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The following ordinary differential equation is called the Gompertz equation, which is used to model population growth:

dydt=ryln(yk)\frac{dy}{dt} = -r y \ln{\left(\frac{y}{k}\right)}

Here, rr and kk are constants known as the growth rate and the carrying capacity, respectively.

a) Use the method of separation of variables to solve the ordinary differential equation for an initial population y(0)=y0y(0) = y_0.

Hint: Integration by substitution may be required when solving this equation!

b) What is the limit of this solution as tt \to \infty?

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Question :

The following ordinary differential equation is called the gompertz equation, which is used to model population growth:

dydt=ryln(yk)\frac{dy}{dt} = -r y \ln{\left(\frac{y}{k}\right)}

here, rr and kk are constants known as the growth rate and the carrying capacity, respectively.

a) use the method of separation of variables to solve the ordinary differential equation for an initial population y(0)=y0y(0) = y_0.

hint: integration by substitution may be required when solving this equation!

b) what is the limit of this solution as tt \to \infty?

Solution:

Neetesh Kumar

Neetesh Kumar | April 13, 2025

Differential equation Homework Help

This is the solution to Initial Value Problem

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Step-by-Step-Solution:

Part a: Solving the Differential Equation

We are given the Gompertz equation:

dydt=ryln(yk)\frac{dy}{dt} = -r y \ln{\left(\frac{y}{k}\right)}

Step 1: Separate the variables

We need to separate yy and tt to use the method of separation of variables. Rearranging the equation:

dyyln(yk)=rdt\dfrac{dy}{y \ln{\left(\frac{y}{k}\right)}} = -r \, dt

Step 2: Perform the integration

Now, integrate both sides:

1yln(yk)dy=rdt\int \dfrac{1}{y \ln{\left(\frac{y}{k}\right)}} \, dy = \int -r \, dt

To integrate the left-hand side, use the substitution:

Let u=ln(yk)u = \ln{\left(\frac{y}{k}\right)}, then du=1ydydu = \frac{1}{y} \, dy. So the left-hand side becomes:

duu=lnu+C1\int \frac{du}{u} = \ln{|u|} + C_1

Substituting back for uu, we get:

lnln(yk)+C1\ln{\left|\ln{\left(\frac{y}{k}\right)}\right|} + C_1

For the right-hand side:

rdt=rt+C2\int -r \, dt = -rt + C_2

Thus, we have:

lnln(yk)=rt+C\ln{\left|\ln{\left(\frac{y}{k}\right)}\right|} = -rt + C

Where C=C2C1C = C_2 - C_1.

Step 3: Solve for yy

Exponentiate both sides to eliminate the logarithm:

ln(yk)=ert+C\left|\ln{\left(\frac{y}{k}\right)}\right| = e^{-rt + C}

Let eC=C3e^C = C_3, so:

ln(yk)=C3ert\ln{\left(\frac{y}{k}\right)} = C_3 e^{-rt}

Exponentiating both sides again:

yk=eC3ert\frac{y}{k} = e^{C_3 e^{-rt}}

Thus, the solution is:

y(t)=keC3erty(t) = k e^{C_3 e^{-rt}}

Step 4: Apply the initial condition y(0)=y0y(0) = y_0

We are given that at t=0t = 0, y=y0y = y_0. Substitute into the equation:

y0=keC3e0y_0 = k e^{C_3 e^{0}}

This simplifies to:

y0=keC3y_0 = k e^{C_3}

Thus, we find C3=ln(y0k)C_3 = \ln{\left(\frac{y_0}{k}\right)}. So the solution becomes:

y(t)=keln(y0kert)y(t) = k e^{\ln{\left(\frac{y_0}{k}e^{-rt}\right)} }

Finally, we have the solution:

y(t)=k(y0k).erty(t) = k \left(\frac{y_0}{k}\right).{e^{-rt}}


Part b: Finding the limit as tt \to \infty

To find the limit of the solution as tt \to \infty, consider:

limty(t)=limtk(y0k)ert\lim_{t \to \infty} y(t) = \lim_{t \to \infty} k \left(\frac{y_0}{k}\right){e^{-rt}}

As tt \to \infty, ert0e^{-rt} \to 0, so:

k.(y0k)=y0k.\left(\frac{y_0}{k}\right) = y_0

Therefore, the limit is:

limty(t)=y0\lim_{t \to \infty} y(t) = y_0

Thus, the population approaches the carrying capacity y0y_0 as tt \to \infty.


Final Answer:

  • The solution to the differential equation is:

y(t)=k(y0k).ert\boxed{y(t) = k \left(\frac{y_0}{k}\right).{e^{-rt}}}

  • The limit of this solution as tt \to \infty is:

limty(t)=y0\boxed{\lim_{t \to \infty} y(t) = \boxed{y_0}}



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