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Definition

Consider the differential equation y = f ( x , y ) . An equilibrium solution    is any solution to the differential equation of the form y = c , where c is a constant.

To determine the equilibrium solutions to the differential equation y = f ( x , y ) , set the right-hand side equal to zero. An equilibrium solution of the differential equation is any function of the form y = k such that f ( x , k ) = 0 for all values of x in the domain of f .

An important characteristic of equilibrium solutions concerns whether or not they approach the line y = k as an asymptote for large values of x .

Definition

Consider the differential equation y = f ( x , y ) , and assume that all solutions to this differential equation are defined for x x 0 . Let y = k be an equilibrium solution to the differential equation.

  1. y = k is an asymptotically stable solution    to the differential equation if there exists ε > 0 such that for any value c ( k ε , k + ε ) the solution to the initial-value problem
    y = f ( x , y ) , y ( x 0 ) = c

    approaches k as x approaches infinity.
  2. y = k is an asymptotically unstable solution    to the differential equation if there exists ε > 0 such that for any value c ( k ε , k + ε ) the solution to the initial-value problem
    y = f ( x , y ) , y ( x 0 ) = c

    never approaches k as x approaches infinity.
  3. y = k is an asymptotically semi-stable solution    to the differential equation if it is neither asymptotically stable nor asymptotically unstable.

Now we return to the differential equation y = ( x 3 ) ( y 2 4 ) , with the initial condition y ( 0 ) = 0.5 . The direction field for this initial-value problem, along with the corresponding solution, is shown in [link] .

A direction field for the given differential equation. The arrows are horizontal and pointing to the right at y = -4, y = 4, and x = 6. The closer the arrows are to x = 6, the more horizontal the arrows become. The further away, the more vertical they are. The arrows point down for y > 4 and x < 4, -4 < y < 4 and x > 6, and y < -4 and x < 6. In all other areas, the arrows are pointing up. A solution is graphed that goes through (0, 0.5). It begins along y = -4 in quadrant three, increases from -4 to 4 between x = -1 and 1, and ends going along y = 4 in quadrant 1.
Direction field for the initial-value problem y = ( x 3 ) ( y 2 4 ) , y ( 0 ) = 0.5 .

The values of the solution to this initial-value problem stay between y = −2 and y = 2 , which are the equilibrium solutions to the differential equation. Furthermore, as x approaches infinity, y approaches 2 . The behavior of solutions is similar if the initial value is higher than 2 , for example, y ( 0 ) = 2.3 . In this case, the solutions decrease and approach y = 2 as x approaches infinity. Therefore y = 2 is an asymptotically stable solution to the differential equation.

What happens when the initial value is below y = −2 ? This scenario is illustrated in [link] , with the initial value y ( 0 ) = −3 .

A direction field for the given differential equation. The arrows are horizontal and pointing to the right at y = -4, y = 4, and x = 6. The closer the arrows are to x = 6, the more horizontal the arrows become. The further away, the more vertical they are. The arrows point down for y > 4 and x < 4, -4 < y < 4 and x > 6, and y < -4 and x < 6. In all other areas, the arrows are pointing up. A solution is graphed that goes along y = -4 in quadrant 3 and curves between x = -1 and x = 0 to go to negative infinity along the y axis.
Direction field for the initial-value problem y = ( x 3 ) ( y 2 4 ) , y ( 0 ) = −3 .

The solution decreases rapidly toward negative infinity as x approaches infinity. Furthermore, if the initial value is slightly higher than −2 , then the solution approaches 2 , which is the other equilibrium solution. Therefore in neither case does the solution approach y = −2 , so y = −2 is called an asymptotically unstable, or unstable, equilibrium solution.

Stability of an equilibrium solution

Create a direction field for the differential equation y = ( y 3 ) 2 ( y 2 + y 2 ) and identify any equilibrium solutions. Classify each of the equilibrium solutions as stable, unstable, or semi-stable.

The direction field is shown in [link] .

A graph of a direction field with arrows pointing to the right at y = -4, y = 2, and y = 6. For y < -4, the arrows point up. For -4 < y < 2, the arrows point down. For 2 < y <6, the arrows point up, becoming flatter and flatter as they approach y = 6. For y > 6, the arrows point up and become more and more vertical the further they get from y = 6.
Direction field for the differential equation y = ( y 3 ) 2 ( y 2 + y 2 ) .

The equilibrium solutions are y = −2 , y = 1 , and y = 3 . To classify each of the solutions, look at an arrow directly above or below each of these values. For example, at y = −2 the arrows directly below this solution point up, and the arrows directly above the solution point down. Therefore all initial conditions close to y = −2 approach y = −2 , and the solution is stable. For the solution y = 1 , all initial conditions above and below y = 1 are repelled (pushed away) from y = 1 , so this solution is unstable. The solution y = 3 is semi-stable, because for initial conditions slightly greater than 3 , the solution approaches infinity, and for initial conditions slightly less than 3 , the solution approaches y = 1 .

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Source:  OpenStax, Calculus volume 2. OpenStax CNX. Feb 05, 2016 Download for free at http://cnx.org/content/col11965/1.2
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