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Ist durch Satz \(1.1\) gesichert, daB die DGln (a) \(y^{\prime}=\sin (x y)+x^{2} \mathrm{e}^{y} ;\) (b) \(y^{\prime}=\sqrt[3]{x y}\) genau eine Lösung durch den Punkt \((0,0)\) bzw. \((1,0)\) besitzen?

Short Answer

Expert verified
Exists and is unique for the first equation through (0,0), but not guaranteed uniquely for the second equation through (1,0).

Step by step solution

01

Identify the Initial Value Problem (IVP)

For each differential equation given, identify the initial point where the solution exists.(a) For the first equation, the initial point is \((0,0)\).(b) For the second equation, the initial point is \((1,0)\).
02

Apply the Existence and Uniqueness Theorem

The theorem states that if \(f(x, y)\) and \(\frac{\text{d} f}{\text{d} y}\) are continuous in a neighborhood of the initial point, then a unique solution exists.
03

Check for Continuity and Partial Derivative

(a) For \(y^{\prime} = \sin(xy) + x^{2} e^{y}\).- \(f(x, y) = \sin(xy) + x^{2} e^{y}\) is continuous in any region of \((x, y)\).- The partial derivative, \(\frac{\text{d} f}{\text{d} y} = x \cos(xy) + x^{2} e^{y}\), is also continuous everywhere.Therefore, due to continuity, there's exactly one solution through the point \((0,0)\).(b) For \(y^{\prime} = \sqrt[3]{xy}\).- \(f(x, y) = \sqrt[3]{xy}\) is continuous for all \((x, y)\).- The partial derivative, \(\frac{\text{d} f}{\text{d} y} = \frac{1}{3}x^{1/3}y^{-2/3}\), is not continuous at \((1,0)\) because of division by zero term \((y^{-2/3})\).Therefore, there's no guarantee of existence and uniqueness of the solution through the point \((1,0)\) due to lack of continuity.

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Key Concepts

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

Initial Value Problem (IVP)
An Initial Value Problem (IVP) is a differential equation accompanied by a specified value at a given point, called the initial condition. The goal is to find a function that satisfies the differential equation and meets the initial condition. For example:
(a) For the differential equation ewline ewline \( y' = \sin(xy) + x^2 e^y \), the initial condition is \( y(0) = 0 \). ewline ewline (b) For the differential equation ewline ewline \( y' = \sqrt[3]{xy} \), the initial condition is \( y(1) = 0 \). ewline ewline Whenever you have an IVP, you're trying to find a specific function that will solve the differential equation and pass through the initial condition point. Understanding the IVP clearly will guide you to use the appropriate methods.
Continuity in Differential Equations
Continuity is vital for solving differential equations, especially when applying the Existence and Uniqueness Theorem. If a function \( f(x, y) \) and its partial derivative with respect to \( y \) are both continuous in a neighborhood around the initial value point, then a unique solution exists. For our given problems:
- For ewline ewline \( y' = \sin(xy) + x^2 e^y \), \( f(x,y) = \sin(xy) + x^2 e^y \). This function is continuous because all terms (\(x y\) and the exponential function) are continuous everywhere.
- Its partial derivative is computed as ewline ewline \( \frac{\partial f}{\partial y} = x \cos(xy) + x^2 e^y \), which is also continuous in \( (x, y) \) space.
This confirms the exact solution for \( y' = \sin(xy) + x^2 e^y \) through the point \( (0,0) \).
However, for ewline ewline \( y' = \sqrt[3]{xy} \), \( f(x,y) = \sqrt[3]{xy} \) is continuous.
But its partial derivative, ewline ewline \( \frac{\partial f}{\partial y} = \frac{1}{3} x^{1/3} y^{-2/3} \), is not continuous at \( (1,0) \). Thus, there is no guarantee that a unique solution exists for the second equation at \( (1,0) \).
Partial Derivatives in Differential Equations
Partial derivatives play a crucial role in solving differential equations, especially in determining the existence and uniqueness of solutions. A partial derivative represents how a function changes as one of its variables changes, holding the other variables constant. To check for uniqueness:
- First, differentiate the given function \( f(x, y) \) concerning \( y \).
- This results in \( \frac{\partial f}{\partial y} \), which we need to check for continuity.
For ewline ewline \( y' = \sin(xy) + x^2 e^y \), we found ewline ewline \( \frac{\partial f}{\partial y} = x \cos(xy) + x^2 e^y \).
For ewline ewline \( y' = \sqrt[3]{xy} \), we determined ewline ewline \( \frac{\partial f}{\partial y} = \frac{1}{3} x^{1/3} y^{-2/3} \).
The continuity of the partial derivative indicates whether a unique solution exists: continuous partial derivatives (like in the first equation) mean there is a unique solution, while discontinuous ones (as in the second equation) do not guarantee a unique solution. This distinction is essential for thoroughly understanding differential equations.

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Most popular questions from this chapter

Gegeben sei ein (mathematisches) Pendel der Länge \(l\) und der Masse \(m\). (a) Gib ein mathematisches Modell für die Auslenkung \(\alpha=\alpha(t)\) als Funktion der Zeit \(t\) an. Hierbei ist \(\alpha\) der Winkel zwischen dem frei aufgehängten und dem ausgelenkten Pendel. (b) Wie vereinfacht sich dieses Modell für den Fall kleiner Auslenkungen ( *Linearisierung \(«\) )?

Unter einer Riccati- \(D G l^{16}\) versteht man eine DGl der Form $$ y^{\prime}+g(x) y+h(x) y^{2}=k(x) $$ mit stetigen Funktionen \(g, h, k\). (a) Zeige: Sind \(y_{1}\) und \(y_{2}\) Lösungen der Riccati-Dgl, so genügt die Differenz \(y:=y_{1}-y_{2}\) einer Bernoulli DGl. (b) Bestimme sämtliche Lösungen der DGl $$ y^{\prime}=\frac{y^{2}}{x^{3}}-\frac{y}{x}+2 x \quad(x>0) $$ Anleitung: \(y_{1}(x)=x^{2}\) ist eine Lösung der DGl.

Sei \(\varphi(t)\) die zu den Anfangsbedingungen \(\varphi(0)=0, \varphi^{\prime}(0)=\varphi_{1}>0\) gehörende Lösung der Pendelgleichung $$ m l \varphi^{\prime \prime}(t)=-m g \sin \varphi(t) $$ und \(E=\frac{m}{2} l^{2} \varphi_{1}^{2}\) die zugeh?rige (kinetische) Energie des Pendels zum Zeitpunkt \(t=0 . Z \mathrm{Zu}\) einem beliebigen Zeitpunkt \(t\) ergibt sich \(E\) als Summe aus kinetischer und potentieller Energie der Pendelmasse: $$ E=\frac{m}{2} l^{2}\left[\varphi^{\prime}(t)\right]^{2}+m g l[1-\cos \varphi(t)] $$ (s. Abschn. 1.3.3, Anwendung II). Beweise unter der Voraussetzung, daB die Gesamtenergie gröBer ist als die maximale potentielle Energie (d.h. \(E>2 m g l\) ): (a) Die Lösung \(\varphi(t)\) der Pendelgleichung existiert für alle \(t\) und ist eine ungerade Funktion. Ferner gilt \(\varphi^{\prime}(t)>0\) für alle \(t\) und \(\lim _{t \rightarrow \pm \infty} \varphi(t)=\pm \infty\) (b) Es gibt genau eine reelle Zahl \(\tau\) mit \(\varphi(\tau)=2 \pi\) (benutze (a)). Welchen Wert besitzt \(\varphi^{\prime}(\tau)\) ? (c) Für alle \(t\) gilt: \(\varphi(t+\tau)=\varphi(t)+2 \pi\). Anleitung: Zeige, daB sowohl \(\varphi_{0}(t):=\varphi(t+\tau)\) als auch \(\psi_{0}(t):=\varphi(t)+2 \pi\) der Pendelgleichung mit gemeinsamen Anfangsdaten genügt. (d) Die Bewegung $$ \left[\begin{array}{c} x(t) \\ y(t) \end{array}\right]=\left[\begin{array}{l} l \cos \varphi(t) \\ l \sin \varphi(t) \end{array}\right] $$ der Pendelmasse ist periodisch mit der Periode \(\tau\) (benutze (c)). Gib einen Integralausdruck für \(\tau\) an.

Bestimme die allgemeine Lösung der DGl \(3 y^{2} y^{\prime}-2 y^{3}=x+1\)

Von Volterra \(^{23}\) wurde das folgende Modell für eine Räuber-Beute- Population angegeben: $$ \left\\{\begin{array}{l} \dot{x}=-(a-b y) x \\ \dot{y}=(c-d x) y \end{array}\right. $$ Dabei ist \(x\) die Anzahl der R?uber- und \(y\) die Anzahl der Beutetiere. (a) Wie lautet die Phasen-DGl? (b) Bestimme mit Hilfe von (a) die Orbits.

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