# The Hyperthrophy Of The Tibia Induced By The Volley-Ball .

M Tsili

###### Keywords

hyperthrophy, internal bone remodeling, tibia, volley-ball

###### Citation

M Tsili. *The Hyperthrophy Of The Tibia Induced By The Volley-Ball .*. The Internet Journal of Bioengineering. 2008 Volume 4 Number 1.

###### Abstract

In this work we studied the internal remodeling of the tibia, induced by the volleyball. It is shown that after a long time, the tibia of the athlete will be stren-gthened, that is it will be more stiff and less porous. The result is theoretical, based on a proposed theory of internal bone remodeling (Hegedus and Cowin, 1976) and comes in accordance with several clinical findings (Fehling et., al.,1995; Calbet et., al., 1999; Rittweger et., al.,2000; Ito et., al.,2001).In their studies, as the bone mineral den-sity (BMD) as the muscle strength indices (MBSI) of the tibia of the volleyball pla-yers were evaluated and they were significant higher, than the corresponding clini-cal findings of the normally active control subjects.

### Introduction

Living bone is continually undergoing process of growth, reinforcement and resorption, termed collectively “remodeling”. Accordingly to Frost (1964) there are two kinds of bone remodeling: surface and internal. Many theories of internal bone remodeling have been suggested (Martin, 1972; Cowin and Hegedus 1976; Hegedus and Cowin, 1976; Cowin and Nachlinger, 1978; Cowin and Van -Buskirk,1 978; Carter et., al.,1987; Carter et., al., 1989).The purpose of this paper is to consider the internal remodeling of the tibia, induced by the volley-ball. For that reason, we will base upon the theory of Hegedus and Cowin (1976) which is known as “theory of adaptive elasticity”.

During a volley-ball game, it is possible to distinguish that the following hold:

i) The players are running in order to successfully rebut the ball, before it co-mes to contact with the ground.

ii) The volleyball spiker is vertically jumping as high as possible, in order to hit the ball. Also the players of the opposite team, are simultaneously vertically jumping as high as possible, in order to rebut the hit of the volleyball spi-ker.

iii) Finally the player who serves the ball, is sometimes jumping as high as possible, but he (she) is not landing to his (her) initial location. This jump can be modeled as an oblique shoot in the plane Oxz (x, z are the horizontal and vertical axons respectively). Particularly the center of the mass of the player is launched from the origin, with a velocity u_{o.} An angle α is formed between the direction of the vector of velocity u_{o } and the horizontal axon, as it seems in Fig. 1. The maximums high h_{M } and the horizontal displacement S_{M} are gi-ven by respectively:

where g is the acceleration of the gravity.

The server is mainly interested to jump as high as possible than as long as possible, in order to succesfully send the ball towards the region of the op-posite team. Also it is forbidden the server to leave his (her) area during the service, because of the international rules of volleyball playing. The last means that his (her) horizontal displacement is always under restriction. Therefore it holds h_{M} >S_{M} from which we result to:

Since sinα >sin76º = 0.97 ≈1,the jump of the server can approximatelly be con- sidered as a vertical.Therefore during the volleyball game, the tibia of the ath- lete is under an axial impact load, due as to running as to vertical jumps.

### Biomechanical analysis of the volleyball

We assume that a person with healthy bones, that is with bones which are not under osteoporosis or osteopetrosis ( Hegedus and Cowin,1976) participates to a volley-ball game or training and he (she) continues to be exersized with the same way, for a long time period. Initially the athlete was not dealed with the volley-ball playing, but he (she) was following a normal lifestyle, by wal-king with a constant velocity v_{o}. Consequently his (her) tibia was in a steady state at which no remodeling occurred, subjected only to a constant compres-sive load G_{o}, due to the vertical component of ground reaction force, at late

stance phase during walking. Selecting the experimental data from Andriacchi et., al., (1977); Rohrle et., al., (1984), neglecting the weight of the foot because is small (Harless,1860) and using a linear regression analysis, it is possible to find:

The walking activity corresponds to a velocity v_{o}, whose magnitude lies be-tween 0.5m/sec and 2m/sec (Whalen et., al., 1988). Then because of eq. (2.1), it is possible to conclude that the magnitude of the initial load G_{o}, _{ lies bet-ween 1.01B.W. and 1.329B.W. In addition we suppose that initialy the tibia had a uniform reference volume fraction ξο, such that 0< ξο<1 and a uniform relative volume fraction eo= 0. }

At t = 0 the athlete starts his (her) volleyball activity. We assumed that the player is x times running and is also ψ times vertically jumping. Then the ti-bia is under an average load G_{z} such that:

where Gz _{i}, i = 1,2, ..., x and Gz_{j}, j = x +1, x+2, ..., ψ are respectively: the vertical component of ground reaction force at late stance, during the i time of running and the vertical component of ground reaction force at landing phase, during the j time of jumping. Taking the experimental data from Alexander and Jayes (1980); Bates et.,al., (1983), Cavagna (1964); Cavanagh and LaFortune (1980); Fu-kanaga et., al., (1980); Winter et., al., (1983) and using a linear regression analy-sis, it is possible to obtain:

where v_{i} is the running velocity for the i time of running and assumed to be constant. The running activity corresponds to a velocity v, whose magnitude is at least 2.5m/sec (Whalen et., al., 1988). Then because of (2.3), it is possible to obtain that the magnitude of the running load Gz_{i} , is _{ at least 1.7 B.W. Also it holds: 2B.W.< Gzj < 4B.W (Gross and Nelsson ,1987; Nigg ,1985; Valiant and Ca-vanagh , 1983). Therefore accordingly to the abovementioned and by the help of eq. (2.2) we conclude that Gz > Go.
}

A hollow circular cylinder, subjected only to an axial impact load

In this section we will study the dynamic problem of a hollow circular cy-

The stress equations:

where ρ is the density of the tibia.

Also the stress-strain relations for a transversely isotropic material are:

where:

In addition the boundary conditions are:

where B is the weight of the athlete in units of B.W. and assumed to be con-stant during the training period.

Accordingly to Cowin and Nachlinger (1978), our problem accepts a unique solution. Assume the followings:

where A(t), B(t) and C(t) are unknown functions. Then (3.2) becomes:

Substituting the assumed strain field into equations (3.4), it is possible to find:

Applying the boundary conditions, we find that A(t), B(t) and C(t) are given by:

The displacements, the strains and the stresses, can be calculated by replacing (3.12)-(3.13) into (3.9), (3.10) and (3.11) respectively. Finally when the obtained strains are employed, the remodeling rate equation (3.1) concludes to the form:

Since we don’t know the exact values of the material functions, we will use approximate forms of them, for small values of e. Accordingly to Hegedus and Cowin (1976); Cowin and Van-Buskirk (1978), the proper approximations are:

_{o}, c_{1}, c_{2}, α_{Τ, } α_{Α}, Λ_{1}, Λ_{2}, Μ_{1}, Μ_{2} are constant coefficients. Therefore equa-tion (3.14) after the above approximations, concludes to:

that is we deal with an equation of the form:

##### Figure 20

The mathematical analysis and the exploration of the solutions of (3.17) that satisfies the initial condition e(0) =0, are in my earlier work ( Tsili, 2000, pp. 237-238) and it will not be repeated here. Only the final results, that are in Tables 1., 2., 3. and have been taken from my paper (Tsili, 2000) are registered.

##### Figure 21

##### Figure 22

### Discussion – Results

Our model predicts the clinical results of several researchers who have e-valuated the bone mineral density (BMD) and the muscle bone strength indice (MBSI) of the tibia of the volley-ball players ( Fehling et., al.,1995; Calbet et., al., 1999; Rittweger et., al., 2000; Ito et., al., 2001). In their studies as the BMD as the MBSI of the tibia of the volleyball players (and generally of the athle-tes whose bones are subjected to high impact loads) are significant higher, than the corresponding findings of the normally active control subjects.

In addition, there are some clinical findings concerning the assessment of the BMD or the hole body of the volley-ball players (Alfredson et., al., 1997; Hara et., al., 2001; Nikander et., al., 2005; Nikander et., al., 2006; Nichols et., al., 2007). Accordingly to the abovementioned citations, the BMD of the hole bo-dy of the volleyball players (and generally of the athletes whose sports deal with high impact loads),are significant higher compared with the corresponding findings of the normally active control subjects.Therefore the acceptable solu-tions of our problem, are in table 4. Accordingly to the results of this table, after a long time, the tibia of the athlete will be strengthened, that is it will be less porous and more stiff.

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