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Suppose the equation $$ M d x+N d y=0 $$ is homogeneous. (a) Show that Equation (A) is invariant under the transformation $$ x=k \zeta, \quad y=k \eta $$ where \(k\) is a constant. (b) Show that the general solution of Equation (A) can be written in the form $$ x=c \phi\left(\frac{y}{x}\right) $$ where \(c\) is an arbitrary constant. (c) Use the result of (b) to show that the solution (C) is also invariant under the transformation (B). (d) Interpret geometrically the results proved in (a) and (c).

Short Answer

Expert verified
In summary: (a) The given homogeneous differential equation is invariant under the transformation \(x=k \zeta, \quad y=k \eta\), meaning the equation holds for the transformed variables as well. (b) The general solution of the given homogeneous differential equation can be written in the form \(x = c \phi\left(\frac{y}{x}\right)\), where \(c\) is an arbitrary constant. (c) The solution of the homogeneous differential equation is also invariant under the transformation, preserving its structure and properties when scaled by a constant factor k. (d) Geometrically, the invariance under the transformation for both the equation and its solution shows self-similarity and scale-invariance within the family of solutions, maintaining their geometric features and properties when subjected to scaling by a constant factor k.

Step by step solution

01

a) Show the equation is invariant under the transformation

Given the equation \[M dx + N dy = 0,\] and the transformation \[x=k \zeta,\quad y=k \eta,\] we want to show that the equation remains invariant under this transformation. To show this, we differentiate both \(x\) and \(y\) with respect to \(\zeta,\) we get $$ \frac{dx}{d\zeta} = k, \qquad \frac{dy}{d\eta}=k $$ Now, we substitute these into the given equation, we get $$ M(k d\zeta) + N(k d\eta) = 0 $$ $$ k(M d\zeta + N d\eta) = 0 $$ Since \(k\) is a non-zero constant, the equation above holds if \(M d\zeta + N d\eta = 0\). Thus, the equation is invariant under the transformation.
02

b) Show the general solution can be written in the form

Now we want to show that the general solution of Equation (A) can be written in the form $$ x = c \phi\left(\frac{y}{x}\right) $$ To do this, we can use the substitution \(v = \frac{y}{x}\) or \(y= xv\). Now take the derivative of \(y\) with respect to \(x\), we get $$ \frac{dy}{dx} = x\frac{dv}{dx} + v $$ Substitute the above expression and \(y = xv\) into the given equation: $$ M dx + N(x\frac{dv}{dx} + v) dx = 0 $$ This can be simplified as, $$ M + N(x\frac{dv}{dx} + v) = 0 $$ Now, rearrange the equation to get a separated equation: $$ \frac{dv}{dx} = - \frac{M + Nv}{Nx} $$ Integrate both sides to obtain the general solution: $$ \int \frac{dv}{M + Nv} = - \int \frac{dx}{x} $$ Let \(\phi(v) = \int \frac{dv}{M + Nv}\). Integrating both sides we have: $$ \phi(v) = -\ln |x| + \ln|c| $$ Exponentiating both sides and solving for x we get $$ x = c \phi\left(\frac{y}{x}\right) $$ which proves the result.
03

c) Show that the solution is invariant under the transformation

Given the transformation: $$ x=k \zeta, \quad y=k \eta $$ and the general solution of Equation (A), which is: $$ x = c \phi\left(\frac{y}{x}\right) $$ We want to show that the solution is invariant under the transformation. Substituting the transformation into the general solution, we get $$ k \zeta = c \phi\left(\frac{k \eta}{k \zeta}\right) $$ Divide both sides by \(k\): $$ \zeta = \frac{c}{k} \phi\left(\frac{\eta}{\zeta}\right) $$ Now, we can see that the solution has the same form as the given general solution. Thus, the solution is invariant under the transformation.
04

d) Geometrical interpretation

The geometric interpretation of the results proved in (a) and (c) can be summarized as follows: 1. Invariance under the transformation in (a) signifies that any solution to the given homogeneous differential equation remains invariant under the transformation \(x=k\zeta, \quad y=k\eta\). In simpler terms, it means that the graph of the solution is scale-invariant. The family of solutions will continue to maintain its geometric feature and properties when scaled by a constant factor k. 2. Invariance under the transformation in (c) refers to the invariant properties of the general solution of the given homogeneous differential equation. This means that the transformation preserves the underlying structure of the solution space, showing the self-similarity nature of the family of solutions under the transformation.

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Key Concepts

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

Invariance Transformations
An invariance transformation is a mathematical operation that leaves certain properties of an equation unchanged. For homogeneous differential equations, such transformations help in understanding how solutions behave under scaling. Consider the equation \( M dx + N dy = 0 \), which remains invariant under the transformation \( x = k \zeta, y = k \eta \). Differentiating both sides, we find that the equation simplifies to \( k(M d\zeta + N d\eta) = 0 \). This shows that the original equation remains unchanged when variables are scaled, highlighting symmetry in its solutions.
General Solution of Differential Equations
Finding the general solution to a differential equation provides a functional form that satisfies the equation for all possible initial conditions. For the equation \( M dx + N dy = 0 \), the solution can be expressed as \( x = c \phi\left(\frac{y}{x}\right) \), where \( c \) is an arbitrary constant. This result is derived by substituting \( v = \frac{y}{x} \), turning the differential equation into a form that can be integrated. This integration involves splitting variables and results in a solution that is flexible enough to fit a broad range of scenarios, demonstrating the power of differential equations to model varying behaviors.
Geometric Interpretation in Differential Equations
The geometric interpretation of differential equations helps visualize their solutions. For homogeneous differential equations, solutions are scale-invariant, meaning their graphical representation maintains shape when scaled. Invariance under transformation, as shown in steps (a) and (c), implies that multiplying the variables by a constant \( k \) doesn't alter the solution's structure. This property reveals self-similarity among the solution curves, allowing us to understand how systems behave under different magnitudes while retaining geometric similarity, integral for fields like physics and engineering.
Scale-Invariant Solutions
Scale-invariant solutions imply that the form of a solution doesn't change when its parameters are multiplied by a constant factor. This feature is beneficial in many applications, such as modeling natural phenomena. The solution \( x = c \phi\left(\frac{y}{x}\right) \) remains unaffected by the transformation \( x=k \zeta, y=k \eta \), confirming its scale invariance. Essentially, if a problem can be solved at one scale, it can be extrapolated to others, making it a powerful tool for solving real-world problems where scaling is a natural consideration.

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Most popular questions from this chapter

Solve the initial-value problems. $$ \frac{d y}{d x}+3 x^{2} y=x^{2}, \quad y(0)=2. $$

(a) Show that the homogeneous equation $$ (A x+B y) d x+(C x+D y) d y=0 $$ is exact if and only if \(B=C\). (b) Show that the homogeneous equation $$ \left(A x^{2}+B x y+C y^{2}\right) d x+\left(D x^{2}+E x y+F y^{2}\right) d y=0 $$ is exact if and only if \(B=2 D\) and \(E=2 C\).

Solve the initial-value problems. (a) Let \(f_{1}\) be a solution of $$ \frac{d y}{d x}+P(x) y=Q_{1}(x) $$ and \(f_{2}\) be a solution of $$ \frac{d y}{d x}+P(x) y=Q_{2}(x) $$ where \(P, Q_{1}\), and \(Q_{2}\) are all defined on the same real interval \(I\). Prove that \(f_{1}+f_{2}\) is a solution of $$ \frac{d y}{d x}+P(x) y=Q_{1}(x)+Q_{2}(x) $$ on \(I\). (b) Use the result of (a) to solve the equation $$ \frac{d y}{d x}+y=2 \sin x+5 \sin 2 x $$

Solve the initial-value problems. Consider the Clairaut equation $$ y=p x+p^{2}, \quad \text { where } \quad p=\frac{d y}{d x} $$ (a) Find a one-parameter family of solutions of this equation. (b) Proceed as in the Remark of Exercise 20 and find an "extra" solution that is not a member of the one-parameter family found in part (a). (c) Graph the integral curves corresponding to several members of the one- parameter family of part (a); graph the integral curve corresponding to the "extra" solution of part (b); and describe the geometric relationship between the graphs of the members of the one-parameter family and the graph of the "extra" solution.

Solve each of the following by two methods (see Exercise \(21(a))\) : (a) \((x+2 y) d x+(2 x-y) d y=0\). (b) \((3 x-y) d x-(x+y) d y=0\)

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