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Presented by
Dr. Swapnaneel Pradhan
CELL MEMBRANE
 This membrane consists almost entirely of a lipid bilayer, but it also contains large numbers of
protein molecules in the lipid, many of which penetrate all the way through the membrane.
 The lipid bilayer is not miscible with either the extracellular fluid or the intracellular fluid. Therefore, it
constitutes a barrier against movement of water molecules and water-soluble substances between
the extracellular and intracellular fluid compartments.
 The protein molecules in the membrane have entirely different properties for transporting
substances. Their molecular structures interrupt the continuity of the lipid bilayer, constituting an
alternative pathway through the cell membrane. Many of these penetrating proteins can function as
transport proteins.
 Channel proteins: These proteins have
watery spaces all the way through the
molecule and allow free movement of
water, as well as selected ions or
molecules.
 Carrier proteins: These Proteins bind with
molecules or ions that are to be
transported, and conformational changes
in the protein molecules then move the
substances through the interstices of the
protein to the other side of the membrane.
Channel proteins and carrier proteins are usually selective for the types of molecules or ions that are
allowed to cross the membrane.
Transport
Proteins
Channel
Proteins
Carrier
proteins
Transport through
Cell Membrane
Transport through the cell membrane, either
directly through the lipid bilayer or through
the proteins, occurs via one of two basic
processes:
• Active transport
• Passive transport (Diffusion)
Transport
Active
Transport
Primary Secondary
Passive
Transport
Simple
diffusion
Facilitated
diffusion
PASSIVE TRANSPORT
Simple Diffusion
Simple diffusion can occur through
the cell membrane by two
pathways:
1. through the interstices of the
lipid bilayer if the diffusing
substance is lipid soluble,
2. through watery channels that
penetrate all the way through
some of the large transport
proteins.
• An important factor that determines how rapidly a substance diffuses through the lipid
bilayer is the lipid solubility of the substance.
Rate of diffusion ∝ lipid solubility of substance
• For example, the lipid solubilities of oxygen, nitrogen, carbon dioxide, and alcohols are
high, and all these substances can dissolve directly in the lipid bilayer and diffuse through
the cell membrane in the same manner that diffusion of water solutes occurs in a watery
solution.
• Even though water is highly insoluble in the membrane lipids, it readily passes through
channels in protein molecules that penetrate all the way through the membrane.
• Many of the body’s cell membranes contain protein “pores” called aquaporins that
selectively permit rapid passage of water through the membrane. For example, diffusion of
water through the red blood cell membrane.
• Other lipid-insoluble molecules can pass through the protein pore channels in the same
way as water molecules if they are water soluble and small enough. However, as they
become larger, their penetration falls off rapidly. For example, diffusion of urea molecules
through cell membrane.
SELECTI
VE
PERMEABILI
TY AND
“GATING
”
OF
CHANNELS
The protein channels are distinguished by two
important characteristics:
They are often selectively permeable to certain
substances, and
Many of the channels can be opened or closed by
gates that are regulated by:
Electrical signals (voltage-gated channels), or
Chemicals that bind to the channel proteins (ligand-
gated channels).
Selective Permeability of Protein Channels
• Many of the protein channels are highly selective for transport of one or
more specific ions or molecules. This selectivity results from the
characteristics of the channel, such as its diameter, its shape, and the
nature of the electrical charges and chemical bonds along its inside
surfaces.
• Different selectivity filters for the various ion channels are believed to
determine, in large part, the specificity of various channels for cations or
anions or for particular ions, such as sodium (Na+), potassium (K+),
and calcium (Ca++), that gain access to the channels.
Potassium channels permit passage of
potassium ions across the cell membrane about 1000
times more readily than they permit passage of
sodium ions.
Potassium channels have a tetrameric
structure consisting of four identical protein subunits
surrounding a central pore. At the top of the channel
pore are pore loops that form a narrow selectivity filter.
Lining the selectivity filter are carbonyl oxygens. When
hydrated potassium ions enter the selectivity filter,
they interact with the carbonyl oxygens and shed most
of their bound water molecules, permitting the
dehydrated potassium ions to pass through the
channel. The carbonyl oxygens are too far apart,
however, to enable them to interact closely with the
smaller sodium ions, which are therefore effectively
excluded by the selectivity filter from passing through
Gating of protein channels provides a means
of controlling ion permeability of the channels. This
mechanism is shown in selective gating of both
sodium (Na+) and potassium ions (K+). It is believed
that some of the gates are actual gate like
extensions of the transport protein molecule, which
can close the opening of the channel or can be lifted
away from the opening by a conformational change
in the shape of the protein molecule itself.
The opening and closing of gates are
controlled in two principal ways:
1. Voltage gating
2. Chemical (ligand) gating
Typesof Gating
Voltage gating:
In the case of voltage gating, the molecular
conformation of the gate or of its chemical bonds responds
to the electrical potential across the cell membrane. E.g.
Voltage gating of sodium and potassium ions in neurons.
Chemical (ligand) gating:
Some protein channel gates are opened by the
binding of a chemical substance (a ligand) with the
protein, which causes a conformational or chemical
bonding change in the protein molecule that opens or
closes the gate. One of the most important instances of
chemical gating is the effect of acetylcholine on the so-
called acetylcholine channel.
This figure shows two recordings of electrical current
flowing through a single sodium channel when there
was an approximate 25-millivolt potential gradient
across the membrane. It should be noted that the
channel conducts current in an all-or-none fashion.
That is, the gate of the channel snaps open and then
snaps closed, with each open state lasting for only a
fraction of a millisecond up to several milliseconds,
demonstrating the rapidity with which changes can
occur during the opening and closing of the protein
molecular gates.
Facilitated diffusion is also called carrier-mediated diffusion because a substance
transported in this manner diffuses through the membrane with the help of a specific carrier
protein. That is, the carrier facilitates diffusion of the substance to the other side. E.g.
Glucose and most of the amino acids.
Mechanism of Action
Facilitated diffusion is carried out by a carrier
protein with a pore large enough to transport a
specific molecule partway through. It also has a
binding “receptor” on the inside of the protein carrier.
The molecule to be transported enters the pore and
becomes bound. Then, in a fraction of a second, a
conformational or chemical change occurs in the
carrier protein, so the pore now opens to the opposite
side of the membrane. Because the binding force of
the receptor is weak, the thermal motion of the
attached molecule causes it to break away and be
released on the opposite side of the membrane.
Difference between Facilitated
diffusion and simple diffusion
according to Rate of diffusion:
Although the rate of simple diffusion through
an open channel increases proportionately with the
concentration of the diffusing substance, in facilitated
diffusion the rate of diffusion approaches a maximum,
called Vmax, as the concentration of the diffusing
substance increases.
This is because the rate at which molecules
can be transported by this mechanism can never be
greater than the rate at which the carrier protein
molecule can undergo change back and forth
between its two states.
Factors affecting net rate of diffusion
Concentration Difference Across a Membrane:
The rate at which the substance diffuses inward is proportional to
the concentration of molecules on the outside because this concentration
determines how many molecules strike the outside of the membrane each
second. Conversely, the rate at which molecules diffuse outward is
proportional to their concentration inside the membrane. Therefore, the rate
of net diffusion into the cell is proportional to the concentration on the outside
minus the concentration on the inside, or:
Net diffusion ∝ (Co – Ci)
in which Co is concentration outside and Ci is concentration inside (fig. A).
Membrane Electrical Potential:
If an electrical potential is applied across the membrane, as
shown in Figure, the electrical charges of the ions cause them to move
through the membrane even though no concentration difference exists to
cause movement.
At normal body temperature, the rate of diffusion across a cell
membrane is guided by the difference in electric potential (fig. B).
Factors affecting net rate of diffusion
Pressure Difference Across a Membrane:
At times, considerable pressure difference develops
between the two sides of a diffusible membrane. For example,
The pressure is about 20 mm Hg greater inside the capillary
than outside.
Pressure actually means the sum of all the forces of
the different molecules striking a unit surface area at a given
instant. Therefore, having a higher pressure on one side of a
membrane than on the other side means that the sum of all the
forces of the molecules striking the channels on that side of the
membrane is greater than on the other side.
The result is that increased amounts of energy are
available to cause net movement of molecules from the high-
pressure side toward the low-pressure side.
Thus diffusion occurs from high pressure to low
pressure zone.
By far the most abundant substance that
diffuses through the cell membrane is water. Enough
water ordinarily diffuses in each direction through the
red blood cell membrane per second to equal about 100
times the volume of the cell itself. Yet normally the
amount that diffuses in the two directions is balanced so
precisely that zero net movement of water occurs.
Therefore, the volume of the cell remains constant.
However, under certain conditions, a concentration
difference for water can develop across a membrane.
When this concentration difference for water develops,
net movement of water does occur across the cell
membrane, causing the cell to either swell or shrink,
depending on the direction of the water movement. This
process of net movement of water caused by a
concentration difference of water is called osmosis.
The amount of pressure required to stop osmosis is
called the osmotic pressure of the solution.
The principle of a pressure difference opposing
osmosis is demonstrated in figure, which shows a selectively
permeable membrane separating two columns of fluid, one
containing pure water and the other containing a solution of
water and any solute that will not penetrate the membrane.
Osmosis of water from chamber B into chamber A causes the
levels of the fluid columns to become farther and farther apart,
until eventually a pressure difference develops between the two
sides of the membrane great enough to oppose the osmotic
effect. The pressure difference across the membrane at this
point is equal to the osmotic pressure of the solution that
contains the nondiffusible solute.
Active Transport
Introduction
 At times, a large concentration of a substance is required in the intracellular fluid even though the
extracellular fluid contains only a small concentration. This situation is true, for instance, for
potassium ions. Conversely, it is important to keep the concentrations of other ions very low inside
the cell even though their concentrations in the extracellular fluid are great. This situation is
especially true for sodium ions. Neither of these two effects could occur by simple diffusion.
Instead, some energy source must cause excess movement of potassium ions to the inside of cells
and excess movement of sodium ions to the outside of cells. When a cell membrane moves
molecules or ions “uphill” against a concentration gradient (or “uphill” against an electrical or
pressure gradient), the process is called active transport.
 Different substances that are actively transported through at least some cell membranes include
sodium, potassium, calcium, iron, hydrogen, chloride, iodide, and urate ions, several different
sugars, and most of the amino acids.
Three basic
requirements:
1. Energy
2. Carrier protein
3. ATPase enzyme
Types of Active Transport
 Active transport is divided into two types according to the
source of the energy used to facilitate the transport:
 Primary active transport,
 Secondary active transport.
 In primary active transport, the energy is derived directly
from breakdown of adenosine triphosphate (ATP) or some
other high-energy phosphate compound.
 In secondary active transport, the energy is derived
secondarily from energy that has been stored in the form of
ionic concentration differences of secondary molecular or
ionic substances between the two sides of a cell
membrane, created originally by primary active transport.
Active
Transport
Primary Active
Transport
Secondary Active
Transport
Primary Active
transport
In primary active
transport, the energy is
derived directly from
breakdown of adenosine
triphosphate (ATP) or some
other high-energy phosphate
compound.
Among the substances
that are transported by
primary active transport
sodium, potassium, calcium,
hydrogen, chloride, etc. are a
few exaples.
It is a transport process that
pumps sodium ions outward
through the cell membrane of all
cells and at the same time pumps
potassium ions from the outside to
the inside.
This pump is responsible for
maintaining the sodium and
potassium concentration
differences across the cell
membrane, as well as for
establishing a negative electrical
voltage inside the cells.
The carrier protein is a complex of
two separate globular proteins—a larger
one called the α subunit, with a molecular
weight of about 100,000, and a smaller
one called the β subunit, with a molecular
weight of about 55,000. Although the
function of the smaller protein is not
known (except that it might anchor the
protein complex in the lipid membrane),
the larger protein has three specific
features that are important for the
functioning of the pump:
1. It has three binding sites for sodium
ions on the portion of the protein that
protrudes to the inside of the cell.
2. It has two binding sites for potassium
ions on the outside.
3. The inside portion of this protein near
the sodium binding sites has
adenosine triphosphatase (ATPase)
activity.
When two potassium ions bind on
the outside of the carrier protein and three
sodium ions bind on the inside, the ATPase
function of the protein becomes activated.
Activation of the ATPase function leads to
cleavage of one molecule of ATP, splitting
it to adenosine diphosphate (ADP) and
liberating a high-energy phosphate bond of
energy. This liberated energy is then
believed to cause a chemical and
conformational change in the protein
carrier molecule, extruding the three
sodium ions to the outside and the two
potassium ions to the inside.
Controlling Cell Volume
One of the most important
functions of the Na+-K+ pump is to
control the volume of each cell. Inside
the cell are large numbers of proteins
and other organic molecules that
cannot escape from the cell. Most of
these proteins and other organic
molecules are negatively charged
and therefore attract large numbers of
potassium, sodium, and other positive
ions as well. All these molecules and
ions then cause osmosis of water to
the interior of the cell. Unless this
process is checked, the cell will swell
indefinitely until it bursts. The normal
mechanism for preventing this
outcome is the Na+-K+ pump.
Electrogenic Nature of the Na+-K+
Pump
The fact that the Na+-K+
pump moves three Na+ ions to the
exterior for every two K+ ions that are
moved to the interior means that a
net of one positive charge is moved
from the interior of the cell to the
exterior for each cycle of the pump.
This action creates positivity outside
the cell but results in a deficit of
positive ions inside the cell; that is, it
causes negativity on the inside.
Therefore, the Na+-K+ pump is said
to be electrogenic because it creates
an electrical potential across the cell
membrane.
Pathologies
Energetics of Primary Active Transport
The amount of energy required to transport a substance actively through
a membrane is determined by how much the substance is concentrated
during transport. Compared with the energy required to concentrate a
substance 10-fold, concentrating it 100-fold requires twice as much energy,
and concentrating it 1000-fold requires three times as much energy. In other
words, the energy required is proportional to the logarithm of the degree that
the substance is concentrated, as expressed by the following formula:
Energy (in calories per osmole) =1400 log
𝐶1
𝐶2
Secondary Active
transport
Secondary Active
Transport is of two types:
• Co-transport
• Counter transport
When sodium ions are transported out of cells by primary active transport, a
large concentration gradient of sodium ions across the cell membrane usually develops,
with high concentration outside the cell and low concentration inside. This gradient
represents a storehouse of energy because the excess sodium outside the cell
membrane is always attempting to diffuse to the interior. Under appropriate conditions,
this diffusion energy of sodium can pull other substances along with the sodium through
the cell membrane. This phenomenon, called co-transport, is one form of secondary
active transport.
Examples of co-transport are Glucose, amino acids, chlorine, iodine, urates etc.
The ions are transported in the same
direction
Co-Transport of
Glucose along with
Sodium Ions
The transport carrier protein has two
binding sites on its exterior side, one for sodium
and one for glucose. Also, the concentration of
sodium ions is high on the outside and low inside,
which provides energy for the transport. A special
property of the transport protein is that a
conformational change to allow sodium movement
to the interior will not occur until a glucose
molecule also attaches. When they both become
attached, the conformational change takes place,
and the sodium and glucose are transported to the
inside of the cell at the same time. Hence, this is a
sodium-glucose co-transport mechanism.
Sodium-glucose co-transporters are
especially important mechanisms in transporting
glucose across renal and intestinal epithelial cells.
In counter-transport, sodium ions again attempt to diffuse to the interior of the
cell because of their large concentration gradient. However, this time, the substance to
be transported is on the inside of the cell and must be transported to the outside.
Therefore, the sodium ion binds to the carrier protein where it projects to the exterior
surface of the membrane, while the substance to be counter-transported binds to the
interior projection of the carrier protein. Once both have become bound, a
conformational change occurs, and energy released by the action of the sodium ion
moving to the interior causes the other substance to move to the exterior.
The ions are transported in the opposite direction
Counter-Transport of
Calcium and
Hydrogen Ions along
with Sodium Ions
Two especially important counter-transport
mechanisms are sodium-calcium and sodium-hydrogen
counter-transport.
Sodium-calcium counter-transport occurs
through all or almost all cell membranes, with sodium
ions moving to the interior and calcium ions to the
exterior; both are bound to the same transport protein in
a counter-transport mode. This mechanism is in addition
to primary active transport of calcium that occurs in
some cells.
Sodium-hydrogen counter-transport occurs in
several tissues. An especially important example is in
the proximal tubules of the kidneys, where sodium ions
move from the lumen of the tubule to the interior of the
tubular cell while hydrogen ions are counter-transported
into the tubule lumen.
ACTIVE TRANSPORT THROUGH
CELLULAR SHEETS
At many places in the body, substances must be
transported all the way through a cellular sheet
instead of simply through the cell membrane.
Transport of this type occurs through the intestinal
epithelium, epithelium of the renal tubules, epithelium
of all exocrine glands, epithelium of the gallbladder,
and membrane of the choroid plexus of the brain,
along with other membranes.
The basic mechanism for transport of a substance
through a cellular sheet is
• active transport through the cell membrane on
one side of the transporting cells in the sheet, and
then
• either simple diffusion or facilitated diffusion
through the membrane on the opposite side of the
cell.

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Transport across cell membrane

  • 2. CELL MEMBRANE  This membrane consists almost entirely of a lipid bilayer, but it also contains large numbers of protein molecules in the lipid, many of which penetrate all the way through the membrane.  The lipid bilayer is not miscible with either the extracellular fluid or the intracellular fluid. Therefore, it constitutes a barrier against movement of water molecules and water-soluble substances between the extracellular and intracellular fluid compartments.  The protein molecules in the membrane have entirely different properties for transporting substances. Their molecular structures interrupt the continuity of the lipid bilayer, constituting an alternative pathway through the cell membrane. Many of these penetrating proteins can function as transport proteins.
  • 3.  Channel proteins: These proteins have watery spaces all the way through the molecule and allow free movement of water, as well as selected ions or molecules.  Carrier proteins: These Proteins bind with molecules or ions that are to be transported, and conformational changes in the protein molecules then move the substances through the interstices of the protein to the other side of the membrane. Channel proteins and carrier proteins are usually selective for the types of molecules or ions that are allowed to cross the membrane. Transport Proteins Channel Proteins Carrier proteins
  • 4. Transport through Cell Membrane Transport through the cell membrane, either directly through the lipid bilayer or through the proteins, occurs via one of two basic processes: • Active transport • Passive transport (Diffusion) Transport Active Transport Primary Secondary Passive Transport Simple diffusion Facilitated diffusion
  • 6. Simple Diffusion Simple diffusion can occur through the cell membrane by two pathways: 1. through the interstices of the lipid bilayer if the diffusing substance is lipid soluble, 2. through watery channels that penetrate all the way through some of the large transport proteins.
  • 7. • An important factor that determines how rapidly a substance diffuses through the lipid bilayer is the lipid solubility of the substance. Rate of diffusion ∝ lipid solubility of substance • For example, the lipid solubilities of oxygen, nitrogen, carbon dioxide, and alcohols are high, and all these substances can dissolve directly in the lipid bilayer and diffuse through the cell membrane in the same manner that diffusion of water solutes occurs in a watery solution.
  • 8. • Even though water is highly insoluble in the membrane lipids, it readily passes through channels in protein molecules that penetrate all the way through the membrane. • Many of the body’s cell membranes contain protein “pores” called aquaporins that selectively permit rapid passage of water through the membrane. For example, diffusion of water through the red blood cell membrane. • Other lipid-insoluble molecules can pass through the protein pore channels in the same way as water molecules if they are water soluble and small enough. However, as they become larger, their penetration falls off rapidly. For example, diffusion of urea molecules through cell membrane.
  • 9. SELECTI VE PERMEABILI TY AND “GATING ” OF CHANNELS The protein channels are distinguished by two important characteristics: They are often selectively permeable to certain substances, and Many of the channels can be opened or closed by gates that are regulated by: Electrical signals (voltage-gated channels), or Chemicals that bind to the channel proteins (ligand- gated channels).
  • 10. Selective Permeability of Protein Channels • Many of the protein channels are highly selective for transport of one or more specific ions or molecules. This selectivity results from the characteristics of the channel, such as its diameter, its shape, and the nature of the electrical charges and chemical bonds along its inside surfaces. • Different selectivity filters for the various ion channels are believed to determine, in large part, the specificity of various channels for cations or anions or for particular ions, such as sodium (Na+), potassium (K+), and calcium (Ca++), that gain access to the channels.
  • 11. Potassium channels permit passage of potassium ions across the cell membrane about 1000 times more readily than they permit passage of sodium ions. Potassium channels have a tetrameric structure consisting of four identical protein subunits surrounding a central pore. At the top of the channel pore are pore loops that form a narrow selectivity filter. Lining the selectivity filter are carbonyl oxygens. When hydrated potassium ions enter the selectivity filter, they interact with the carbonyl oxygens and shed most of their bound water molecules, permitting the dehydrated potassium ions to pass through the channel. The carbonyl oxygens are too far apart, however, to enable them to interact closely with the smaller sodium ions, which are therefore effectively excluded by the selectivity filter from passing through
  • 12. Gating of protein channels provides a means of controlling ion permeability of the channels. This mechanism is shown in selective gating of both sodium (Na+) and potassium ions (K+). It is believed that some of the gates are actual gate like extensions of the transport protein molecule, which can close the opening of the channel or can be lifted away from the opening by a conformational change in the shape of the protein molecule itself. The opening and closing of gates are controlled in two principal ways: 1. Voltage gating 2. Chemical (ligand) gating
  • 13. Typesof Gating Voltage gating: In the case of voltage gating, the molecular conformation of the gate or of its chemical bonds responds to the electrical potential across the cell membrane. E.g. Voltage gating of sodium and potassium ions in neurons. Chemical (ligand) gating: Some protein channel gates are opened by the binding of a chemical substance (a ligand) with the protein, which causes a conformational or chemical bonding change in the protein molecule that opens or closes the gate. One of the most important instances of chemical gating is the effect of acetylcholine on the so- called acetylcholine channel.
  • 14. This figure shows two recordings of electrical current flowing through a single sodium channel when there was an approximate 25-millivolt potential gradient across the membrane. It should be noted that the channel conducts current in an all-or-none fashion. That is, the gate of the channel snaps open and then snaps closed, with each open state lasting for only a fraction of a millisecond up to several milliseconds, demonstrating the rapidity with which changes can occur during the opening and closing of the protein molecular gates.
  • 15. Facilitated diffusion is also called carrier-mediated diffusion because a substance transported in this manner diffuses through the membrane with the help of a specific carrier protein. That is, the carrier facilitates diffusion of the substance to the other side. E.g. Glucose and most of the amino acids.
  • 16. Mechanism of Action Facilitated diffusion is carried out by a carrier protein with a pore large enough to transport a specific molecule partway through. It also has a binding “receptor” on the inside of the protein carrier. The molecule to be transported enters the pore and becomes bound. Then, in a fraction of a second, a conformational or chemical change occurs in the carrier protein, so the pore now opens to the opposite side of the membrane. Because the binding force of the receptor is weak, the thermal motion of the attached molecule causes it to break away and be released on the opposite side of the membrane.
  • 17. Difference between Facilitated diffusion and simple diffusion according to Rate of diffusion: Although the rate of simple diffusion through an open channel increases proportionately with the concentration of the diffusing substance, in facilitated diffusion the rate of diffusion approaches a maximum, called Vmax, as the concentration of the diffusing substance increases. This is because the rate at which molecules can be transported by this mechanism can never be greater than the rate at which the carrier protein molecule can undergo change back and forth between its two states.
  • 18. Factors affecting net rate of diffusion Concentration Difference Across a Membrane: The rate at which the substance diffuses inward is proportional to the concentration of molecules on the outside because this concentration determines how many molecules strike the outside of the membrane each second. Conversely, the rate at which molecules diffuse outward is proportional to their concentration inside the membrane. Therefore, the rate of net diffusion into the cell is proportional to the concentration on the outside minus the concentration on the inside, or: Net diffusion ∝ (Co – Ci) in which Co is concentration outside and Ci is concentration inside (fig. A). Membrane Electrical Potential: If an electrical potential is applied across the membrane, as shown in Figure, the electrical charges of the ions cause them to move through the membrane even though no concentration difference exists to cause movement. At normal body temperature, the rate of diffusion across a cell membrane is guided by the difference in electric potential (fig. B).
  • 19. Factors affecting net rate of diffusion Pressure Difference Across a Membrane: At times, considerable pressure difference develops between the two sides of a diffusible membrane. For example, The pressure is about 20 mm Hg greater inside the capillary than outside. Pressure actually means the sum of all the forces of the different molecules striking a unit surface area at a given instant. Therefore, having a higher pressure on one side of a membrane than on the other side means that the sum of all the forces of the molecules striking the channels on that side of the membrane is greater than on the other side. The result is that increased amounts of energy are available to cause net movement of molecules from the high- pressure side toward the low-pressure side. Thus diffusion occurs from high pressure to low pressure zone.
  • 20. By far the most abundant substance that diffuses through the cell membrane is water. Enough water ordinarily diffuses in each direction through the red blood cell membrane per second to equal about 100 times the volume of the cell itself. Yet normally the amount that diffuses in the two directions is balanced so precisely that zero net movement of water occurs. Therefore, the volume of the cell remains constant. However, under certain conditions, a concentration difference for water can develop across a membrane. When this concentration difference for water develops, net movement of water does occur across the cell membrane, causing the cell to either swell or shrink, depending on the direction of the water movement. This process of net movement of water caused by a concentration difference of water is called osmosis.
  • 21. The amount of pressure required to stop osmosis is called the osmotic pressure of the solution. The principle of a pressure difference opposing osmosis is demonstrated in figure, which shows a selectively permeable membrane separating two columns of fluid, one containing pure water and the other containing a solution of water and any solute that will not penetrate the membrane. Osmosis of water from chamber B into chamber A causes the levels of the fluid columns to become farther and farther apart, until eventually a pressure difference develops between the two sides of the membrane great enough to oppose the osmotic effect. The pressure difference across the membrane at this point is equal to the osmotic pressure of the solution that contains the nondiffusible solute.
  • 23. Introduction  At times, a large concentration of a substance is required in the intracellular fluid even though the extracellular fluid contains only a small concentration. This situation is true, for instance, for potassium ions. Conversely, it is important to keep the concentrations of other ions very low inside the cell even though their concentrations in the extracellular fluid are great. This situation is especially true for sodium ions. Neither of these two effects could occur by simple diffusion. Instead, some energy source must cause excess movement of potassium ions to the inside of cells and excess movement of sodium ions to the outside of cells. When a cell membrane moves molecules or ions “uphill” against a concentration gradient (or “uphill” against an electrical or pressure gradient), the process is called active transport.  Different substances that are actively transported through at least some cell membranes include sodium, potassium, calcium, iron, hydrogen, chloride, iodide, and urate ions, several different sugars, and most of the amino acids. Three basic requirements: 1. Energy 2. Carrier protein 3. ATPase enzyme
  • 24. Types of Active Transport  Active transport is divided into two types according to the source of the energy used to facilitate the transport:  Primary active transport,  Secondary active transport.  In primary active transport, the energy is derived directly from breakdown of adenosine triphosphate (ATP) or some other high-energy phosphate compound.  In secondary active transport, the energy is derived secondarily from energy that has been stored in the form of ionic concentration differences of secondary molecular or ionic substances between the two sides of a cell membrane, created originally by primary active transport. Active Transport Primary Active Transport Secondary Active Transport
  • 25. Primary Active transport In primary active transport, the energy is derived directly from breakdown of adenosine triphosphate (ATP) or some other high-energy phosphate compound. Among the substances that are transported by primary active transport sodium, potassium, calcium, hydrogen, chloride, etc. are a few exaples.
  • 26. It is a transport process that pumps sodium ions outward through the cell membrane of all cells and at the same time pumps potassium ions from the outside to the inside. This pump is responsible for maintaining the sodium and potassium concentration differences across the cell membrane, as well as for establishing a negative electrical voltage inside the cells.
  • 27. The carrier protein is a complex of two separate globular proteins—a larger one called the α subunit, with a molecular weight of about 100,000, and a smaller one called the β subunit, with a molecular weight of about 55,000. Although the function of the smaller protein is not known (except that it might anchor the protein complex in the lipid membrane), the larger protein has three specific features that are important for the functioning of the pump: 1. It has three binding sites for sodium ions on the portion of the protein that protrudes to the inside of the cell. 2. It has two binding sites for potassium ions on the outside. 3. The inside portion of this protein near the sodium binding sites has adenosine triphosphatase (ATPase) activity.
  • 28. When two potassium ions bind on the outside of the carrier protein and three sodium ions bind on the inside, the ATPase function of the protein becomes activated. Activation of the ATPase function leads to cleavage of one molecule of ATP, splitting it to adenosine diphosphate (ADP) and liberating a high-energy phosphate bond of energy. This liberated energy is then believed to cause a chemical and conformational change in the protein carrier molecule, extruding the three sodium ions to the outside and the two potassium ions to the inside.
  • 29. Controlling Cell Volume One of the most important functions of the Na+-K+ pump is to control the volume of each cell. Inside the cell are large numbers of proteins and other organic molecules that cannot escape from the cell. Most of these proteins and other organic molecules are negatively charged and therefore attract large numbers of potassium, sodium, and other positive ions as well. All these molecules and ions then cause osmosis of water to the interior of the cell. Unless this process is checked, the cell will swell indefinitely until it bursts. The normal mechanism for preventing this outcome is the Na+-K+ pump. Electrogenic Nature of the Na+-K+ Pump The fact that the Na+-K+ pump moves three Na+ ions to the exterior for every two K+ ions that are moved to the interior means that a net of one positive charge is moved from the interior of the cell to the exterior for each cycle of the pump. This action creates positivity outside the cell but results in a deficit of positive ions inside the cell; that is, it causes negativity on the inside. Therefore, the Na+-K+ pump is said to be electrogenic because it creates an electrical potential across the cell membrane.
  • 31. Energetics of Primary Active Transport The amount of energy required to transport a substance actively through a membrane is determined by how much the substance is concentrated during transport. Compared with the energy required to concentrate a substance 10-fold, concentrating it 100-fold requires twice as much energy, and concentrating it 1000-fold requires three times as much energy. In other words, the energy required is proportional to the logarithm of the degree that the substance is concentrated, as expressed by the following formula: Energy (in calories per osmole) =1400 log 𝐶1 𝐶2
  • 32. Secondary Active transport Secondary Active Transport is of two types: • Co-transport • Counter transport
  • 33. When sodium ions are transported out of cells by primary active transport, a large concentration gradient of sodium ions across the cell membrane usually develops, with high concentration outside the cell and low concentration inside. This gradient represents a storehouse of energy because the excess sodium outside the cell membrane is always attempting to diffuse to the interior. Under appropriate conditions, this diffusion energy of sodium can pull other substances along with the sodium through the cell membrane. This phenomenon, called co-transport, is one form of secondary active transport. Examples of co-transport are Glucose, amino acids, chlorine, iodine, urates etc. The ions are transported in the same direction
  • 34. Co-Transport of Glucose along with Sodium Ions The transport carrier protein has two binding sites on its exterior side, one for sodium and one for glucose. Also, the concentration of sodium ions is high on the outside and low inside, which provides energy for the transport. A special property of the transport protein is that a conformational change to allow sodium movement to the interior will not occur until a glucose molecule also attaches. When they both become attached, the conformational change takes place, and the sodium and glucose are transported to the inside of the cell at the same time. Hence, this is a sodium-glucose co-transport mechanism. Sodium-glucose co-transporters are especially important mechanisms in transporting glucose across renal and intestinal epithelial cells.
  • 35. In counter-transport, sodium ions again attempt to diffuse to the interior of the cell because of their large concentration gradient. However, this time, the substance to be transported is on the inside of the cell and must be transported to the outside. Therefore, the sodium ion binds to the carrier protein where it projects to the exterior surface of the membrane, while the substance to be counter-transported binds to the interior projection of the carrier protein. Once both have become bound, a conformational change occurs, and energy released by the action of the sodium ion moving to the interior causes the other substance to move to the exterior. The ions are transported in the opposite direction
  • 36. Counter-Transport of Calcium and Hydrogen Ions along with Sodium Ions Two especially important counter-transport mechanisms are sodium-calcium and sodium-hydrogen counter-transport. Sodium-calcium counter-transport occurs through all or almost all cell membranes, with sodium ions moving to the interior and calcium ions to the exterior; both are bound to the same transport protein in a counter-transport mode. This mechanism is in addition to primary active transport of calcium that occurs in some cells. Sodium-hydrogen counter-transport occurs in several tissues. An especially important example is in the proximal tubules of the kidneys, where sodium ions move from the lumen of the tubule to the interior of the tubular cell while hydrogen ions are counter-transported into the tubule lumen.
  • 37. ACTIVE TRANSPORT THROUGH CELLULAR SHEETS At many places in the body, substances must be transported all the way through a cellular sheet instead of simply through the cell membrane. Transport of this type occurs through the intestinal epithelium, epithelium of the renal tubules, epithelium of all exocrine glands, epithelium of the gallbladder, and membrane of the choroid plexus of the brain, along with other membranes. The basic mechanism for transport of a substance through a cellular sheet is • active transport through the cell membrane on one side of the transporting cells in the sheet, and then • either simple diffusion or facilitated diffusion through the membrane on the opposite side of the cell.