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    The Specific Growth Rates of Tissues: A Review and a Re-Evaluation

    Source: Journal of Biomechanical Engineering:;2011:;volume( 133 ):;issue: 004::page 41001
    Author:
    Stephen C. Cowin
    DOI: 10.1115/1.4003341
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The first objective of this review and re-evaluation is to present a brief history of efforts to mathematically model the growth of tissues. The second objective is to place this historical material in a current perspective where it may be of help in future research. The overall objective is to look backward in order to see ways forward. It is noted that two distinct methods of imaging or modeling the growth of an organism were inspired over 70 years ago by (1915, “XXVII Morphology and Mathematics,” Trans. - R. Soc. Edinbrgh, 50, pp. 857–895; 1942, On Growth and Form, Cambridge University Press, Cambridge, UK) method of coordinate transformations to study the growth and form of organisms. One is based on the solid mechanics concept of the deformation of an object, and the other is based on the fluid mechanics concept of the velocity field of a fluid. The solid mechanics model is called the distributed continuous growth (DCG) model by (1981, “Growth as a Finite Displacement Field,” Proceedings of the IUTAM Symposium on Finite Elasticity , D. E. Carlson and R. T. Shield, eds., Nijhoff, The Hague, pp. 348–355) and (1982, “Analytical Description of Growth,” J. Theor. Biol., 94, pp. 555–577), and the fluid mechanics model is called the graphical growth velocity field representation (GVFR) by (2010, “Continuum Kinematical Modeling of Mass Increasing Biological Growth,” Int. J. Eng. Sci., 48, pp. 1137–1145). The GVFR is a minimum or simple model based only on the assumption that a velocity field may be used effectively to illustrate experimental results concerning the temporal evolution of the size and shape of the organism that reveals the centers of growth and growth gradients first described by (1924, “Constant Differential Growth-Ratios and Their Significance,” Nature (London), 114, pp. 895–896; 1972, Problems of Relative Growth, 2nd ed., L. MacVeagh, ed., Dover, New York). It is the method with an independent future that some earlier writers considered as an aspect of the DCG model. The development of the DCG hypothesis and the mixture theory models into models for the predicted growth of an organism is taking longer because these models are complicated and the development and refinement of the basic concepts are slower.
    keyword(s): Biological tissues , Modeling , Gradients , Mixtures , Deformation AND Fluids ,
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      The Specific Growth Rates of Tissues: A Review and a Re-Evaluation

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    contributor authorStephen C. Cowin
    date accessioned2017-05-09T00:42:32Z
    date available2017-05-09T00:42:32Z
    date copyrightApril, 2011
    date issued2011
    identifier issn0148-0731
    identifier otherJBENDY-27203#041001_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/145454
    description abstractThe first objective of this review and re-evaluation is to present a brief history of efforts to mathematically model the growth of tissues. The second objective is to place this historical material in a current perspective where it may be of help in future research. The overall objective is to look backward in order to see ways forward. It is noted that two distinct methods of imaging or modeling the growth of an organism were inspired over 70 years ago by (1915, “XXVII Morphology and Mathematics,” Trans. - R. Soc. Edinbrgh, 50, pp. 857–895; 1942, On Growth and Form, Cambridge University Press, Cambridge, UK) method of coordinate transformations to study the growth and form of organisms. One is based on the solid mechanics concept of the deformation of an object, and the other is based on the fluid mechanics concept of the velocity field of a fluid. The solid mechanics model is called the distributed continuous growth (DCG) model by (1981, “Growth as a Finite Displacement Field,” Proceedings of the IUTAM Symposium on Finite Elasticity , D. E. Carlson and R. T. Shield, eds., Nijhoff, The Hague, pp. 348–355) and (1982, “Analytical Description of Growth,” J. Theor. Biol., 94, pp. 555–577), and the fluid mechanics model is called the graphical growth velocity field representation (GVFR) by (2010, “Continuum Kinematical Modeling of Mass Increasing Biological Growth,” Int. J. Eng. Sci., 48, pp. 1137–1145). The GVFR is a minimum or simple model based only on the assumption that a velocity field may be used effectively to illustrate experimental results concerning the temporal evolution of the size and shape of the organism that reveals the centers of growth and growth gradients first described by (1924, “Constant Differential Growth-Ratios and Their Significance,” Nature (London), 114, pp. 895–896; 1972, Problems of Relative Growth, 2nd ed., L. MacVeagh, ed., Dover, New York). It is the method with an independent future that some earlier writers considered as an aspect of the DCG model. The development of the DCG hypothesis and the mixture theory models into models for the predicted growth of an organism is taking longer because these models are complicated and the development and refinement of the basic concepts are slower.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleThe Specific Growth Rates of Tissues: A Review and a Re-Evaluation
    typeJournal Paper
    journal volume133
    journal issue4
    journal titleJournal of Biomechanical Engineering
    identifier doi10.1115/1.4003341
    journal fristpage41001
    identifier eissn1528-8951
    keywordsBiological tissues
    keywordsModeling
    keywordsGradients
    keywordsMixtures
    keywordsDeformation AND Fluids
    treeJournal of Biomechanical Engineering:;2011:;volume( 133 ):;issue: 004
    contenttypeFulltext
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