Difference between revisions of "Diffusion - Physiology"
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| + | |backcolour = C1F0F6 | ||
| + | |linkpage =Transport Across Membranes - Physiology | ||
| + | |linktext =TRANSPORT ACROSS MEMBRANES | ||
| + | |maplink = Urinary System (Content Map) - Anatomy & Physiology | ||
| + | |pagetype =Anatomy | ||
| + | }} | ||
| + | <br> | ||
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==Introduction== | ==Introduction== | ||
| − | + | If gases or liquids are unevenly distributed, this inequality will be corrected by the movement of molecules from the region of high concentration to that of low. This is achieved by the process of diffusion. This works by the random '''thermal movement''' of molecules. If there is a gas present in an air tight room and then a door is opened into the next room the laws of probability state that some of the randomly moving molecules will escape through the door into the adjoining room and that eventually the concentrations in both rooms with be approximately the same. In the period between the door opening and the rooms having the same concentration net movement will be from the original room to the new room. This is because as there are more molecules in the original room there is an increased chance that these molecules will leave the room; and as there are few molecules in the second room there is a slim chance that they will move into the first room. | |
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| − | This works by the random '''thermal movement''' of molecules. If there is a gas present in an air tight room and then a door is opened into the next room | ||
==Ficks Law== | ==Ficks Law== | ||
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| − | '''L''' = distance separating the two areas | + | <big>'''Q = DA((C<sub>1</sub> - C<sub>2</sub>) ÷ L)'''</big> |
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| + | '''Q''' = the transport rate of a substance by diffusion | ||
| + | '''D''' = The diffusion coefficient | ||
| + | '''A''' = The cross sectional area which the substance is to diffuse across | ||
| + | '''C<sub>1</sub> C<sub>2</sub>''' = The concentrations in the two areas | ||
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| + | '''L''' = distance separating the two areas | ||
Ficks law demonstrates that the rate of diffusion can be maximised by increasing the area over which diffusion can occur, minimising the distance it has to occur over and increasing the gradient it occurs along. In the body it tends to be the former two which are taken into account when adapting surfaces for diffusion to occur over. | Ficks law demonstrates that the rate of diffusion can be maximised by increasing the area over which diffusion can occur, minimising the distance it has to occur over and increasing the gradient it occurs along. In the body it tends to be the former two which are taken into account when adapting surfaces for diffusion to occur over. | ||
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==Diffusion Through the Lipid Bilayer== | ==Diffusion Through the Lipid Bilayer== | ||
| − | * Lipid soluble substances are able to diffuse freely across the | + | * Lipid soluble substances are able to diffuse freely across the lipid bilayer of cells. |
| − | * This occurs passively down the concentration gradient. | + | * This obviously occurs passively down the concentration gradient. |
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| + | ==More Information== | ||
| − | + | If more information is need it can be found [http://en.wikipedia.org/wiki/Passive_diffusion here] | |
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Revision as of 11:02, 2 September 2008
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Introduction
If gases or liquids are unevenly distributed, this inequality will be corrected by the movement of molecules from the region of high concentration to that of low. This is achieved by the process of diffusion. This works by the random thermal movement of molecules. If there is a gas present in an air tight room and then a door is opened into the next room the laws of probability state that some of the randomly moving molecules will escape through the door into the adjoining room and that eventually the concentrations in both rooms with be approximately the same. In the period between the door opening and the rooms having the same concentration net movement will be from the original room to the new room. This is because as there are more molecules in the original room there is an increased chance that these molecules will leave the room; and as there are few molecules in the second room there is a slim chance that they will move into the first room.
Ficks Law
Q = DA((C1 - C2) ÷ L) Q = the transport rate of a substance by diffusion D = The diffusion coefficient A = The cross sectional area which the substance is to diffuse across C1 C2 = The concentrations in the two areas L = distance separating the two areas
Ficks law demonstrates that the rate of diffusion can be maximised by increasing the area over which diffusion can occur, minimising the distance it has to occur over and increasing the gradient it occurs along. In the body it tends to be the former two which are taken into account when adapting surfaces for diffusion to occur over.
Diffusion as a Transport Mechanism
Diffusion is very efficient over short distances and does not require energy. As such it is used in a variety of body systems where gradients and membranes suited to it are found. However over large distances diffusion is very slow.
Diffusion Through the Lipid Bilayer
- Lipid soluble substances are able to diffuse freely across the lipid bilayer of cells.
- This obviously occurs passively down the concentration gradient.
More Information
If more information is need it can be found here