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Solve the differential equations in Problems \(34-43 .\) Assume \(a, b,\) and \(k\) are nonzero constants. $$\frac{d y}{d t}=k y^{2}\left(1+t^{2}\right)$$

Short Answer

Expert verified
\( y = -\frac{1}{kt + \frac{kt^3}{3} + C} \)

Step by step solution

01

Separate Variables

The given differential equation is \( \frac{dy}{dt} = ky^2(1+t^2) \). To solve it, we begin by separating the variables. We will move all terms involving \( y \) to one side and all terms involving \( t \) to the other side. This gives us: \( \frac{1}{y^2} \, dy = k(1+t^2) \, dt \).
02

Integrate Both Sides

Next, we will integrate both sides of the equation. The left side with respect to \( y \) and the right side with respect to \( t \). The integral of \( \frac{1}{y^2} \) is \( -\frac{1}{y} + C_1 \), and the integral of \( k(1+t^2) \) is \( kt + \frac{kt^3}{3} + C_2 \). Thus, we have: \( -\frac{1}{y} = kt + \frac{kt^3}{3} + C \), where \( C \) includes both integration constants \( C_1 \) and \( C_2 \).
03

Solve for y

To find the expression for \( y \), we solve \( -\frac{1}{y} = kt + \frac{kt^3}{3} + C \) for \( y \). Taking the reciprocal, we have \( y = -\frac{1}{kt + \frac{kt^3}{3} + C} \).
04

Simplify the Expression

Finally, we simplify the expression for \( y \), if possible. However, in its current form, \( y = -\frac{1}{kt + \frac{kt^3}{3} + C} \) is as simplified as it can be without specific values for \( k \) and \( C \).

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Key Concepts

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

Separation of Variables
Separation of Variables is a method used to solve differential equations. It is a powerful technique because it allows us to break down complex equations into simpler parts. This is essential for solving equations like \(\frac{dy}{dt} = ky^2(1+t^2)\).
The aim is to separate the variables, typically \(y\) and \(t\) in our case, to opposite sides of the equation. This conversion simplifies the integration process later on.
Here's the step-by-step breakdown:
  • Identify all terms involving \(y\) and \(t\).
  • Organize them so that all \(y\)-related terms are on one side, and all \(t\)-related terms are on the other side.
  • This allows us to separate the equation into the form \( \frac{1}{y^2} \, dy = k(1+t^2) \, dt \).
After achieving this form, each side can be integrated individually with respect to its own variable.
Integration
Integration is a fundamental concept in calculus. It's the process of finding the antiderivative or the "integral" of a function. This is crucial in solving the separated variable differential equation.
Once we have the separated form \( \frac{1}{y^2} \, dy = k(1+t^2) \, dt \), we integrate both sides:
  • The left side, \( \int \frac{1}{y^2} \, dy \), results in \( -\frac{1}{y} + C_1 \). This is because \( \frac{1}{y^2} \) integrates to \( -\frac{1}{y} \).

  • The right side, \( \int k(1+t^2) \, dt \), simplifies to \( kt + \frac{kt^3}{3} + C_2 \), as each term's integral is taken separately and combined.
After integration, the solution combines the constants from both sides into a single constant \( C \). These constants account for the indefinite nature of integration, as they can vary to satisfy different initial conditions.
Initial Conditions
Initial conditions are often provided in differential equations to find a specific solution to a problem. They help determine the integration constant \( C \) and refine the general solution obtained through integration.
In our example, initial conditions would allow us to solve for \( C \) by substituting known values of \( y \) and \( t \). This step is crucial when a particular solution is desired rather than a family of solutions.
Without specific initial conditions, our solution remains in its general form:
  • \( y = -\frac{1}{kt + \frac{kt^3}{3} + C} \).
Thus, incorporating initial conditions gives more precision to our solution, making it applicable to real-world problems where initial data is usually known or measured. Initial conditions align the mathematical model with specific scenarios or experiments.

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Most popular questions from this chapter

Is the statement true or false? Assume that \(y=f(x)\) is a solution to the equation \(d y / d x=g(x) .\) If the statement is true, explain how you know. If the statement is false, give a counterexample. If \(\lim _{x \rightarrow \infty} g(x)=\infty,\) then \(\lim _{x \rightarrow \infty} f(x)=\infty.\)

Consider a conflict between two armies of \(x\) and \(y\) soldiers, respectively. During World War I, F. W. Lanchester assumed that if both armies are fighting a conventional battle within sight of one another, the rate at which soldiers in one army are put out of action (killed or wounded) is proportional to the amount of fire the other army can concentrate on them, which is in turn proportional to the number of soldiers in the opposing army. Thus Lanchester assumed that if there are no reinforcements and \(t\) represents time since the start of the battle, then \(x\) and \(y\) obey the differential equations $$\begin{array}{l} \frac{d x}{d t}=-a y \\ \frac{d y}{d t}=-b x \quad a, b>0 \end{array}$$. In this problem we adapt Lanchester's model for a conventional battle to the case in which one or both of the armies is a guerrilla force. We assume that the rate at which a guerrilla force is put out of action is proportional to the product of the strengths of the two armies. (a) Give a justification for the assumption that the rate at which a guerrilla force is put out of action is proportional to the product of the strengths of the two armies. (b) Write the differential equations which describe a conflict between a guerrilla army of strength \(x\) and a conventional army of strength \(y,\) assuming all the constants of proportionality are 1 (c) Find a differential equation involving \(d y / d x\) and solve it to find equations of phase trajectories. (d) Describe which side wins in terms of the constant of integration. What happens if the constant is zero? (e) Use your solution to part (d) to divide the phase plane into regions according to which side wins.

Give an example of: A differential equation for a quantity that is increasing and grows fastest when the quantity is small and grows more slowly as the quantity gets larger.

A rumor spreads among a group of 400 people. The number of people, \(N(t),\) who have heard the rumor by time \(t\) in hours since the rumor started is approximated by $$N(t)=\frac{400}{1+399 e^{-0.4 t}}$$ (a) Find \(N(0)\) and interpret it. (b) How many people will have heard the rumor after 2 hours? After 10 hours? (c) Graph \(N(t)\) (d) Approximately how long will it take until half the people have heard the rumor? 399 people? (e) When is the rumor spreading fastest?

Give the solution to the logistic differential equation with initial condition. $$\frac{d P}{d t}=0.8 P\left(1-\frac{P}{8500}\right) \text { with } P_{0}=500$$

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