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Find the equilibrium solution of the following equations, make a sketch of the direction field, for \(t \geq 0,\) and determine whether the equilibrium solution is stable. The direction field needs to indicate only whether solutions are increasing or decreasing on either side of the equilibrium solution. $$y^{\prime}(t)=-6 y+12$$

Short Answer

Expert verified
Answer: The equilibrium solution is y = 2. It is stable as solutions on either side of the equilibrium solution approach y = 2; the solution is decreasing when y > 2 and increasing when y < 2.

Step by step solution

01

Find the equilibrium solution

To find the equilibrium solution(s), we set the first derivative of y(t), \(y^{\prime}(t)\) to zero and solve for y. $$0=-6y + 12$$ Solve for y: $$6y = 12$$ $$y = 2$$ The equilibrium solution is y = 2.
02

Analyze stability

To analyze the stability of the equilibrium solution, we can look at the expression for the derivative of y(t), namely: $$y^{\prime}(t) = -6y + 12$$ Let's consider the equilibrium solution y = 2: 1. If y > 2, then \(y^{\prime}(t) = -6y + 12 < 0\), which means the solution is decreasing. 2. If y < 2, then \(y^{\prime}(t) = -6y + 12 > 0\), which means the solution is increasing. Since solutions on either side of the equilibrium solution are approaching y = 2, this equilibrium solution is stable.
03

Sketch the direction field

We need to sketch the direction field by indicating whether solutions are increasing or decreasing on either side of the equilibrium solution. 1. If y > 2, the derivative is negative, which means the solution is decreasing. We can draw arrows pointing downwards in the region above y = 2. 2. If y < 2, the derivative is positive, which means the solution is increasing. We can draw arrows pointing upwards in the region below y = 2. 3. At the equilibrium solution y = 2, the derivative is 0, which indicates arrows pointing horizontally to the right. Remember, this direction field only needs to show the behavior of the solutions around the equilibrium solution. If you sketch the direction field as described, you will see that solutions in the region above the equilibrium solution decrease, while solutions in the region below the equilibrium solution increase. This confirms our previous analysis that the equilibrium solution y = 2 is stable.

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Most popular questions from this chapter

Consider the general first-order linear equation \(y^{\prime}(t)+a(t) y(t)=f(t) .\) This equation can be solved, in principle, by defining the integrating factor \(p(t)=\exp \left(\int a(t) d t\right) .\) Here is how the integrating factor works. Multiply both sides of the equation by \(p\) (which is always positive) and show that the left side becomes an exact derivative. Therefore, the equation becomes $$p(t)\left(y^{\prime}(t)+a(t) y(t)\right)=\frac{d}{d t}(p(t) y(t))=p(t) f(t).$$ Now integrate both sides of the equation with respect to t to obtain the solution. Use this method to solve the following initial value problems. Begin by computing the required integrating factor. $$y^{\prime}(t)+\frac{3}{t} y(t)=1-2 t, \quad y(2)=0$$

Solve the following initial value problems. When possible, give the solution as an explicit function of \(t\) $$y^{\prime}(t)=\frac{3 y(y+1)}{t}, y(1)=1$$

Write a logistic equation with the following parameter values. Then solve the initial value problem and graph the solution. Let \(r\) be the natural growth rate, \(K\) the carrying capacity, and \(P_{0}\) the initial population. $$r=0.4, K=5500, P_{0}=100$$

An object in free fall may be modeled by assuming that the only forces at work are the gravitational force and air resistance. By Newton's Second Law of Motion (mass \(\times\) acceleration \(=\) the sum of the external forces), the velocity of the object satisfies the differential equation $$\underbrace {m}_{\text {mass}}\quad \cdot \underbrace{v^{\prime}(t)}_{\text {acceleration }}=\underbrace {m g+f(v)}_{\text {external forces}}$$ where \(f\) is a function that models the air resistance (assuming the positive direction is downward). One common assumption (often used for motion in air) is that \(f(v)=-k v^{2},\) where \(k>0\) is a drag coefficient. a. Show that the equation can be written in the form \(v^{\prime}(t)=g-a v^{2},\) where \(a=k / m\) b. For what (positive) value of \(v\) is \(v^{\prime}(t)=0 ?\) (This equilibrium solution is called the terminal velocity.) c. Find the solution of this separable equation assuming \(v(0)=0\) and \(0 < v^{2} < g / a\) d. Graph the solution found in part (c) with \(g=9.8 \mathrm{m} / \mathrm{s}^{2}\) \(m=1,\) and \(k=0.1,\) and verify that the terminal velocity agrees with the value found in part (b).

Determine whether the following equations are separable. If so, solve the initial value problem. $$y^{\prime}(t)=e^{t y}, y(0)=1$$

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