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Molecular Biology of the Cell by Bruce Alberts, Alexander Johnson, Julian Lewis, David Morgan, Martin Raff, Keith Roberts, Peter Walter by by Bruce Alberts, Alexander Johnson, Julian Lewis, David Morg

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602 Chapter 11: Membrane Transport of Small Molecules and the Electrical Properties of Membranes

lipid

bilayer

LIGHT

electrochemical

gradient

Figure 11–7 Three ways of driving

active transport. The actively transported

molecule is shown in orange, and the

energy source is shown in red. Redox

driven active transport is discussed in

Chapter 14 (see Figures 14–18 and 14–19).

P

ADP

COUPLED

TRANSPORTER

ATP

ATP-DRIVEN

PUMP

LIGHT-DRIVEN

PUMP

K m ; they are called uniporters. Others function as coupled transporters, in which

the transfer of one solute strictly depends on the transport of a second. Coupled

transport involves either the simultaneous transfer of a second solute in the same

direction, performed by symporters (also called co-transporters), or the transfer

of a second solute in the opposite MBoC6 direction, m11.07/11.07 performed by antiporters (also called

exchangers) (Figure 11–8).

The tight coupling between the transfer of two solutes allows the coupled

transporters to harvest the energy stored in the electrochemical gradient of one

solute, typically an inorganic ion, to transport the other. In this way, the free

energy released during the movement of an inorganic ion down an electrochemical

gradient is used as the driving force to pump other solutes uphill, against

their electrochemical gradient. This strategy can work in either direction; some

coupled transporters function as symporters, others as antiporters. In the plasma

membrane of animal cells, Na + is the usual co-transported ion because its electrochemical

gradient provides a large driving force for the active transport of a

second molecule. The Na + that enters the cell during coupled transport is subsequently

pumped out by an ATP-driven Na + -K + pump in the plasma membrane

(as we discuss later), which, by maintaining the Na + gradient, indirectly drives

the coupled transport. Such ion-driven coupled transporters as just described

are said to mediate secondary active transport. In contrast, ATP-driven pumps are

said to mediate primary active transport because in these the free energy of ATP

hydrolysis is used to directly drive the transport of a solute against its concentration

gradient.

Intestinal and kidney epithelial cells contain a variety of symporters that are

driven by the Na + gradient across the plasma membrane. Each Na + -driven symporter

is specific for importing a small group of related sugars or amino acids

into the cell. Because the Na + tends to move into the cell down its electrochemical

gradient, the sugar or amino acid is, in a sense, “dragged” into the cell with

it. The greater the electrochemical gradient for Na + , the more solute is pumped

transported molecule

co-transported ion

lipid

bilayer

UNIPORT SYMPORT ANTIPORT

coupled transport

Figure 11–8 This schematic diagram

shows transporters functioning as

uniporters, symporters, and antiporters

(Movie 11.1).

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