analogue, 'lipid raft', is hypothesized to exist in cell membranes and perform biological functions. Also, a narrow annular lipid shell of membrane lipids in contact with integral membrane proteins have low fluidity compared to bulk lipids in biological membranes, as these lipid molecules stay stuck to surface of the protein macromolecules.
Membrane fluidity can be measured with electron spin resonance (ESR), fluorescence, or deuterium nuclear magnetic resonance spectroscopy (NMR). ESR measurements involve observing spin probe behaviour in the membrane. Fluorescence experiments involve observing fluorescent probes incorporated into the membrane. Solid state deuterium nuclear magnetic resonance spectroscopy involves observing deuterated lipids. The techniques are complementary in that they operate on different timescales.
Membrane fluidity can be described by two different types of motion: rotational and lateral. In ESR, rotational correlation time of spin probes is used to characterize how much restriction is imposed on the probe by the membrane. In fluorescence, steady-state anisotropy of the probe can be used, in addition to the rotation correlation time of the fluorescent probe. Fluorescent probes show varying degree of preference for being in an environment of restricted motion. In heterogeneous membranes, some probes will only be found in regions of higher membrane fluidity, while others are only found in regions of lower membrane fluidity. Partitioning preference of probes can also be a gauge of membrane fluidity. In deuterium NMR, the average carbon-deuterium bond orientation of the deuterated lipid gives rise to specific spectroscopic features. All three of techniques can give some measure of the time-averaged orientation of the relevant (probe) molecule, which is indicative of the rotational dynamics of the molecule.
Lateral motion of molecules within the membrane can be measured by a number of fluorescence techniques: fluorescence recovery after photobleaching (FRAP) involves photobleaching a uniformly labelled membrane with an intense laser beam and measuring how long it takes for fluorescent probes to diffuse back into the photobleached spot. Fluorescence correlation spectroscopy (FCS) monitors the fluctuations in fluorescence intensity measured from a small number of probes in a small space. These fluctuations are affected by the mode of lateral diffusion of the probe. Single particle tracking involves following the trajectory of fluorescent molecules or gold particles attached to a biomolecule and applying statistical analysis to extract information about the lateral diffusion of the tracked particle.
A study of central linewidths of electron spin resonance spectra of thylakoid membranes and aqueous dispersions of their total extracted lipids, labeled with stearic acid spin label (SASL) (having spin or doxyl moiety at 5,7,9,12,13,14 and 16th carbons, with reference to carbonyl group), reveals a fluidity gradient. Decreasing linewidth from 5th to 16th carbons represents increasing degree of motional freedom (fluidity gradient) from headgroup-side to methyl terminal in both native membranes and their aqueous lipid extract (a multilamellar liposomal structure, typical of lipid bilayer organization). This pattern points at similarity of lipid bilayer organization in both native membranes and liposomes. This observation is critical, as thylakoid membranes comprising largely galactolipids, contain only 10% phospholipid, unlike other biological membranes consisting largely of phospholipids. Proteins in chloroplast thylakoid membranes, apparently, restrict lipid fatty acyl chain segmental mobility from 9th to 16th carbons vis a vis their liposomal conterparts. Surprisingly, liposomal fatty acyl chains are more restricted at 5th and 7th carbon positions as compared at these positions in thylakoid membranes. This is explainable as due to motional restricting effect at these positions, because of steric hindrance by large chlorophyll headgroups, specially so, in liposomes. However, in native thylakoid membranes, chlorophylls are mainly complexed with proteins as light-harvesting complexes and may not largely be free to restrain lipid fluidity, as such.
Diffusion coefficients of fluorescent lipid analogues are about 10−8cm2/s in fluid lipid membranes. In gel lipid membranes and natural biomembranes, the diffusion coefficients are about 10−11cm2/s to 10−9cm2/s.
Charged lipid membranes
The melting of charged lipid membranes, such as 1,2-dimyristoyl-sn-glycero-3-phosphoglycerol (DMPG), can take place over a wide range of temperature. Within this range of temperatures, these membranes become very viscous.
Microorganisms subjected to thermal stress are known to alter the lipid composition of their cell membrane (see homeoviscous adaptation). This is one way they can adjust the fluidity of their membrane in response to their environment. Membrane fluidity is known to affect the function of biomolecules residing within or associated with the membrane structure. For example,the binding of some peripheral proteins is dependent on membrane fluidity. Lateral diffusion (within the membrane matrix) of membrane-related enzymes can affect reaction rates. Consequently, membrane-dependent functions, such as phagocytosis and cell signalling, can be regulated by the fluidity of the cell-membrane.
- Lipid bilayer phase behavior
- Saffman–Delbrück model
- Homeoviscous adaptation
- Lipid bilayer
- Annular lipid shell
- Gennis, R. B. (1989) Biomembranes: Molecular Structure and Function. Springer, ISBN 0387967605.
- Heimburg, T. (2007) Thermal Biophysics of Membranes. Wiley-VCH, ISBN 3527404716.
- Simons K, Vaz WL (2004). "Model systems, lipid rafts, and cell membranes". Annual review of biophysics and biomolecular structure 33: 269–95. doi:10.1146/annurev.biophys.32.110601.141803. PMID 15139814.
- Baumgart, Tobias; Hunt, Geoff; Farkas, Elaine R.; Webb, Watt W.; Feigenson, Gerald W. (2007). "Fluorescence probe partitioning between Lo/Ld phases in lipid membranes". Biochimica et Biophysica Acta (BBA) – Biomembranes 1768 (9): 2182–94. doi:10.1016/j.bbamem.2007.05.012. PMC 2702987. PMID 17588529.
- Almeida, P. and Vaz, W. (1995). "Lateral diffusion in membranes", Ch. 6, pp. 305–357 in: Lipowsky, R. and Sackmann, E. (eds.) Handbook of biological physics. Elsevier Science B.V. doi:10.1016/S1383-8121(06)80023-0, ISBN 978-0-444-81975-8
- YashRoy R C (1990) Magnetic resonance studies of dynamic organisation of lipids in chloroplast membranes. Journal of Biosciences, vol. 15(4), pp. 281-288.http://www.researchgate.net/publication/225688482_Magnetic_resonance_studies_of_dynamic_organisation_of_lipids_in_chloroplast_membranes?ev=prf_pub
- Heimburg, Thomas and Marsh, Derek (1996). "Thermodynamics of the Interaction of Proteins with Lipid Membranes". In Kenneth M. Merz Jr. and Benoît Roux. Biological Membranes. Boston: Birkhäuser. pp. 405–462. doi:10.1007/978-1-4684-8580-6_13. ISBN 978-1-4684-8580-6.
- Helmreich EJ (2003). "Environmental influences on signal transduction through membranes: A retrospective mini-review". Biophysical chemistry 100 (1–3): 519–34. doi:10.1016/S0301-4622(02)00303-4. PMID 12646388.