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Solve the differential equations $$(t+1) \frac{d s}{d t}+2 s=3(t+1)+\frac{1}{(t+1)^{2}}, \quad t>-1$$

Short Answer

Expert verified
The general solution is \(s(t) = \frac{3}{4}(t+1)^2 + \frac{t}{(t+1)^2} + \frac{C}{(t+1)^2}\).

Step by step solution

01

Identify type of differential equation

The given differential equation is \[(t+1) \frac{d s}{d t} + 2s = 3(t+1) + \frac{1}{(t+1)^{2}}\]This is a first-order linear differential equation in the standard form \[a(t) \frac{ds}{dt} + b(t)s = c(t)\] where \[a(t) = t+1, \ b(t) = 2, \ c(t) = 3(t+1) + \frac{1}{(t+1)^2}\]We need to solve this equation by finding an integrating factor.
02

Compute the integrating factor

To find the integrating factor \(\mu(t)\), we use the formula:\[\mu(t) = e^{\int \frac{b(t)}{a(t)} dt}\] with \(b(t) = 2\) and \(a(t) = t+1\).Calculate the integral:\[\frac{b(t)}{a(t)} = \frac{2}{t+1}\]\[\int \frac{2}{t+1} dt = 2\ln|t+1| = \ln|(t+1)^2|\]\[\mu(t) = e^{\ln|(t+1)^2|} = (t+1)^2\]Thus, the integrating factor \(\mu(t) = (t+1)^2\).
03

Multiply the differential equation by the integrating factor

Multiply the entire differential equation by \((t+1)^2\) to facilitate integration.\[(t+1)^3 \frac{ds}{dt} + 2(t+1)^2s = 3(t+1)^3 + 1\]
04

Transform to exact equation and integrate

The transformed equation can be rewritten as:\[\frac{d}{dt}[(t+1)^2s] = 3(t+1)^3 + 1\]Integrate both sides with respect to \(t\):\[\int \frac{d}{dt}[(t+1)^2s] dt = \int (3(t+1)^3 + 1) dt\]On the left side, integration gives us:\[(t+1)^2s\]On the right side:\[\int 3(t+1)^3 dt + \int 1 dt = \left(\frac{3}{4}(t+1)^4\right) + t\]
05

Solve for s(t) and apply integration constant

Thus:\[(t+1)^2s = \frac{3}{4}(t+1)^4 + t + C\]Solve for \(s(t)\) by dividing both sides by \((t+1)^2\):\[s(t) = \frac{3}{4}(t+1)^2 + \frac{t}{(t+1)^2} + \frac{C}{(t+1)^2}\]
06

Solution verification

The general solution is given by:\[s(t) = \frac{3}{4}(t+1)^2 + \frac{t}{(t+1)^2} + \frac{C}{(t+1)^2}\]This satisfies the original differential equation for any constant \(C\).

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Key Concepts

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

First-Order Linear Differential Equation
A first-order linear differential equation is a type of equation that involves the first derivative of the unknown function. This is solved relatively easily compared to higher-order equations. These equations are expressed in the form:
  • \( a(t) \frac{ds}{dt} + b(t)s = c(t) \)
where \(a(t), b(t),\) and \(c(t)\) are functions of the independent variable \(t\). You also encounter a differential equation where the highest derivative is the first derivative, hence the name "first-order."
In our exercise, we identified this with \(a(t) = t+1, b(t) = 2, \) and \(c(t) = 3(t+1) + \frac{1}{(t+1)^2} \). Understanding the standard form helps in applying methods for solving, like using an integrating factor, which we'll explore next.
Integrating Factor
The integrating factor is a powerful tool in solving first-order linear differential equations. It transforms the equation into a form where integration becomes straightforward. You compute the integrating factor, denoted \(\mu(t)\), using:
  • \( \mu(t) = e^{\int \frac{b(t)}{a(t)} dt} \)
This formula is derived from multiplying the differential equation by \(\mu(t)\) to facilitate direct integration.
In the example provided, \(b(t) = 2\) and \(a(t) = t+1\). The process involved calculating the integral:
  • \( \int \frac{2}{t+1} dt = 2\ln|t+1| \)
is then exponentiated to yield the integrating factor:
  • \( \mu(t) = (t+1)^2 \)
Using the integrating factor to multiply through the differential equation enables us to reframe it for simple integration.
General Solution
Finding the general solution requires integrating the transformed differential equation and solving for the unknown function. After applying the integrating factor, the equation becomes an exact form:
  • \( \frac{d}{dt}[(t+1)^2s] = 3(t+1)^3 + 1 \)
With this equation, integration on both sides with respect to \(t\) gives us:
  • Left side: \( (t+1)^2s \)
  • Right side: \( \frac{3}{4}(t+1)^4 + t + C \)
where \(C\) is the constant of integration. Solving for \(s(t)\) gives the general solution:
  • \( s(t) = \frac{3}{4}(t+1)^2 + \frac{t}{(t+1)^2} + \frac{C}{(t+1)^2} \)
This represents a family of solutions where any value of \(C\) provides a valid solution to the differential equation. The beauty of the general solution is its ability to encompass an infinite number of particular solutions.

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Most popular questions from this chapter

Write an equivalent first-order differential equation and initial condition for \(y.\) $$y=1+\int_{0}^{x} y(t) d t$$

Solve the differential equations $$x y^{\prime}-y=2 x \ln x$$

Obtain a slope field, and graph the particular solution over the specified interval. Use your CAS DE solver to find the general solution of the differential equation. \(y^{\prime}=(\sin x)(\sin y), \quad y(0)=2 ; \quad-6 \leq x \leq 6, \quad-6 \leq y \leq 6\)

Use a CAS to explore graphically each of the differential equations. Perform the following steps to help with your explorations. a. Plot a slope field for the differential equation in the given \(x y\) -window. b. Find the general solution of the differential equation using your CAS DE solver. c. Graph the solutions for the values of the arbitrary constant \(C=-2,-1,0,1,2\) superimposed on your slope field plot. d. Find and graph the solution that satisfies the specified initial condition over the interval \([0, b]\) e. Find the Euler numerical approximation to the solution of the initial value problem with 4 subintervals of the \(x\) -interval, and plot the Euler approximation superimposed on the graph produced in part (d). f. Repeat part (e) for \(8,16,\) and 32 subintervals. Plot these three Euler approximations superimposed on the graph from part (e). g. Find the error ( \(y\) (exact) \(-y\) (Euler)) at the specified point \(x=b\) for each of your four Euler approximations. Discuss the improvement in the percentage error. $$\begin{aligned}&y^{\prime}=y(2-y), \quad y(0)=1 / 2 ; \quad 0 \leq x \leq 4,0 \leq y \leq 3\\\&b=3\end{aligned}$$

For the system ( \(2 a\) ) and ( 2 b), show that any trajectory starting on the unit circle \(x^{2}+y^{2}=1\) will traverse the unit circle in a periodic solution. First introduce polar coordinates and rewrite the system as \(d r / d t=r\left(1-r^{2}\right)\) and \(-d \theta / d t=-1\).

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