Active Calculus · 7: Differential Equations

7.2: Qualitative Behavior of Solutions to Differential Equations

Motivating Questions
  • What is a slope field?
  • How can we use a slope field to obtain qualitative information about the solutions of a differential equation?
  • What are stable and unstable equilibrium solutions of an autonomous differential equation?

In earlier work, we have used the tangent line to the graph of a function ff at a point aa to approximate the values of ff near a.a\text{.} The usefulness of this approximation is that we need to know very little about the function; armed with only the value f(a)f(a) and the derivative f′(a),f'(a)\text{,} we may find the equation of the tangent line and the approximation

f(x)≈f(a)+f′(a)(x−a). f(x) \approx f(a) + f'(a)(x-a)\text{.}

Remember that a first-order differential equation gives us information about the derivative of an unknown function. Since the derivative at a point tells us the slope of the tangent line at this point, a differential equation gives us crucial information about the tangent lines to the graph of a solution. We will use this information about the tangent lines to create a slope field for the differential equation, which enables us to sketch solutions to initial value problems. Our aim will be to understand the solutions qualitatively. That is, we would like to understand the basic nature of solutions, such as their long-range behavior, without precisely determining the value of a solution at a particular point.

Preview Activity 7.2.17.2.1

Let's consider the initial value problem

dydt=t−2,  y(0)=1. \frac{dy}{dt} = t - 2, \ \ y(0) = 1\text{.}

a. Use the differential equation to find the slope of the tangent line to the solution y(t)y(t) at t=0.t=0\text{.} Then use the initial value to find the equation of the tangent line at t=0.t=0\text{.} Sketch this tangent line over the interval −0.25≤t≤0.25-0.25 \leq t \leq 0.25 on the axes provided in Figure 7.2.17.2.1.

7_2_PA_tangents.svg

Figure 7.2.17.2.1. Grid for plotting partial tangent lines.

b. Also shown in Figure 7.2.17.2.1 are the tangent lines to the solution y(t)y(t) at the points t=1,2,t=1, 2\text{,} and 33 (we will see how to find these later). Use the graph to measure the slope of each tangent line and verify that each agrees with the value specified by the differential equation.

c. Using these tangent lines as a guide, sketch a graph of the solution y(t)y(t) over the interval 0≤t≤30\leq t\leq 3 so that the lines are tangent to the graph of y(t).y(t)\text{.}

d. Use the Fundamental Theorem of Calculus to find y(t),y(t)\text{,} the solution to this initial value problem.

e. Graph the solution you found in (d) on the axes provided, and compare it to the sketch you made using the tangent lines.

Slope fields

Preview Activity 7.2.17.2.1 shows that we can sketch the solution to an initial value problem if we know an appropriate collection of tangent lines. We can use the differential equation to find the slope of the tangent line at any point of interest, and hence plot such a collection.

Let's continue looking at the differential equation dydt=t−2.\frac{dy}{dt} = t-2\text{.} If t=0,t=0\text{,} this equation says that dy/dt=0−2=−2.dy/dt = 0-2=-2\text{.} Note that this value holds regardless of the value of y.y\text{.} We will therefore sketch tangent lines for several values of yy and t=0t=0 with a slope of −2,-2\text{,} as shown in Figure 7.2.27.2.2.

7_2_field_0.svg
Figure 7.2.27.2.2: Tangent lines at points with t=0.t=0\text{.}
7_2_field_1.svg
Figure 7.2.37.2.3: Adding tangent lines at points with t=1.t=1\text{.}

Let's continue in the same way: if t=1,t=1\text{,} the differential equation tells us that dy/dt=1−2=−1,dy/dt = 1-2=-1\text{,} and this holds regardless of the value of y.y\text{.} We now sketch tangent lines for several values of yy and t=1t=1 with a slope of −1-1 in Figure 7.2.37.2.3.

Similarly, we see that when t=2,t=2\text{,} dy/dt=0dy/dt = 0 and when t=3,t=3\text{,} dy/dt=1.dy/dt=1\text{.} We may therefore add to our growing collection of tangent line plots to achieve Figure 7.2.47.2.4.

7_2_field_3.svg
Figure 7.2.47.2.4: Adding tangent lines at points with t=2t=2 and t=3.t=3\text{.}
7_2_field_23.svg
Figure 7.2.57.2.5: A completed slope field.

In Figure 7.2.47.2.4, we begin to see the solutions to the differential equation emerge. For the sake of even greater clarity, we add more tangent lines to provide the more complete picture shown at right in Figure 7.2.57.2.5.

Figure 7.2.57.2.5 is called a slope field for the differential equation. It allows us to sketch solutions just as we did in the preview activity. We can begin with the initial value y(0)=1y(0) = 1 and start sketching the solution by following the tangent line. Whenever the solution passes through a point at which a tangent line is drawn, that line is tangent to the solution. This principle leads us to the sequence of images in Figure 7.2.67.2.6.

7_2_field_31.svg7_2_field_32.svg7_2_field_33.svg  

Figure 7.2.67.2.6. A sequence of images that show how to sketch the IVP solution that satisfies y(0)=1.y(0)=1\text{.}

In fact, we can draw solutions for any initial value. Figure 7.2.77.2.7 shows solutions for several different initial values for y(0).y(0)\text{.}

7_2_field_4.svg

Figure 7.2.77.2.7. Different solutions to dydt=t−2\frac{dy}{dt} = t-2 that correspond to different initial values.

Just as we did for the equation dydt=t−2,\frac{dy}{dt} = t-2\text{,} we can construct a slope field for any differential equation of interest. The slope field provides us with visual information about how we expect solutions to the differential equation to behave.

Activity 7.2.27.2.2

Consider the autonomous differential equation

dydt=−12(y−4). \frac{dy}{dt} = -\frac{1}{2}(y - 4)\text{.}
  1. Make a plot of dydt\frac{dy}{dt} versus yy on the axes provided in Figure 7.2.87.2.8. Looking at the graph, for what values of yy does yy increase and for what values of yy does yy decrease?
    7_2_Act1_1.svg
    Figure 7.2.87.2.8: Axes for plotting dydt\frac{dy}{dt} versus y.y\text{.}
    7_2_Act1_2.svg
    Figure 7.2.97.2.9: Axes for plotting the slope field for dydt=−12(y−4).\frac{dy}{dt} = -\frac 12( y - 4)\text{.}
  2. Next, sketch the slope field for this differential equation on the axes provided in Figure 7.2.97.2.9.
  3. Use your work in (b) to sketch (on the same axes in Figure 7.2.17.2.19.) solutions that satisfy y(0)=0,y(0) = 0\text{,} y(0)=2,y(0) = 2\text{,} y(0)=4y(0) = 4 and y(0)=6.y(0) = 6\text{.}
  4. Verify that y(t)=4+2e−t/2y(t) = 4 + 2e^{-t/2} is a solution to the given differential equation with the initial value y(0)=6.y(0) = 6\text{.} Compare its graph to the one you sketched in (c).
  5. What is special about the solution where y(0)=4?y(0) = 4\text{?}

Equilibrium solutions and stability

As our work in Activity 7.2.27.2.2 demonstrates, first-order autonomous equations may have solutions that are constant. These are simple to detect by inspecting the differential equation dy/dt=f(y):dy/dt = f(y)\text{:} constant solutions necessarily have a zero derivative, so dy/dt=0=f(y).dy/dt = 0 = f(y)\text{.}

For example, in Activity 7.2.27.2.2, we considered the equation dydt=f(y)=−12(y−4).\frac{dy}{dt} = f(y)=-\frac12(y-4)\text{.} Constant solutions are found by setting f(y)=−12(y−4)=0,f(y) = -\frac12(y-4) = 0\text{,} which we immediately see implies that y=4.y = 4\text{.}

Values of yy for which f(y)=0f(y) = 0 in an autonomous differential equation dydt=f(y)\frac{dy}{dt} = f(y) are called equilibrium solutions of the differential equation.

Activity 7.2.37.2.3

Consider the autonomous differential equation

dydt=−12y(y−4). \frac{dy}{dt} = -\frac{1}{2}y(y-4)\text{.}
  1. Make a plot of dydt\frac{dy}{dt} versus yy on the axes provided in Figure 7.2.107.2.10. Looking at the graph, for what values of yy does yy increase and for what values of yy does yy decrease?
    7_2_Act1_1.svg
    Figure 7.2.107.2.10: Axes for plotting dy/dtdy/dt vs yy for dydt=−12y(y−4).\frac{dy}{dt} = -\frac 12 y(y-4)\text{.}
    7_2_Act1_2.svg
    Figure 7.2.117.2.11: Axes for plotting the slope field for dydt=−12y(y−4).\frac{dy}{dt} = -\frac 12 y(y-4)\text{.}
  2. Identify any equilibrium solutions of the given differential equation.
  3. Now sketch the slope field for the given differential equation on the axes provided in Figure 7.2.117.2.11.
  4. Sketch the solutions to the given differential equation that correspond to initial values y(0)=−1,0,1,…,5.y(0)=-1, 0, 1, \ldots, 5\text{.}
  5. An equilibrium solution y‾\overline{y} is called stable if nearby solutions converge to y‾.\overline{y}\text{.} This means that if the initial condition varies slightly from y‾,\overline{y}\text{,} then lim⁡t→∞y(t)=y‾.\lim_{t\to\infty}y(t) = \overline{y}\text{.} Conversely, an equilibrium solution y‾\overline{y} is called unstable if nearby solutions are pushed away from y‾.\overline{y}\text{.} Using your work above, classify the equilibrium solutions you found in (b) as either stable or unstable.
  6. Suppose that y(t)y(t) describes the population of a species of living organisms and that the initial value y(0)y(0) is positive. What can you say about the eventual fate of this population?
  7. Now consider a general autonomous differential equation of the form dy/dt=f(y).dy/dt = f(y)\text{.} Remember that an equilibrium solution y‾\overline{y} satisfies f(y‾)=0.f(\overline{y}) = 0\text{.} If we graph dy/dt=f(y)dy/dt = f(y) as a function of y,y\text{,} for which of the differential equations represented in Figure 7.2.127.2.12 and Figure 7.2.137.2.13 is y‾\overline{y} a stable equilibrium and for which is y‾\overline{y} unstable? Why?
7_2_Act2_3.svg
Figure 7.2.127.2.12: Plot of dydt\frac{dy}{dt} as a function of y.y\text{.}
7_2_Act2_4.svg
Figure 7.2.137.2.13: Plot of dydt\frac{dy}{dt} as a different function of y.y\text{.}

Summary

  • A slope field is a plot created by graphing the tangent lines of many different solutions to a differential equation.
  • Once we have a slope field, we may sketch the graph of solutions by drawing a curve that is always tangent to the lines in the slope field.
  • Autonomous differential equations sometimes have constant solutions that we call equilibrium solutions. These may be classified as stable or unstable, depending on the behavior of nearby solutions.

Credit and licence

This page titled 7.2: Qualitative Behavior of Solutions to Differential Equations was last modified on Fri, 29 Sep 2023 00:33:23 GMT and is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Matthew Boelkins, David Austin, and Steven Schlicker ( ScholarWorks @Grand Valley State University ) via source content that was edited to the style and standards of the LibreTexts platform.

Source: https://math.libretexts.org/Bookshelves/Calculus/Active_Calculus_(Boelkins_et_al.)/07%3A_Differential_Equations/7.02%3A_Qualitative_Behavior_of_Solutions_to_Differential_Equations

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