Molecular basis of the elastic properties of biological objectsMOLECULAR BASIS OF ELASTIC PROPERTIES
bioobject
The elastic properties and strength of tissues except bone, mainly
determined by the elastin and collagen fibers and their complexes.
Higher strength and modulus of elasticity of bone caused by the presence
"fiberglass" structures built of collagen and crystals
hydroxyapatite.
Proteins elastin and collagen are part of precisely those tissues that
continuously subjected to mechanical stresses. For example, in the lung
Collagen and elastin are respectively 12-20 and 5-10% by dry weight. In
wall of large blood vessels on these proteins may account for about
50% by dry weight. The ratio of elastin and collagen in
arterial wall changes in the course of the circulatory system. In the wall
Thoracic aortic elastin x 1/2 times as much as the abdominal aorta and other
large arteries is about 3 times less than collagen. since
mechanical properties of elastin and collagen fibers are not the same, the difference
in their contents, but also in the spatial arrangement within the vascular
the wall causes that the elastic properties of different vessels strongly
differ.
Elastin filaments have a relatively high elongation, ie. E.
low modulus of elasticity in tension along the fiber: (0,4-1,0) • 10e
N / m2. Collagen threads have an order of magnitude higher modulus
(0,5-1,0) • 107 N / m 2 m. Ie. Characterized by a low ability to
stretching. It is believed that in the tissues of elastin fibers are under
voltage even at moderate tension. Collagen fibers alone
are currently in a state of tension only when a strong deformation
Fabric: With a high modulus of elasticity and strength, these fibers
prevent rupture of tendons, blood vessel walls and other
fabrics with large mechanical loads, and provide light
alveolar tissue stabilization at high volumes. With a weak strain
tissue collagen strands are not stretched, but it deforms their network.
The most detailed nature of the deformation of tissue at various elongations studied
in skeletal muscle by thermodynamic methods. We will consider
muscle deformation under constant volume and its unchanged
temperature. According to the laws of thermodynamics (refer. Ch. One) change
muscle free energy during deformation by external force
f is the mechanical work / A / done on the muscle by
its elongation of A /. On the basis of the equation (1.2), in which the Academy of Sciences
= AU due to a constant volume, we get:
f = - TA [SIAl & [U / Al, (10.22)
where the subscript I denotes the dependence on the length. From this equation,
it is clear that the resulting tensile elastic muscle force (right-hand side
equation) is determined by the change in the entropy change in the internal and AtS
energy AtU. Of interest are the two extreme cases.
If AtU - 0, the elastic force is described by only the first term on the right
side of equation (10.22), and its occurrence is associated with a decrease in
entropy, as this term is positive in sign at AtS • <0.
The reduction in entropy indicates that the process should be released elongation
heat. This thermal effect is observed in the experiment on the muscle when it is
sprains, relevant section A in Fig. 78 Consequently, the
deformation is associated with a decrease in entropy, and its mechanism is
orientation of the moving parts of the protein molecules responsible for the elastic
muscle properties along the direction of the force /. Thus there is an ordering
the molecular structure of the muscles, reduces the number of possible conformations
(states) of proteins. Component - TAtS / Al in equation (10.22) is often
called thermokinetic elastic force.
Literature which was used:
Wikipedia- free encyclopedia which contain general information about mechanical properties of biological tissues.
Biophysics - Yuri Vladimirov- this book gives correct and true information information about mechanical properties of biological tissues.
Date: 2016-01-03; view: 885
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