How Does the Gompertz Equation Model Tumor Growth?

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SUMMARY

The Gompertz equation, represented as dN/dt=-rN*ln(N/K), effectively models tumor growth, where N(t) denotes the tumor cell count and r, K are positive parameters. The discussion highlights the critical points of the function f(N)=-rN*ln(N/K) and explores asymptotic stability, indicating that stability can be assessed without solving the differential equation by analyzing the sign of dN/dt near N=0 and N=K. The solution for N(t) under the initial condition N(0)=N0 is derived, emphasizing the importance of maintaining the constant K throughout the calculations.

PREREQUISITES
  • Understanding of differential equations and their applications in biological modeling.
  • Familiarity with the Gompertz growth model and its parameters (r and K).
  • Knowledge of logarithmic functions and their properties.
  • Ability to analyze stability in dynamical systems.
NEXT STEPS
  • Study the derivation and implications of the Gompertz equation in biological contexts.
  • Learn about stability analysis techniques for differential equations.
  • Explore graphical representations of the Gompertz function and its critical points.
  • Investigate other mathematical models for tumor growth, such as the logistic growth model.
USEFUL FOR

Mathematicians, biologists, and researchers involved in cancer modeling, as well as students studying differential equations and their applications in biological systems.

Jamin2112
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Homework Statement



As long as N isn't too small, the growth of cancerous tumors can be modeled by the Gompertz equation,

dN/dt=-rN*ln(N/K),

where N(t) is proportional to the number of cells in the tumor, and r, K > 0 are parameters.

(a) Sketch the graph f(N)=-rn*ln(N/k) verses N, find the critical points, and determine whether each is asymptotically stable or unstable.

(b) For the initial condition N(0)=N0 (N0>0), solve the Gompertz equation for N(t). Does this agree with your results from (a) in the limit as t -->∞?

(c) Sketch N(t) vs. t for initial conditions (i) 0 < N0 < K, (ii) N0=K, and (iii) N0 > K.

Homework Equations





The Attempt at a Solution



(a)

Below is my sketch. I figured, since r,K,N>0 (can't have negative size of tumor), this is just a natural log function upside down and stretched out a little bit.

screen-capture-3.png


I'm not sure how to tell if it's asymptotically stable. I know that on the graph of N(t) versus t, it will start out with a positive slope; decrease in slope until the slope is zero at N(t)=K; then the slope will gradually become more negative.

(b)

dN/dt=-rN*ln(N/K)
==> dN / (N*ln(N/K) = -rdt
==> d/dN (ln(ln(N/K))) = -rdt
==> ln(ln(N/K) = -rt + C
==> ln(N/K) = e-rt+C = ©e-rt (©=ec. I'm going to merge my constant shizzle while I solve)
==>N/K = e©ert
==>N=N(t)= Ke©ert = ®e(-rt) (®=ke©)


... This is where I'm stuck. I've always been told that I can merge constants as I go along; but doing so in this problem screws everything up because I need K to stay with me!
 
Physics news on Phys.org
Check your derivation : ln(ln(N/K) ) doesn't make sense when N <K. It's better to handle the 3 cases separately.
 
Jamin2112 said:
Sketch the graph f(N)=-rn*ln(N/k) that should be f(N)=-rN*ln(N/k) verses N, find the critical points, and determine whether each is asymptotically stable or unstable.


I'm not sure how to tell if it's asymptotically stable. I know that on the graph of N(t) versus t, it will start out with a positive slope; decrease in slope until the slope is zero at N(t)=K; then the slope will gradually become more negative.

(b)

dN/dt=-rN*ln(N/K)
==> dN / (N*ln(N/K) = -rdt
==> d/dN (ln(ln(N/K))) = -rdt
==> ln(ln(N/K) = -rt + C
==> ln(N/K) = e-rt+C = ©e-rt (©=ec. I'm going to merge my constant shizzle while I solve)
==>N/K = e©ert
==>N=N(t)= Ke©ert = ®e(-rt) (®=ke©)


... This is where I'm stuck. I've always been told that I can merge constants as I go along; but doing so in this problem screws everything up because I need K to stay with me!

Your question suggests to me having been copied to here not quite accurately. At any rate a natural reading of the first sentence above seems to be asking for critical points of f. There is one maximum of f but that is an inflection point of N against t. It doesn't come to me to think stability is something you characterise inflection points by.

Confusion between f and N has made your red sentence all wrong but I am sure you will get it right when you realize that.

For the asymptotic stability you do not need to solve the d.e., you just need to look at the sign of f, i.e. of dN/dt, near N=0, and near the top limit N=K (both sides of that one).

For your problem with the arbitrary constant it is a bit fiddly.

You got to ln(N/K) = Ce-rt (I agree with your integration) and you are probably thinking (N/K) = eCe-rt, ah that's N = KeCe-rt my K seems to have been swallowed into a lumped arbitrary constant. But it hasn't - eCe-rt is not eCe-rt but (eC)e-rt, not the same as multiplying K by eC, think about it.
 

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