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Consider the initial value problem $$ y^{\prime}=\sqrt{1-y^{2}}, \quad y(0)=0 . $$ (a) Show that \(y=\sin t\) is an explicit solution on the \(t\)-interval \(-\pi / 2 \leq t \leq \pi / 2\). (b) Show that \(y=\sin t\) is not a solution on either of the intervals \(-3 \pi / 2t^{*}\) ? (d) Show that the solution of the initial value problem is given by $$ y=\left\\{\begin{array}{lrl} -1, & -\infty &

Short Answer

Expert verified
No, y=sin(t) is not a solution on the interval -3π/2 < t < -π/2, because the derivative y'=cos(t) is negative in this interval while the equation y'=√(1-y²) gives a non-negative value.

Step by step solution

01

(a) Verify the explicit solution on interval -π/2 ≤ t ≤ π/2.

To show that y=sin(t) is an explicit solution of the differential equation y'=√(1-y²), we need to differentiate sin(t) with respect to t and see whether the given equation is satisfied in the interval -π/2 ≤ t ≤ π/2. Let's do that: $$ y' = \frac{d}{dt} \sin{t} = \cos{t} $$ Now we get y'=cos(t). Next, we need to substitute y=sin(t) into the given equation and see if both sides are equal: $$ y' = \sqrt{1-y^2} \Rightarrow \cos{t} = \sqrt{1-\sin^2{t}} $$ Since we already know that cos²(t) + sin²(t) = 1, we can see that both cos(t) and √(1-sin²(t)) are the same, and therefore the given solution is an explicit solution on the interval -π/2 ≤ t ≤ π/2.
02

(b) Verify the explicit solution on the intervals -3π/2 < t < -π/2 and π/2 < t < 3π/2.

Since we already established that y=sin(t) and y'=cos(t) in part (a), we just need to check whether the given equation y'=√(1-y²) is satisfied on the intervals -3π/2 < t < -π/2 and π/2 < t < 3π/2. However, we know that in these two intervals, cos(t) is negative. Meanwhile, the right side of the given equation, √(1-y²), is non-negative. Therefore, y'=cos(t) cannot be equal to √(1-y²) on these intervals. Thus, y=sin(t) is not a solution on the intervals -3π/2 < t < -π/2 and π/2 < t < 3π/2.
03

(c) Find the equilibrium solutions and analyze the graph of the function at equilibrium points.

We need to find values of y when the function y'=√(1-y²) becomes zero. The function will be zero when the quantity under the square root (1-y²) is zero. Therefore, $$ 1 - y^2 = 0 \Rightarrow y^2 = 1 \Rightarrow y = \pm 1 $$ Thus, the equilibrium solutions are y=1 and y=-1. Suppose, the solution y(t) reaches an equilibrium value at t=t*. Then, for t>t*, the graph of y(t) will be a horizontal line at y=1 or y=-1, because the derivative (i.e., the rate of change) will be zero at the equilibrium points.
04

(d) Show the given piecewise function as the solution to the initial value problem.

We are given the following piecewise function as the solution to the initial value problem: $$ y=\left\{\begin{array}{lrl} -1, & -\infty & <t<-\pi / 2 \\ \sin t, & -\pi / 2 & \leq t \leq \pi / 2 \\ 1, & \pi / 2 & <t<\infty . \end{array}\right. $$ We have already established that y=sin(t) is a solution for the interval -π/2 ≤ t ≤ π/2 in part (a). We know that the function has equilibrium solutions at y=1 and y=-1 and that the graph is a horizontal line at these values when the derivative is zero. In part (b), we have already shown that y=sin(t) is not a solution in the other intervals, i.e., -∞ < t<-π/2 and π/2 < t < ∞. Since y=-1 and y=1 are the equilibrium solutions and lie in those intervals, we now have a complete piecewise solution for the initial value problem: $$ y=\left\{\begin{array}{lrl} -1, & -\infty & <t<-\pi / 2 \\ \sin t, & -\pi / 2 & \leq t \leq \pi / 2 \\ 1, & \pi / 2 & <t<\infty . \end{array}\right. $$

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Key Concepts

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

Equilibrium Solutions
An equilibrium solution in the context of differential equations refers to a constant solution where the rate of change is zero. For the differential equation \( y' = \sqrt{1-y^2} \), equilibrium occurs when the derivative \( y' \) is equal to zero. This means:
  • \( \sqrt{1-y^2} = 0 \)
  • \( 1-y^2 = 0 \)
  • \( y^2 = 1 \)
  • \( y = \pm 1 \)
Thus, \( y = 1 \) and \( y = -1 \) are equilibrium solutions. When a function reaches these values, it stays there because further changes in \( y \) will result in no change in the derivative, indicating the graph of the function flattens out. At these equilibrium points, the function becomes a horizontal line, showing that these are stable states where the system does not change.
Piecewise Function
A piecewise function is a function that is defined by different expressions depending on the value of the independent variable. In our initial value problem, the solution to the differential equation is given by:\[y=\left\{\begin{array}{lll}-1, & -\infty < t < -\pi/2 \\sin t, & -\pi/2 \leq t \leq \pi/2 \1, & \pi/2 < t < \infty \\end{array}\right.\]This piecewise function combines three parts:
  • For \( t \) values less than \(-\pi/2\), \( y \) remains at the equilibrium solution \(-1\).
  • For \( t \) within \([-\pi/2, \pi/2]\), \( y \) follows a \( \sin t \) pattern, representing the dynamic part of the function.
  • For \( t \) greater than \( \pi/2 \), \( y \) is at the other equilibrium solution \(1\).
Piecewise functions are useful for modeling situations where a behavior changes at specific points or intervals, capturing transitions in simple terms.
Explicit Solution
An explicit solution to a differential equation expresses the dependent variable directly in terms of the independent variable. In the initial value problem \( y' = \sqrt{1-y^2} \), the explicit solution \( y = \sin t \) is verified over the interval \( -\pi/2 \leq t \leq \pi/2 \). This means you can clearly define \( y \) using cosine, as shown:- Differentiate \( y = \sin t \) to get \( y' = \cos t \).- Substitute \( y = \sin t \) into the equation, verifying that \( \cos t = \sqrt{1-\sin^2 t} \).This identity is proven using the Pythagorean identity \( \cos^2 t + \sin^2 t = 1 \). As a result, the solution satisfies the differential equation explicitly, showing a direct expression for \( y \) over the given interval, while explaining why it doesn't work beyond it, due to negative cosine values that do not satisfy the original equation.

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Most popular questions from this chapter

(a) Obtain an implicit solution and, if possible, an explicit solution of the initial value problem. (b) If you can find an explicit solution of the problem, determine the \(t\)-interval of existence. $$ t^{2} y^{\prime}+\sec y=0, \quad y(-1)=0 $$

Oscillating Flow Rate A tank initially contains \(10 \mathrm{lb}\) of solvent in \(200 \mathrm{gal}\) of water. At time \(t=0\), a pulsating or oscillating flow begins. To model this flow, we assume that the input and output flow rates are both equal to \(3+\sin t \mathrm{gal} / \mathrm{min}\). Thus, the flow rate oscillates between a maximum of \(4 \mathrm{gal} / \mathrm{min}\) and a \(\mathrm{minimum}\) of \(2 \mathrm{gal} / \mathrm{min}\); it repeats its pattern every \(2 \pi \approx 6.28 \mathrm{~min}\). Assume that the inflow concentration remains constant at \(0.5 \mathrm{lb}\) of solvent per gallon. (a) Does the amount of solution in the tank, \(V\), remain constant or not? Explain. (b) Let \(Q(t)\) denote the amount of solvent (in pounds) in the tank at time \(t\) (in minutes). Explain, on the basis of physical reasoning, whether you expect the amount of solvent in the tank to approach an equilibrium value or not. In other words, do you expect \(\lim _{t \rightarrow \infty} Q(t)\) to exist and, if so, what is this limit? (c) Formulate the initial value problem to be solved. (d) Solve the initial value problem. Determine \(\lim _{t \rightarrow \infty} Q(t)\) if it exists.

An object undergoes one-dimensional motion along the \(x\)-axis subject to the given decelerating forces. At time \(t=0\), the object's position is \(x=0\) and its velocity is \(v=v_{0}\). In each case, the decelerating force is a function of the object's position \(x(t)\) or its velocity \(v(t)\) or both. Transform the problem into one having distance \(x\) as the independent variable. Determine the position \(x_{f}\) at which the object comes to rest. (If the object does not come to rest, \(x_{f}=\infty\).) $$ m \frac{d v}{d t}=-k x v^{2} $$

Consider a population modeled by the initial value problem $$ \frac{d P}{d t}=(1-P) P+M, \quad P(0)=P_{0} $$ where the migration rate \(M\) is constant. [The model (8) is derived from equation (6) by setting the constants \(r\) and \(P_{*}\) to unity. We did this so that we can focus on the effect \(M\) has on the solutions.] For the given values of \(M\) and \(P(0)\), (a) Determine all the equilibrium populations (the nonnegative equilibrium solutions) of differential equation (8). As in Example 1, sketch a diagram showing those regions in the first quadrant of the \(t P\)-plane where the population is increasing \(\left[P^{\prime}(t)>0\right]\) and those regions where the population is decreasing \(\left[P^{\prime}(t)<0\right]\). (b) Describe the qualitative behavior of the solution as time increases. Use the information obtained in (a) as well as the insights provided by the figures in Exercises 11-13 (these figures provide specific but representative examples of the possibilities). $$ M=2, \quad P(0)=4 $$

An object undergoes one-dimensional motion along the \(x\)-axis subject to the given decelerating forces. At time \(t=0\), the object's position is \(x=0\) and its velocity is \(v=v_{0}\). In each case, the decelerating force is a function of the object's position \(x(t)\) or its velocity \(v(t)\) or both. Transform the problem into one having distance \(x\) as the independent variable. Determine the position \(x_{f}\) at which the object comes to rest. (If the object does not come to rest, \(x_{f}=\infty\).) $$ m \frac{d v}{d t}=-k e^{-x} $$

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