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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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Na +<br />

K +<br />

BIOLOGICAL BASIS FOR R ADIATION SAFETY 287<br />

pure-water side. Water will therefore flow through the semipermeable barrier from<br />

the pure-water side in<strong>to</strong> the solution side by osmosis, and the water in the solution<br />

arm will rise. Water will continue <strong>to</strong> flow through the barrier, and the solution column<br />

will continue <strong>to</strong> rise, until the hydrostatic pressure due <strong>to</strong> the increased height of<br />

the column of water is great enough <strong>to</strong> prevent further inflow of water through<br />

the semipermeable barrier. The hydrostatic pressure needed <strong>to</strong> prevent further flow<br />

through the barrier is called the osmotic pressure of the solution. Osmotic pressure<br />

is determined by the concentration of the solution and increases with increasing<br />

concentration.<br />

Biological membranes may be selectively permeable <strong>to</strong> various different<br />

molecules. This selective permeability, which allows only certain ions <strong>to</strong> pass, is<br />

responsible for the electrical potential differences that form the basis for the operation<br />

of the nervous system and muscles, including the cardiac muscle. Consider<br />

the arms of a U tube that are separated by a membrane that allows only K + ions <strong>to</strong><br />

pass through, as in Figure 7-3. Let us pour a solution containing a relatively high<br />

concentration of KCl and a low concentration of NaCl in<strong>to</strong> one arm of the U tube,<br />

and a KCl–NaCl solution that is relatively more concentrated in Na + than in K +<br />

in<strong>to</strong> the other arm. The solutions on both sides of the membrane are electrically<br />

neutral. However, since the membrane is permeable <strong>to</strong> K + ions, the K + ions will<br />

diffuse through the membrane from the more <strong>to</strong> the less concentrated K + solution.<br />

This transfer of K + ions results in a net loss of positive ions on one side of the membrane<br />

and a net gain of positive ions on the other side, thus upsetting the electrical<br />

neutrality. Since one side will now have a net positive charge and the other a net<br />

negative charge, these opposite charges will attract each other and will migrate <strong>to</strong><br />

the membrane separating the two solutions. This accumulation of positive ions on<br />

one side and negative ions on the other side of the membrane leads <strong>to</strong> an electrical<br />

potential difference across the membrane. This potential difference continues <strong>to</strong><br />

increase as more K + ions move through the membrane until the built-up positive<br />

potential is great enough <strong>to</strong> prevent more positively charged K ions from passing<br />

through the membrane. Passage of ions from a region of high <strong>to</strong> low concentration<br />

is accomplished without the expenditure of energy. However, transfer of ions against<br />

a concentration gradient, which is called active transport, requires the expenditure<br />

of energy.<br />

Na +<br />

K +<br />

Cl - Cl -<br />

–<br />

–<br />

–<br />

–<br />

–<br />

–<br />

–<br />

–<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

Polarized<br />

Membrane<br />

Figure 7-3. Schematic illustration of ionic transport, in which<br />

the membrane is permeable only <strong>to</strong> the K + ion. The accumulation<br />

of positive charges on one side of the membrane and negative<br />

ions on the other side leads <strong>to</strong> a potential difference across the<br />

membrane.

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