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Generalized Mathematical Model for Biological Growths

Purnachandra Rao Koya, Ayele Taye Goshu*

School of Mathematical and Statistical Sciences, Hawassa University, Hawassa, Ethiopia Email: drkpraocecc@yahoo.co.in, *ayele_taye@yahoo.com

Received June 11,2013; revised July 15, 2013; accepted August 1, 2013

Copyright © 2013 Purnachandra Rao Koya, Ayele Taye Goshu. This is an open access article distributed under the Creative Com-mons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

ABSTRACT

In this paper, we present a generalization of the commonly used growth models. We introduce Koya-Goshu biological growth model, as a more general solution of the rate-state ordinary differential equation. It is shown that the commonly used growth models such as Brody, Von Bertalanffy, Richards, Weibull, Monomolecular, Mitscherlich, Gompertz, Lo-gistic, and generalized Logistic functions are its special cases. We have constructed growth and relative growth func-tions as solufunc-tions of the rate-state equation. The generalized growth function is the most flexible so that it can be useful in model selection problems. It is also capable of generating new useful models that have never been used so far. The function incorporates two parameters with one influencing growth pattern and the other influencing asymptotic behav-iors. The relationships among these growth models are studies in details and provided in a flow chart.

Keywords: Growth Model; Koya-Goshu Function; Gompertz, Logistic; Richards; Weibull

1. Introduction

Measuring biological growth has been important in many fields. Many researchers have contributed in developing relevant models: [1] for Brody function; [2] for Von Bertalanffy function; [3,4] for Richards function; [5] for Gompertz function; [6-8] for Logistic function; [6,9-11] for Generalized Logistic; [12,13] for Weibull function; [1,14] for Monomolecular function.

The mathematical representation of the relative growth is described by the ordinary differential equation (ODE) or rate-state equation

 

 

d

d t

f t

r f t

t  (1) Here f t

 

is representing growth function and t is

relative rate function at time . This ordinary differen-tial equation has many solutions among which some are studied in this paper. The growth models have been widely used in many biological growth problems includ-ing: in animal sciences [1,5,7,8,15,16] and in forestry [17,18]. Simulation studies by [19] indicates that such growth functions are so flexible to wrongly fit to given data set and recommends more care while selecting the models.

r

t

A number of attempts have been made to generalize

the growth models. For example, [17] modified the ODE (1) by including one parameter  as:

  

d d

y

k y

t

 

  from which some growth models

are derived. Moreover, they have shown that the model has upper limit but no inflection point when  1

1 ; and has both upper limit and inflection point for   .

[18] defined 9-parameters model as:

. The first two terms include all commonly known growth functions except Weibull, and so they included to the third term to account for it.

3 3 1 1 2 2

1 2 e 3

p q y

p q p q t

y K y tK yK y e

The generalized logistic function has been studied by some researchers [6,9-11]. Eberhardt and Breiwick [9] applied the models to growth of birds and mammals populations.

In the current paper, we provide a new single general-ized growth model as solution of the ODE (1) consisting of eight parameters. It can also serve for model selection purposes. We also study the mathematical relationships among the models presented herein. Inflection points of the models are discussed.

2. Koya-Goshu Growth Function as a

Generalization of Growth Functions

In this section we define a new generalized growth func-

(2)

tion, named as Koya-Goshu growth function and show how it accommodates the commonly known growth models such as: Logistic, Generalized Logistic, Gom- pertz, Brody, Monomolecular, Mitscherlich, Von Berta-lanffy, Richards, Generalized Weibull and Weibull func-tions.

The new generalized growth function, Koya-Goshu growth function, is defined as

 

1 e    m k t

L L

f tAAA  B     (2)

Here the parameters are defined as follows: 1

1

m L

L

A A

B

A A



 

  

  is derived from

A A A m, L, ,

 

: limt

A  f tf, A is upper asymptote of f t

 

L

A : Lower asymptote of f t

 

 

A  f

:

Growth rate parameter

 Time shift, a constant :

 Time scale, a constant , :m

 Shape parameters of the growth function, 0, 0

m  

2.1. Description of Koya-Goshu Growth Model

The Koya-Goshu growth model is 8-parameter

A A A k, L, , , , , ,   m

0.

function. The model is a more general solution of the ODE (1). Note that 0 and

equal at time

AA 

0

B  m 

Regarding the quantity ,

as ;

B 1

B 

B as ;

as . The quantity can assume any value in the open interval

0 B 

m 

0

m 

,1

B

1

B

0 B 1

for Richards, and in (0, 1) for both Von Bertalanffy and Brody. For both Logistic and Gompertz, can take any positive real number. For Weibull, while for generalized Weibull case,

.

When time is non-negative, the Koya-Goshu func-tion is well defined for modeling growths. The funcfunc-tion represents sigmoid curve for m < 0 and

t

 any positive odd integer. However, if m > 0 or (m < 0 and  is any real number other than positive odd integer), the function is well defined growth model for time ttL where

 

1 1

log

L

t

k B

  

    . This implies that the function misses lower asymptote in some cases. To account for the asymptote, modification can be made by taking

 

L

f tA for   t tL or can be written as:

 

 

1 e ,

,

m t k

L L L

L L

A A A B t t

f t

A t t

        

   

 

 

 

Thus, the Koya-Goshu function in (2) can be generally expressed as:

 

 

1 e    m

k t

L L L

f t A U t t A A B

   

 

      

 

(3) Here * is used to denote multiplication. Also here

0,

1,

L L

L

t t

U t t

t t

 

 

 is a unit step function, where

L

t   if m0 & odd positive integer or

 

1 1

log

L

t B

k

   

  

if

m0 or

m0 & non positive odd

L

t is a lower bound for the time. Note that ALf t

 

L

with f

 

 defined by the limit of f t

 

as time t

goes to . It serves as a lower asymptote of f t

 

.

Note that the Koya-Goshu function is defined at all points

m,

in m-plane. All the commonly known growth curves lay along the line 1 or m1 only. The function extends the inclusion of other points in the plane than these points. This means that it is so flexible that one can select any other curves than the commonly used ones.

We show that the Koya-Goshu model accommodates all commonly known growth functions. We have given detailed analysis of the growth models and how they are related to each other. The Richards function is a general form of Brody, Von Bertalanffy, Classical Logistic and Gompertz. Brody is same as Monomolecular and Mits- cherlich functions. Brody is a special case of Weibull function. All the relations are illustrated by flow chart in Figure 1. Detailed derivations of the function f t

 

and

relative growth rate t are given in Appendix A. Some selected plots are illustrated in Figures 2-5.

r

2.2. Properties of the Koya-Goshu Function

The function represents both increasing and decaying growths (see Figure 2(a), 3(a), 4(a), 5(a)). It is increas-ing for 0 and decaying for 0. This means that increasing or decaying of the growth is influenced by sign (positive or negative) of , irrespective of the val-ues of m.

The function represents increasing growths with upper asymptote but no lower asymptote:

1) For all positive combination values of both m and

 (see Figures 2(a), 3(a))

2) For all small negative values of and large posi-tive values of

m

 (see Figure 4(a)).

The function represents increasing growths with both upper and lower asymptotes:

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[image:3.595.61.540.74.520.2]

Figure 1. Flow chart illustrating the relationships among the generalized and specialized growth functions.

(a) (b)

[image:3.595.102.493.550.715.2]
(4)
[image:4.595.87.518.85.262.2]

(a) (b)

Figure 3. Plots of (a) growth functions and (b) rate functions with m2, 

2 1, ,2 .

(a) (b)

[image:4.595.91.509.296.656.2]

(c)

Figure 4. Plots of (a) growth functions and (b) (c) rate functions with m 1, 

2 1, ,2 .

positive values of  (see Figure 5(a))

2) For all small negative values of and small posi-tive values of

m

(see Figure 4(a)).

The occurrence of either lower and upper asymptotes

or only upper asymptotes is influenced by only but not

m

. Generally, the parameter  influences growth behavior, while the parameter influences asymptotic behavior of the function.

(5)

(a) (b)

[image:5.595.114.483.86.390.2]

(c) (d)

Figure 5. Plots of (a) (b) growth functions and (c) (d) rate functions with m 2, 

2 1, ,2 .

2.3. Inflection Point of Koya-Goshu Function

We now introduce the definition of inflection points of a curve, and describe the procedure to find inflection points for the growth functions we discuss in this paper. Suppose that the function f t

 

is continuous on an

open interval containing the point . Then the point is called an inflection point of

' 'a

' 'a f t

provided that

on one side of and on the

other side. At the inflexion point itself either or

 

0

 

0

f t

f t

' 'a

 

0 '

f t

'a

 

f t does not exist [20].

 

 

 

1 1

1 1

1

m L

m m

L L

mk

f t f t A

t

A A f t A

 

 

 

     

 

   

    

 

 

(4)

 

  

 

 

1

1 1

1

1 1

L

m L

L

A A

t

f t m m

f t A

t

k f t

 

 

 

 

   

 

 

 

 

  

    

    

  

 

  

 



 

   

     

  

(5)

Here, we observe that

 

  

 

1

1 0

1 1

1

1 0

1 1

1 0

1 e

m L

L

L

t k

f t

A A

m

f t A

t k

m t

m k

B

 

 

 

    

 

 

  

 

  

 

 

      

   

 

 

 

 

 

     

       

 

 

 

 

 



 

   

(6)

Clearly, point of inflection exists in Koya-Goshu func-tion provided the relafunc-tion (5) is satisfied, since

 

0

f t  at that point and also f

 

t 0 and

 

0

f t  are satisfied on the increasing and decreasing

sides of that point.

Here it can be observed that the inflection points of Koya-Goshu function, when the parameters are fixed as 1)

1, 1

(6)

For the other cases when m1,1, the inflection point for the Koya-Goshu function can be obtained by approximations. For example, using Taylor series expan-sion up to first order term, the time of inflection is ap-proximated as:

 

1 1 2 1 2 1 1

1 1 4 1 1

B t

m Bk

mB mB B m

                                (7)

3. Biological Growth Models and the

Parametric Relationships

In this section we studied the parametric relationships among all the biological growth models considered in this paper viz., Koya-Goshu biological growth model, Generalized Logistic, Particular case of Generalized Lo-gistic, Richards, Von Bertalanffy, Brody, LoLo-gistic, Gompertz, Generalized Weibull, Weibull Monomolecu-lar, and Mitscherlich functions. The relationships identi-fied have been exhibited through a flowchart.

3.1. Generalized Logistic Function

The Generalized Logistic function as given in [21] is expressed in its original notations as

 

  1

1 e t M

Y t

Q   

 

  

 

 which we now re-express

it with same notations used in this paper as

 

1 e   m

k t

L L

f tAAA  B    (8)

by replacing in the equation Y t

 

f t

 

,AL,

, ,

A k M

  

  1

m   and

 

1

– 1 L m

L A A Q A A           .

The Generalized Logistic function (7) is hereby a spe-cial case of Koya-Goshu function with  1, 1, and

. The parameter B takes the form 0

m

1

1 L m

L A A B A A       

  . The expression for the relative

growth rate function can be computed as

 

 

1 1 ( ) m L L t L

f t A

A A

r mk

f t A f t

                   

. Similarly, the

expressions for f

 

t and f

 

t are, respectively,

given by

 

 

1 1

1

 

1

m m m

L L

ftmk f tA  AA f tAL 

  

and

 

 

 

1

1

1 L m 1

L

A A

f t mk f t

m f t A

                         .

The single point of inflection occurs when the organism

reaches the growth

 

1 1

m

L L

f t A A A

m

 

  

  at

time

1

1

log 1 L m

L

A A

t m

k A A

                  

where m 

 

0,1 . For 0 , inflexion point does not exist.

1

m

 

3.2. Particular Case of the Generalized Logistic Function

A function called Particular case of the Generalized Lo-gistic function is defined [21] as

 

 0 1

1 e t t

Y t

Q   

 

which we now re-express it

with same notations used in this paper as

 

1 e   m

k t

f tAB    (9)

by replacing in the equation

 

 

0

1

, , , ,

Y t f t A k t

m

  

     

and

1 –Q 1 A m

A

 

   

  . Note that Equation (8) is a special

case of Equation (7) for Generalized Logistic function with AL0,mk  0 In this case, the parameter B

takes the form as

1

1 A m

B

A

 

   

  . The expression for the

relative growth rate function can be computed as rt

 

 

 

1 1 m L t

f t A

A

r mk

f t f t

                    

. Similarly, the ex-

pressions for f

 

t and f

 

t are respectively given

by

 

1 1

 

1 1

 

m m m

ftmkft Af t 

 

 

and

 

 

 

1

1

1 A m 1

f t mk f t

m f t

                      

(7)

point of inflection occurs when the organism reaches the

growth

 

1 1

m

f t A

m

 

  at time

1

1

log 1 ,

0,1

m

A

t m

k A

m

  

 

  

 

 

 

 

1

For 0m , inflexion point does not exist.

3.3. Richards Function

The Richards function is defined as in the usual notations (Richards, 1959) as

 

1 ekt m

f tAB  (10)

Here

1 0

1 A m

B

A

 

    . The Richards function can be directly derived from the ODE or rate-state Equation (1)

with relative rate function

 

1

1

m

t

A

r mk

f t

 

 

 

. The

Richards function becomes special case of Koya-Goshu growth model with  1, 1, 0,AL 0. Here the parameter m can assume any non-zero real number. The expressions for f

 

t and f

t

are given by respec-

tively

 

1 m

 

m m

 

1 1 1

ftmkftAf t

 

 

and

 

 

m1

  

1

m1

 

1

m

f tkft ft  mAm f t

 

 The

sin-gle point of inflection occurs when the growth reaches 1 m

m m

  

 

 of its final growth, i.e.

 

1

m

m f t

m

 

  A

at time

1 0

1 log 1 A m , 1.

t m m

k A

  

 

 

 

    

 

 

3.4. Von Bertalanffy Function

Von Bertalanffy is defined (Bertalanffy, 1957) as

 

3

1 ekt

f tAB  (11)

It is a special case of Richards function (5) with and a special case of Koya-Goshu growth model with

3

m

1, 1, 0,AL 0,m 3

       . Here

1 3 0

1 A

B

A

 

    . It can also be derived from ODE (1) with

relative rate function

 

1 3 3

t

A

r k

f t

 1

 

 

. For Von

Bertalanffy function f

 

t and f

 

t are respectively

given by

 

 

 

2 1 1

3 3 3

3

t kf tA f t

  

f

  and

 

3 2 13

 

13 13

 

2 13 3 13

 

f tk f t Af t    Af t 

   . Here

the single point of inflection occurs when the growth reaches

8 27

of its final growth, i.e.

  

t  8 27

A at time

1 3 0 1

log 3 1 A

t

k A

  

 

 

 

 

 

   

 

 

.

f

3.5. Brody Function

Brody is defined (Brody, 1945) as:

 

1 e kt

f tAB  (12)

It is a special case of Richards function (9) with 1

m and a special case of Koya-Goshu growth model

with. 1, 1, 0, 0, 1, 1 0

L

A

A m B

A

         . It can

also be derived from ODE (1) with rate function

 

1

t

A

r k

f t

 

 

 . Here f

 

t and f

 

t are respec-

tively given byf

 

tk Af t

 

and

 

2

 

f tkAf t. Brody growth function does not

possess a point of inflexion since f

 

t 0 is not sat-isfied for any value of . t

3.6. Logistic Function

The classical Logistic function (Nelder, 1961) is defined as:

 

A

1 e kt

f t

B

 (13)

Here

0

1

A B

A

 

 

. The Logistic function is a spe-

cial case of

1) Richards function (9) with m 1

2) Particular case of logistic function (8) with 0,m 1

  

3) Generalized logistic function (7) with 0,AL 0,m 1, k

     

4) Koya-Goshu function (2) with 1, 1, 0,AL 0,m 1

        .

(8)

 

t

A f t

r k

A

 

  

 . Here, f

 

t and f

 

t are

respec-tively given by f

 

t k f t

 

1 f t

A

 

 

  and

 

 

1 2f t

 

f t kf t

A

 

 

    . The single point of inflection

occurs when the growth reaches half of its final growth

 

2

A

f t  at time

0 1 log

   

  1

      A k A   t .

3.7. Gompertz Function

The Gompertz function (Winsor, 1932) is defined as

 

exp 

e B kt

f tA   (14)

where 0 log A B A     .

It is shown to be a special case of 1) Richards function (9) with 2) Particular case of logistic function (8) with 3) Generalized logistic function (7) with

m 

m 

0,AL 0,m

   ,  

0, L

4) Koya-Goshu function (2) with  1, 1, A 0,m . The

Gompertz function can be derived from the ODE (1) with

rate function

 

log t A r k f t      

. Here,

 

log

 

A

 

f t k f t

f t

 

  

 ,

 

 

log A

 

1

f t kf t

f t

   

    

   

   and the single point of

inflection occurs when the growth reaches

 

1 e of its final growth, i.e., f t

   

 1 e A at time

0 1

log log A t k A                  .

3.8. Generalized Weibull Function

The Weibull function is generalized and named here by Generalized Weibull function as

 

1 e

t K

f t A B

                

 (15)

where B 1 A

A

  . The generalized Weibull is a special

case of Koya-Goshu growth function (2) with . Generalized Weibull functions can be

derived from the ODE (1) with rate function

1, L 0

mA

 

1

1

t

k t A

r f t          

    . For Generalized Weibull,

 

ft and f

 

t are respectively given by

 

 

t

f t k A f t

                     

 

and

 

1

1 t 1 t

t k f t

              

f        

       . The

single point of inflection occurs when the organism

reaches the growth

 

1 1

1 e

f t A B

              at time 1 1 tk           .

3.9. Weibull Function

The Weibull growth model (Rawlings et al., 1998) is given as

 

1 e t f t       

  (16)

The Weibull function can be derived from the ODE (1)

with rate function

 

1

1 t

k t A

r f t               .

Weibull a special case of Generalized Weibull (13) func- tion with A1,B1,k1 and that of Koya-Goshu growth function (2) with

1, L 0, 1, 1, 1

mAABk . For Weibull, f

 

t and

 

f t are respectively given

byf

 

t 1 f t

 

t

              

    and

 

1 t 1

1

t

 

f t f

              t        

       . For

Weibull, the single point of inflection occurs when the

organism reaches the growth

 

1 1

1 e

f t

             at time 1 1

t    

 

 

   

  . This fact can be verified by

directly substituting A1,B1,k1 in the inflection point of Generalized Weibull.

3.10. Monomolecular and Mitscherlich Functions

(9)

Mitscher-lich growth functions are the same, except that the names and notations used are different. Hence, all these three functions exhibit the same properties and behaviors and also they represent the same growth patterns.

Monomolecular growth function is defined (France et al., 1996), in its original notations, as

 

0

0 e 1 1 e

t t

f f f

f

w

w t w w w w

w                    

where w t

 

is the growth function at time , t wf is the final (mature) value, 0 at is the initial value and

ww t0

 is rate of growth. This function can be expressed as Brody function (7) with notations

 

0

0 0

, f , , 1 w ,

w f t w A w A B k

w

     

asf t

 

A

1Bekt

. Monomolecular growth function can be derived from the ODE (1) with rate function

1

t f

r  w w or

 

1

t A r k f t        .

Thus, Monomolecular growth function, just similar to Brody growth function, does not possess a point of in-flexion since f

 

t 0 is not satisfied for any value of

. t

Mitscherlich growth function [22] is defined, in its original notations, as 1 e t

y     where is y

the growth function at time , t  is the final (mature) growth,  is a constant and  is rate of growth. The Mitscherlich function can be expressed with notations

 

, , , e k

yf t  A  k B  

as Brody function

1 e kt

f tAB  given by (7). It can be derived from

the ODE (1) with rate function

t y r y       

  or t

 

1

A r k f t        .

Not that the integral constant becomes

 

log AB  log . Thus, Mitscherlich growth function, just similar to Brody growth function, does not possess a point of inflexion since f

 

t 0 is not sat-isfied for any value of . t

4. Other Relationships

Here we derive explicitly and present few more relation-ships, other than those mentioned in Section 3, among the growth models considered in this paper.

4.1. Relation between Richards and Logistic Functions

Let us now see how Richards and Logistic functions are related. Using the Richards function (9), we can derive Logistic (12) as follows:

 

1 0

Richards 1 e

1 1 e

m kt

m m

kt

f t A B

A A A                                     (17)

 

1 1 0 1 0 0

Richards with 1

1 1 e

1 1 e

1 e

1 1 e

kt

kt

kt kt

f t m

A A A A A A A A B A A                                                 (18) where 1 0

1 A m

B

A

 

    . Hence, Richards growth function with

m 1

leads to the Logistic function.

4.2. Relation between Richards and Gompertz Functions

We now show how Gompertz is related to Richards function, i.e., the relative growth rate function of Rich-ards as leads to that of Gompertz, which is now shown. Note that the relative growth rate functions of Gompertz and Richards are given respectively by

m 

 

log t A r k f t    

  and

 

1 1 m t A r mk f t              .

By applying the limit as on Richards , we get the following:

m  rt

 

 

1 lim Richards lim 1 1

exp log 1

lim 1 m t m m m r A mk f t A

m f t

k m                                                  (19)

Here the last expression is obtained by a simple alge-braic rearrangement of the expression. In this expression

evaluation of limit leads to 0 0

   

(10)

applying L-Hospital rule to get

 

 

 

 

 

2 2 lim Richards 1 1

exp log log

lim

1

1

lim exp log log

log Gompertz m t m m t r A A

m f t m f t

k

m

A A

k

m f t f t

A k r f t                                                    (20) Thus, the limiting value of the Richards relative rate growth function as reduces to the Gompertz relative rate growth function, and hence these two func-tions are related.

m 

4.3. Relation between Particular Case of Generalized Logistic and Gompertz

We now show how Gompertz is related to the particular case of generalized Logistic function, i.e., the relative growth rate function of the particular case of generalized Logistic as leads to that of Gompertz, which is now shown. Note that the relative growth rate func-tions of Gompertz and the particular case of generalized

m 

Logistic are given respectively by

 

log t A r k f t      , and

 

1

1 where 0 m

t

A

r mk m

f t            .

By applying the limit as on rt of the

par-ticular case of generalized Logistic function, we get the following:

m 

 

 

1 lim lim 1 1

exp log 1

lim 1 m t m m m

r par case gen Log

A mk

f t

A

m f t

k m                                                          (21)

Here the last expression is obtained by a simple alge-braic rearrangement after the inverse functions viz, loga-rithmic and exponential operations are used. In this ex-

pression evaluation of limit leads to 0 0

   

  and to avoid

that we apply L-Hospital rule to get

 

 

 

 

 

2 2 lim 1 1

exp log log

lim

1

1

lim exp log log

log Gompertz

m t

m

m

t

r par case gen Log

A A

m f t m f t

k

m

A A

k

m f t f t

A k r f t                                                   (22) Thus, the relative rate growth function the particular case of generalized logistic function as re-duces to the Gompertz relative rate growth function, and hence these two functions are related.

m 

4.4. Relation between Brody and Gompertz Functions

We have shown in the flow chart the relationships among the growth functions by setting the parameters suitably. However, Gompertz and Brody functions can be related through a transformation of time coordinate and that goes as follows:

Let the time variables of Brody and Gompertz are rep-resented by and t  respectively. Now consider the Brody function as

 

1 e kt 1 1 A0 e kt

f t A B A

A

     

 

 

 

  (23)

and the Gompertz function as

 

0 0 0 0 exp exp

exp log exp

exp log exp

exp exp exp exp

f A B k

A A A k

A A A k

A A A k

A k                         (24)

Now on equating the f t

 

and f

 

 from (23)

and (24), we get

0

0

1 1 A e kt exp exp

A A

A k

   

   

   (25)

and this can be expressed as

0

0 1 log exp exp A A t

k A A k

          

(11)

[image:11.595.83.529.111.737.2]

Table 1. List of

growth functions and thei

r r

es

p

ective

rat

e fu

n

ction

s,

exp

res

si

on

s for b

,

in

teg

ral

con

stan

ts

and

in

flect

ion

p

o

(12)

which is the coordinate transformation equation between the time variables of Brody and Gompertz functions.

5. Illustration for How Relative Growth Rate

Function Behaves—Richards Case

The relative growth rate function t is significantly

dif-ferent for the models at early ages and converges to zero for the later ages. The relative growth rate t is an

in-creasing function of while it is a decreasing with time t. However, t grows with in the early ages

allowing the parameter m to play a significant role. Sub-sequently, t dies at later ages irrespective of . We

consider Richards function as example to illustrate this. r

m

r m

r

r m

Consider the Richards relative growth rate function :

t

r

 

1

1 m

t

A

r mk

f t

 

 

 

 

 

 

  (27)

is a function of parameter and time , and limit gives:

m z

 

1 1

0 0

0

limt rt mklimt A m 1 mk A m 1

f t A

 

  

 

   

 

 

 

 

 

 

(28) Equation (28) t is increases with m at early times. Also, on taking the limit of in (27) as t , we get

r

t

r  

 

1

limt rt mklimt A m 1 0

f t

 

 

 

 

 

 

 

 

showing that vanishes at time of growth maturity for

all . t

r m

6. Conclusion

This paper introduces a new generalized mathematical model for biological and other growths, named as Koya- Goshu growth model. It is a generalization of the com- monly used growth functions such as: Brody, Von Ber- talanffy, Richards, Weibull, Monomolecular, Mitscher- lich, Gompertz, Logistic and generalized Logistic func- tions. Koya-Goshu model is constructed as a solution of ordinary differential or rate-state equation. The function incorporates two parameters where one influences grow- th pattern and the other influences asymptotic behavior. The model is so flexible that it can be useful in model selections. Moreover, it generates new and useful growth functions. All of the growth models considered under the study are related to each other as illustrated in the flaw

chart. As further studies, we will take up applications of this model for data fitting and prediction.

REFERENCES

[1] S. Brody, “Bioenergetics and Growth,” Reinhold Pub- lishing Corporation, New York, 1945.

[2] L. von Bertalanffy, “Quantitative Laws in Metabolism and Growth,” The Quarterly Review of Biology, Vol. 3,

No. 2, 1957, p. 218.

[3] F. J. Richards, “A Flexible Growth Function for Empiri- cal Use,” Journal of Experimental Botany, Vol. 10, 1959,

pp. 290-300.http://dx.doi.org/10.1093/jxb/10.2.290 [4] J. France and J. H. M. Thornley, “Mathematical Models

in Agriculture,” Butterworths, London, 1984, p. 335. [5] C. P. Winsor, “The Gompertz Curve as a Growth Curve,”

Proceedings of National Academy of Science, Vol. 18, No.

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Figure

Figure 2. Plots of (a) growth functions and (b) rate functions with m 1, 2 1, ,2
Figure 4. Plots of (a) growth functions and (b) (c) rate functions with m  1, 2 1, ,2
Figure 5. Plots of (a) (b) growth functions and (c) (d) rate functions with m  2, 2 1, ,2
Table 1. List of growth functions and their respective rate functions, expressions for b, integral constants and inflection points

References

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