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Solve the Logistic equation, \(d y / d t=\alpha y(1-\) \((1 / K) y\) ), by viewing it as a Bernoulli equation and then solve the resulting linear equation by using an integrating factor rather than the method of undetermined coefficients that is illustrated in the examples.

Short Answer

Expert verified
By viewing it as a Bernoulli equation and using an integrating factor, the solution is \( y = \frac{Ke^{\alpha t}}{C + e^{\alpha t}} \).

Step by step solution

01

Identify the Bernoulli equation form

Recognize the given logistic equation \(\frac{dy}{dt} = \alpha y(1 - \frac{y}{K})\). Rewrite it in the form of a Bernoulli equation \(\frac{dy}{dt} + P(t)y = Q(t) y^n\) with \ n = 2 \.
02

Divide through by y

To transform the equation, divide through by y: \(\frac{1}{y} \frac{dy}{dt} = \alpha (1 - \frac{y}{K})\), simplifying to \( \frac{dy}{dt} + \-\frac{\alpha}{K} y = \alpha y \).
03

Set up the standard Bernoulli form

Rewrite to fit the Bernoulli form. In this case: \( \frac{dy}{dt} + \frac{\alpha}{K} y = \alpha \).
04

Use the substitution

Let \( v = y^{1 - 1} = y^0 \), simplifying \( \frac{dy}{dt} + \frac{\alpha}{K} y = \alpha y\) to a linear form.
05

Differentiate the substitution

Differentiate \( v = y^{0} \) with respect to \( t \) to get \(\frac{dv}{dt}\frac{dy}{dt} + \frac{\alpha}{K} \frac{dy}{dt} \).
06

Simplify the linear equation

The substitution transforms the equation into a linear one: \( \frac{dv}{dt} + \frac{\alpha}{K} v = \frac{\alpha}{K} \).
07

Find the integrating factor

Identify the integrating factor \( \mu(t) = e^{\frac{\alpha}{K}t} \).
08

Multiply through by the integrating factor

Multiply each term of the differential equation by \( \mu(t) \) to facilitate integration: \( e^{\frac{\alpha}{K}t} \frac{dv}{dt} + \frac{\alpha}{K} e^{\frac{\alpha}{K}t} v = \frac{\alpha}{K} e^{\frac{\alpha}{K} t} \).
09

Integrate both sides

Integrate the simplified equation with respect to \( t \: \frac{d}{dt} (e^{\frac{\alpha}{K} t} v = \frac{\alpha}{K} e^{\frac{\alpha}{K} t} \rightarrow e^{\frac{\alpha}{K} t} v = \alpha t + C\).
10

Solve for the original variable

Solve the resulting equation for \( v \) first, then substitute back to \( y \: y = \frac{Ke^{\alpha t}}{C + e^{\alpha t}}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Bernoulli Equation
The Bernoulli Equation is a special type of non-linear differential equation of the form \( \frac{dy}{dt} + P(t)y = Q(t)y^n \). It’s named after Jacob Bernoulli, a Swiss mathematician.

  • When solving a Bernoulli equation, the first step is often to identify how it can be manipulated into a standard linear form. This usually involves substitution and transformation.

  • For our Logistic Equation problem, the equation is rewritten to fit this form. Initially, we’re given \( \frac{dy}{dt} = \alpha y(1 - \frac{y}{K}) \). To match the Bernoulli form, we divide through to simplify and identify the parameters, which helps us proceed with solving the equation.

  • The critical step to transforming it is to use the substitution \( v = y^{1 - n} \), which results in a linear differential equation.

Understanding how to manipulate non-linear equations into a more manageable form is crucial. Substitution helps convert it into a linear differential equation, which is easier to solve using standard methods.
Integrating Factor
An integrating factor is used to solve linear differential equations.

  • The method involves multiplying through the differential equation by a specific function, called the integrating factor, denoted as \( \mu(t) \), which simplifies the equation such that it can be integrated directly.

Let's see how it applies:
In our example, after simplifying the Bernoulli equation to \( \frac{dv}{dt} + \frac{\alpha}{K} v = \frac{\alpha}{K} \), we identify an integrating factor as \( \mu(t) = e^{\frac{\alpha}{K} t} \).
  • This integrating factor transforms our differential equation into a form that's directly integrable.

  • Essentially, it helps to accumulate the effects of the changing variable. Multiplying both sides by this factor aligns the differential equation to a product rule form, making integration straightforward.

This leads to solving \( \frac{d}{dt} (e^{\frac{\alpha}{K} t} v) = \frac{\alpha}{K} e^{\frac{\alpha}{K} t} \) by integrating both sides, thus easing the computation considerably.
Differential Equations Solving Methods
Solving differential equations involves various methods, including separation of variables, integrating factors, and substitutions.

  • Separation of Variables: This is one of the most basic methods where you rearrange the differential equation so that each variable appears on a different side of the equation. Then integrate both sides with respect to their respective variables.

  • Integrating Factor: As described, it's an effective method for solving linear first-order differential equations by multiplying the equation by a strategically chosen function.

  • Bernoulli Equation Transformation: For non-linear equations in the Bernoulli form, a substitution is used to transform them into a linear equation that can then be solved by other standard methods like integrating factors.

Each method has its specific use cases and becomes handy depending on the nature of the differential equation.

In our logistic equation example, the process combines recognizing the equation form, transforming using substitution, and then applying integrating factors to find the solution efficiently.

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Most popular questions from this chapter

Suppose that the rabbit population on a small island grows at a rate proportional to the number of rabbits present. If this population doubles after 100 days, when does the population triple?

In an electric circuit with one loop that contains a resistor \(R\), a capacitor \(C\), and a voltage source \(E(t)\), the charge \(Q\) on the capacitor is found by solving the initial value problem \(R d Q / d t+Q / C=E(t), Q(0)=Q_{0}\). Solve this problem to find \(Q(t)\) if \(E(t)=\) \(E_{0}\) where \(E_{0}\) is constant. Find \(I(t)=Q^{\prime}(t)\) where \(I(t)\) is the current at any time \(t\).

(a) Find the solution to the IVP \(d y / d t=\) \(-r(1-y / A) y, y(0)=y_{0}\), where \(r\) and \(A\) are positive constants. (b) If \(y_{0}A\), show that \(\lim _{t \rightarrow \infty} y(t)=\infty\). (d) Show that if \(y_{0}>A\), then \(y(t)\) has a vertical asymptote at \(t=\) \(\frac{1}{r} \ln \left(\frac{y_{0}}{y_{0}-A}\right)\).

A hot cup of tea is initially \(100^{\circ} \mathrm{C}\) when poured. How long does it take for the tea to reach a temperature of \(50^{\circ} \mathrm{C}\) if it is at \(80^{\circ} \mathrm{C}\) after \(15 \mathrm{~min}\) and the room temperature is \(30^{\circ} \mathrm{C}\) ?

(See Exercise 21) Compare the Earth's escape velocity to those of Venus and Mars if for Venus \(R \approx 3800\) miles and acceleration of gravity is \(85 \%\) of that of the Earth; and for Mars \(R \approx 2100\) miles and acceleration of gravity is \(38 \%\) of that of the Earth. Which planet has the largest escape velocity? Which has the smallest?

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