Cell membrane
The cell membrane is the reason you are alive right now. Every one of your trillions of cells is wrapped in this structure, a sheet just a few nanometers thick that decides what enters and what stays out. It keeps the chemistry of life running by acting as a gatekeeper, a scaffold, a communications hub, and sometimes an active transporter, all at once.
For most of recorded scientific history, researchers either could not see this membrane or refused to believe it existed. Robert Hooke first described cells in 1665, yet for well over 150 years afterward, scientists focused almost entirely on the rigid cell wall of plant cells. The soft, invisible barrier surrounding animal cells barely registered. When a few careful observers did infer that something must be there, others pushed back hard. As late as the 1890s, many scientists were still arguing that a cell membrane simply did not exist.
What changed everything was a sequence of elegantly simple experiments and a pair of researchers who spread the lipid from human red blood cells across the surface of water and found that it covered twice the area of the cells it came from. That 2:1 ratio told them the membrane had to be two layers thick. From that measurement in 1925, the modern picture of the cell membrane began to take shape. How did scientists move from flat denial to a detailed molecular map of this structure? And what makes the cell membrane so much more than just a wall?
Ernest Overton proposed in 1895 that cell membranes were made of lipids, but reaching even that point had taken two centuries of argument. When plant cells were separated from one another in the early 19th century, scientists concluded that all cells were enclosed by individual walls. That idea then extended to animal cells, treating the wall as a universal feature of life.
By the second half of the 19th century, microscopy still could not resolve the difference between a cell membrane and a cell wall. Some observers made an educated inference: internal components moved around inside cells but not outside, and that asymmetry implied a boundary. Yet the prevailing view held that membranes were not vital components of all cells. A revision to the cell theory in 1890 acknowledged that cell membranes might exist, but demoted them to secondary structures with little functional importance.
Terminology reflected the confusion. Different researchers gave the outer region of the cell competing names across the same decades. Wilhelm Pfeffer called it the Plasmahaut, or plasma skin, in 1877 and then the plasmatic membrane in 1900. Hugo de Vries used the term ectoplast in 1885. Those who doubted a functional permeable boundary existed at all preferred the word plasmalemma, a term coined by S. O. Mast in 1924. The pile-up of competing names was its own kind of evidence that no one had settled the question yet. Osmosis and permeability experiments would eventually force that settlement in the early 20th century.
Gorter and Grendel proposed the lipid bilayer hypothesis in 1925 and the experiment behind it was disarmingly straightforward. They extracted lipids from human red blood cells and spread them across the surface of water. Mature mammalian red blood cells have no nuclei and no cytoplasmic organelles, which meant every lipid they extracted had to have come from the plasma membrane. When they calculated the area that extracted lipid covered against the total surface area of the original cells, the ratio came out to approximately 2:1. Two layers, stacked on top of each other.
The same year, a researcher named Fricke measured the thickness of erythrocyte and yeast cell membranes and found they ranged between 3.3 and 4 nanometers. That measurement was consistent with a single lipid layer rather than two. Critics questioned the dielectric constant used in the calculation, but later tests could not overturn the original result. A separate instrument called the leptoscope measured very thin membranes by comparing light reflected from a sample against a membrane standard of known thickness. Depending on pH and the presence of proteins, the leptoscope returned thickness readings of 8.6 to 23.2 nanometers, and the lower end of that range supported the bilayer idea.
By the 1930s, Hugh Davson and James Danielli proposed what became known as the paucimolecular model. They based it on surface tension studies involving oils and echinoderm eggs. The surface tension at cell surfaces was far lower than expected for a plain oil-water interface, suggesting something else was reducing it. Their proposal: a lipid bilayer sandwiched between two thin protein layers. That model dominated the field for roughly 30 years.
S. J. Singer and G. L. Nicolson published their fluid mosaic model in 1972, replacing the Davson-Danielli framework that had held for three decades. Their core idea was that the membrane behaves like a two-dimensional liquid, with lipid and protein molecules free to drift and diffuse within it rather than locked in a static sandwich.
The model recast proteins not as flat coatings on either side of the bilayer but as structures embedded within it. Integral proteins, the ones that span the full width of the membrane, carry hydrophobic amino acids on the sections that contact the non-polar lipid interior. Their hydrophilic ends face the watery environments on either side. This pairing of chemistry to position turned out to be the key to understanding how the membrane manages traffic.
Decades of refinements have added detail to the 1972 picture without dismantling it. Protein-protein complexes dot the membrane surface. Structures called pickets and fences, formed by the actin-based cytoskeleton, break the membrane into functional zones. Cholesterol-enriched patches called lipid rafts and caveolae create specialized microdomains. The tightly bound ring of lipid that surrounds each integral protein, called the annular lipid shell, behaves as part of the protein complex rather than as free membrane. The fluid mosaic model also deepened the study of hydrophobic forces, which became a foundational concept for understanding biological macromolecules far beyond the membrane itself.
Phospholipids make up the structural backbone of the membrane and account for over 50% of all lipids in plasma membranes. Glycolipids make up only about 2%. Sterols, including cholesterol in animal cells, fill the remaining share. In red blood cells, lipid makes up 30% of the plasma membrane by weight; for most eukaryotic cells, the split between lipid and protein is roughly half and half.
The fatty acid chains attached to phospholipids and glycolipids usually carry between 16 and 20 carbon atoms, with 16-carbon and 18-carbon varieties being the most common. Whether those chains are saturated or unsaturated shapes how the membrane behaves. Unsaturated chains introduce a kink that prevents tight packing, which lowers the temperature at which the membrane transitions from a fluid to a gel-like state. The ability of organisms to tune fluidity by adjusting lipid composition has a name: homeoviscous adaptation.
Cholesterol distributes itself through the irregular spaces between the hydrophobic tails of the membrane lipids. In warm conditions, it restrains the movement of fatty acid chains, reducing permeability and stiffening the membrane. In cold conditions, it does the opposite, acting as an antifreeze that keeps lipids from locking up. Cold-weather animals carry more cholesterol in their membranes than warm-weather animals do. Plants, which lack cholesterol entirely, use related sterol compounds to perform the same regulatory role.
Carbohydrates are concentrated on the outer face of the membrane, forming the glycocalyx. The penultimate sugar in these chains is galactose; the terminal sugar is sialic acid, modified in the Golgi apparatus. Sialic acid carries a negative charge, creating an electrostatic barrier at the cell surface. This outer coat participates in cell adhesion and lymphocyte homing, and viruses exploit the same carbohydrate receptors to gain entry to cells.
Approximately a third of the genes in yeast code for membrane proteins, and that fraction rises still higher in multicellular organisms. Proteins account for roughly half the volume of the cell membrane, and three main categories divide the work: integral proteins, peripheral proteins, and lipid-anchored proteins.
Ion channels are integral proteins that punch hydrophilic pores through the bilayer, letting sodium, potassium, calcium, and chlorine diffuse along their electrochemical gradients. The electrical behavior of nerve cells depends on exactly this mechanism. Proton pumps are a different class of integral protein. They move protons across the membrane by passing them from one amino acid side chain to the next, a relay that powers processes like electron transport and the synthesis of ATP. G-protein coupled receptors cross the bilayer seven times and respond to signal molecules such as hormones and neurotransmitters. They regulate cAMP production and control ion channels as part of cell-to-cell communication.
Peripheral proteins attach to the surface or to integral proteins and tend to interact only temporarily with the membrane before dissociating to carry out their work elsewhere in the cytoplasm. Lipid-anchored proteins are covalently bound to one or more lipid molecules, anchored hydrophobically in the membrane while the protein itself never actually contacts the bilayer directly.
For a protein to reach the membrane, it typically needs an N-terminus signal sequence of amino acids. That sequence directs the protein to the endoplasmic reticulum, which inserts it into a lipid bilayer. From there, vesicles carry the protein to its final destination, fusing with the target membrane to deliver it.
Passive osmosis and diffusion handle some of the simplest traffic. Small, electrically neutral molecules such as carbon dioxide and oxygen cross the bilayer without any cellular energy expenditure, moving from higher to lower concentration until both sides equilibrate. Water follows the same logic through osmosis, driven by the concentration gradient across the semipermeable membrane.
Charged and polar molecules face a harder crossing. The hydrophobic interior of the bilayer blocks amino acids, nucleic acids, carbohydrates, and ions from diffusing freely. Those substances move through protein channels called permeases, which are highly selective and often handle only a single chemical substance. Aquaporins channel water specifically. Other transmembrane transporters actively pump molecules across the membrane, consuming cellular energy to move substances against their concentration gradients.
Endocytosis is the process by which cells engulf material. The plasma membrane deforms inward, forming an invagination that closes off into an internal vesicle. Proteins on the outside of the membrane act as receptors, clustering into depressions and pulling more proteins and lipids to the cytosolic side to deepen the pocket. The vesicle that results can carry solid particles in what is called phagocytosis, or small molecules and ions in what is called pinocytosis. Endocytosis requires energy and qualifies as active transport.
Exocytosis runs the reverse path. A vesicle formed inside the cell travels toward the plasma membrane, makes contact, and the two lipid bilayers fuse. A passage opens and the vesicle discharges its contents into the space outside the cell. Cells use this route to release hormones and enzymes, to clear undigested residues left over from endocytosis, and to ferry substances entirely across a cellular barrier. In the mitochondria and chloroplasts of eukaryotes, a specialized version of this membrane machinery drives the synthesis of ATP through chemiosmosis.
Muscle cells carry a version of the cell membrane called the sarcolemma. It performs all the standard membrane functions and adds several that only muscle cells need. The sarcolemma transmits synaptic signals and helps generate action potentials, and it forms narrow internal channels called T-tubules that run through the entire muscle cell. The average sarcolemma measures 10 nanometers thick, compared to the 4-nanometer thickness of a general cell membrane.
An oocyte, the immature egg cell, wraps itself in the oolemma. Unusually, the oolemma does not follow the standard lipid bilayer structure. Its interior layer is the fertilization envelope, and its exterior is the zona pellucida in mammals (the vitelline membrane in non-mammals), a structure made of glycoproteins rather than lipids. Channels and proteins are still present to carry out membrane functions, but the underlying architecture is distinct.
Nerve cell axons are covered by the axolemma, a specialized plasma membrane responsible for generating the action potential. It consists of a granular, densely packed lipid bilayer that works closely with two cytoskeleton proteins: spectrin and actin. Those cytoskeleton components bind to and interact with the transmembrane proteins embedded in the axolemma.
In polarized cells such as those lining the gut, the membrane is not uniform across the whole cell surface. The apical surface faces the interior lumen. The basolateral surface faces outward toward surrounding tissue. Tight junctions near the apical surface prevent proteins from migrating between these two zones, keeping their distinct compositions intact. The apical surfaces of gut epithelial cells are dense with actin-based projections called microvilli, which expand the surface area available for absorbing nutrients.
Common questions
What is the cell membrane made of?
The cell membrane is a lipid bilayer composed primarily of phospholipids, along with glycolipids and sterols such as cholesterol. Phospholipids typically account for over 50% of all lipids in plasma membranes, while glycolipids make up about 2%. Proteins constitute roughly half the membrane's volume by weight in most eukaryotic cells.
Who discovered that the cell membrane is a lipid bilayer?
Gorter and Grendel proposed the lipid bilayer hypothesis in 1925. They extracted lipids from human red blood cells and measured the surface area those lipids covered when spread over water. The area was approximately twice that of the original red blood cells, indicating the membrane consists of two lipid layers.
What is the fluid mosaic model of the cell membrane?
The fluid mosaic model, published by S. J. Singer and G. L. Nicolson in 1972, describes the cell membrane as a two-dimensional liquid in which lipid and protein molecules diffuse freely. It replaced the earlier paucimolecular model of Davson and Danielli from 1935 and remains the primary framework for understanding membrane structure today.
How does the cell membrane control what enters and exits a cell?
The cell membrane uses both passive and active transport mechanisms. Small neutral molecules such as oxygen and carbon dioxide cross by diffusion without energy input. Charged and polar molecules are moved through protein channels called permeases or by active transporters that consume cellular energy. Endocytosis engulfs material by forming internal vesicles, while exocytosis releases material by fusing internal vesicles with the plasma membrane.
What role does cholesterol play in the cell membrane?
Cholesterol regulates membrane fluidity by dispersing through the spaces between the hydrophobic tails of membrane lipids. In high temperatures it inhibits fatty acid chain movement, stiffening the membrane. In cold temperatures it acts as antifreeze, preventing lipids from packing too tightly. Cold-weather animals carry more cholesterol in their membranes than warm-weather animals.
How long did scientists debate whether the cell membrane existed?
For well over 150 years after Robert Hooke described cells in 1665, scientists focused primarily on the cell wall and largely disregarded the membrane. A revision to the cell theory in 1890 acknowledged membranes but treated them as secondary structures. It was not until the early 20th century, through osmosis and permeability experiments, that the significance of the cell membrane was widely accepted.
All sources
49 references cited across the entry
- 2BookBacteria in Biology, Biotechnology and MedicineSingleton P — Wiley — 1999
- 3JournalPhysiology, MembraneTom Herrmann et al. — March 2, 2019
- 4BookMolecular Biology of the CellAlberts B, Johnson A, Lewis J — Garland Science — 2002
- 5JournalMembrane assembly driven by a biomimetic coupling reactionBudin I, Devaraj NK — January 2012
- 6Chemists Synthesize Artificial Cell MembraneStaff — ScienceDaily — January 25, 2012
- 7Chemists create artificial cell membraneStaff — kurzweilai.net — January 26, 2012
- 8JournalThe effects of intra-membrane viscosity on lipid membrane morphology: complete analytical solutionMahdi Zeidi et al. — 2018
- 9JournalOnce upon a time the cell membranes: 175 years of cell boundary researchLombard J — December 2014
- 11JournalOn Bimolecular Layers of Lipoids on the Chromocytes of the BloodGorter E, Grendel F — March 1925
- 12BookCell and Molecular BiologyGerald Karp — John Wiley & Sons, Inc. — 2009
- 13JournalPlasmolytische Studien über die Wand der Vakuolende Vries H — 1885
- 17JournalStructure and locomotion in Amoeba proteusMast SO — 1924
- 18JournalMembranes in the plant cell. I. Morphological membranes at protoplasmic surfacesPlowe JQ — 1931
- 19BookPlant Cell Biology: From Astronomy to ZoologyWayne R — Elsevier/Academic Press — 2009
- 20JournalAssessment of Membrane Fluidity Fluctuations during Cellular Development Reveals Time and Cell Type SpecificityNoutsi P, Gratton E, Chaieb S — 2016-06-30
- 21BookMolecular Cell BiologyLodish H, Berk A, Zipursky LS — Scientific American Books — 2000
- 22JournalStructure of the Plasma MembraneGeoffrey M. Cooper — 2000
- 23JournalBiomembranes: Structural Organization and Basic FunctionsHarvey Lodish et al. — 2000
- 24JournalCell-surface carbohydrates in cell recognition and responseBrandley BK, Schnaar RL — July 1986
- 25Membrane StructureJesse Gray et al. — Davidson College — 2002
- 26JournalPost-Translational Modifications and Quality Control in the Rough ERHarvey Lodish et al. — 2000
- 27JournalTransport of Small MoleculesGeoffrey M. Cooper — 2000
- 28JournalOsmosis is not driven by water dilutionKramer EM, Myers DR — April 2013
- 29BookMolecular Biology of the CellBruce Alberts et al. — 2002
- 30BookMolecular Biology of the CellBruce Alberts et al. — Garland Science — 2002
- 31BookMedical MicrobiologyMilton R. J. Salton et al. — University of Texas Medical Branch at Galveston — 1996
- 32JournalCarotenoid-related alteration of cell membrane fluidity impacts Staphylococcus aureus susceptibility to host defense peptidesMishra NN, Liu GY, Yeaman MR, Nast CC, Proctor RA, McKinnell J, Bayer AS — February 2011
- 33JournalBacterial lipopolysaccharides and innate immunityAlexander C, Rietschel ET — 2001
- 35JournalMicrocompartments and protein machines in prokaryotesSaier MH — 2013
- 36JournalThe fluid mosaic model of the structure of cell membranesSinger SJ, Nicolson GL — February 1972
- 38JournalMediation, modulation, and consequences of membrane-cytoskeleton interactionsDoherty GJ, McMahon HT — 2008
- 39JournalFrom extracellular to intracellular: the establishment of mitochondria and chloroplastsWhatley JM, John P, Whatley FR — April 1979
- 40BookMolecular Biology of the CellBruce Alberts et al. — Garland Science — 2002
- 41BookMolecular Biology of the CellBruce Alberts et al. — Garland Science — 2002
- 42JournalThe Endoplasmic ReticulumGeoffrey M. Cooper — 2000
- 43JournalThe asymmetrical structure of Golgi apparatus membranes revealed by in situ atomic force microscopeXu H, Su W, Cai M, Jiang J, Zeng X, Wang H — 2013-04-16
- 44JournalSkeletal muscle basement membrane-sarcolemma-cytoskeleton interaction minireview seriesCampbell KP, Stull JT — April 2003
- 45JournalModulation of the bilayer thickness of exocytic pathway membranes by membrane proteins rather than cholesterolMitra K, Ubarretxena-Belandia I, Taguchi T, Warren G, Engelman DM — March 2004
- 46JournalStructure and function of the sarcolemma of skeletal muscleReed R, Wouston TW, Todd PM — July 1966
- 47JournalCell surface changes in the egg at fertilizationWessel GM, Wong JL — October 2009
- 48JournalCharacteristics of the NeuronCedric S. Raine — 1999
- 49JournalThe role of the axolemma in the initiation of traumatically induced axonal injuryFitzpatrick MO, Maxwell WL, Graham DI — March 1998