/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 4 \(2 x(1-x) y^{\prime \prime}+(3-... [FREE SOLUTION] | 91Ó°ÊÓ

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\(2 x(1-x) y^{\prime \prime}+(3-10 x) y^{\prime}-6 y=0\)

Short Answer

Expert verified
The general form of the solution for \(2x(1-x)y''+(3-10x)y'-6y = 0\) will be \(y = c_1 e^{m_1x} + c_2 e^{m_2x}\) after simplifying. But to find the exact solution, the roots \(m_1\) and \(m_2\) from the auxiliary equation needs to be found. Finding these requires a more complex solving process due to the presence of \(x\) terms in the equation.

Step by step solution

01

Convert the differential equation into its standard form

Divide the entire differential equation \(2x(1-x)y''+(3-10x)y'-6y = 0\) by \(2x(1-x)\) to get it into the standard form. This standard form will lead to: \[y''+ \frac{(3-10x)}{2x(1-x)}y' - \frac{3}{x(1-x)}y = 0\]
02

Identify the type of the differential equation

Observing the equation, we see it's in the form of \[y'' + p(x)y'+ q(x)y = 0\] which is a 2nd order linear homogeneous differential equation. Here, \(p(x) = \frac{(3-10x)}{2x(1-x)}\) and \(q(x) = -\frac{3}{x(1-x)}\)
03

Solve the Homogeneous Equation

To find the homogeneous solutions, we first need to solve the auxiliary equation related to the homogeneous differential equation. The characteristic equation is given by \(m^2 + pm + q = 0\). However, due to the presence of \(x\) terms in \(p(x)\) and \(q(x)\), the equation cannot be solved easily. Thus, further simplification or specific solving methods for such equations need to be implemented, which will require advanced mathematical knowledge.
04

General solution

The general solution of this equation will be the sum of two solutions obtained from the characteristic equation i.e., if the roots of the auxiliary equation (characteristic equation) are \(m_1\) and \(m_2\), then the general solution of the equation will be \(y = c_1 e^{m_1x} + c_2 e^{m_2x}\).

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Key Concepts

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

Standard Form of Differential Equations
Second order linear homogeneous differential equations have a standard form. This form makes it easier to analyze and solve the equations. The generic format is:
  • \( y'' + p(x)y' + q(x)y = 0 \)
In this standard form, \( y'' \) represents the second derivative of \( y \), \( y' \) is the first derivative, and \( y \) is the original function. The functions \( p(x) \) and \( q(x) \) are coefficients that might vary with \( x \).

In our example exercise, the equation \( 2x(1-x)y''+(3-10x)y'-6y = 0 \) was transformed into its standard form by dividing every term by \( 2x(1-x) \). This gave us \( y'' + \frac{(3-10x)}{2x(1-x)}y' - \frac{3}{x(1-x)}y = 0 \). Placing a differential equation in standard form lays the groundwork for further analysis, such as determining the characteristic equation.
Characteristic Equation
The characteristic equation is a crucial part of determining the general solution for linear homogeneous differential equations. It typically arises when you assume solutions in the form \( y = e^{mx} \). If you differentiate twice and substitute back into the standard form, you get what's known as the "characteristic equation."

For the general equation \( y'' + py' + qy = 0 \), the characteristic equation is:
  • \( m^2 + pm + q = 0 \)
This quadratic equation provides the roots which help us determine the form of the homogeneous solution. In some instances, like our initial equation, \( p(x) \) and \( q(x) \) might contain \( x \), complicating the situation and requiring more advanced methods for solutions.

Finding the characteristic equation is an essential step when the equation coefficients are constants, although for variable coefficients, other techniques might be necessary.
Homogeneous Solution
A homogeneous solution refers to a solution of the differential equation without any non-homogeneous parts (such as external forcing functions or non-zero terms on the right-hand side). To solve for this, we rely on the characteristic equation.

When deriving the general solution from the characteristic equation's roots, two main scenarios can unfold:
  • If the roots \( m_1 \) and \( m_2 \) are real and distinct, then the solution is \( y = c_1 e^{m_1x} + c_2 e^{m_2x} \).
  • If the roots are real and equal, the solution is adapted to \( y = (c_1 + c_2x)e^{m_1x} \).
  • For complex roots, special considerations come into play, usually involving sine and cosine functions.
The key takeaway is that the solution format fundamentally depends on the type of roots obtained from the characteristic equation. Without delving into specific solutions, understanding the homogeneous solution's format lays the foundational knowledge needed for solving these kinds of equations.
Complex Roots and Real Roots
When solving the characteristic equation, discovering whether the roots are real or complex significantly impacts the form of the solution.

Here's how these situations are managed:
  • Real Roots: If the roots from \( m^2 + pm + q = 0 \) are real and distinct, the solution to the differential equation is formed by linear combinations of exponential functions; \( y = c_1 e^{m_1x} + c_2 e^{m_2x} \).
  • Equal Roots: Should the roots be equal (such cases happen when the discriminant of the characteristic equation equals zero), the solution turns into \( y = (c_1 + c_2x) e^{mx} \).
  • Complex Roots: If the roots are complex, say \( m = a \pm bi \), the real solution uses trigonometric functions, expressed as \( y = e^{ax} (c_1 \cos(bx) + c_2 \sin(bx)) \).
Understanding whether the characteristic equation's roots are real or complex helps predict the structure of differential equation solutions, making further analysis or application much more straightforward.

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Most popular questions from this chapter

$$6 x^{3} y^{\prime \prime \prime}+\left(13 x^{2}-x^{3}\right) y^{\prime \prime}+x y^{\prime}-x y=0$$

To obtain two linearly independent solutions to $$\quad x^{2} y^{\prime \prime}+\left(x+x^{2}\right) y^{\prime}+y=0, \quad x>0$$ complete the following steps. (a) Verify that \((46)\) has a regular singular point at \(x=0\) and that the associated indicial equation has complex roots \(\pm i\) (b) As discussed in Section \(8.5,\) we can express $$\begin{aligned} x^{\alpha+i \beta} &=x^{\alpha} x^{i \beta} \\ &=x^{\alpha} \cos (\beta \ln x)+i x^{\alpha} \sin (\beta \ln x) \end{aligned}$$ Deduce from this formula that $$\frac{d}{d x} x^{\alpha+i \beta}=$$ $$(\alpha+i \beta) x^{\alpha-1+i \beta}$$ (c) Set \(y(x)=\Sigma_{n=0}^{\infty} a_{n} x^{n+i},\) where the coefficients now are complex constants, and substitute this series into equation \((46)\) using the result of part (b). (d) Setting the coefficients of like powers equal to zero, derive the recurrence relation \(a_{n}=-\frac{n-1+i}{(n+i)^{2}+1} a_{n-1}, \quad\) for \(n \geq 1\) (e) Taking \(a_{0}=1,\) compute the coefficients \(a_{1}\) and \(a_{2}\) and thereby obtain the first few terms of a complex solution to \((46)\) (f) By computing the real and imaginary parts of the solution obtained in part (e), derive the following linearly independent real solutions to (46): $$\begin{aligned} y_{1}(x)=&[\cos (\ln x)]\left\\{1-\frac{2}{5} x+\frac{1}{10} x^{2}+\cdots\right\\} \\ &+[\sin (\ln x)]\left\\{\frac{1}{5} x-\frac{1}{20} x^{2}+\cdots\right\\} \\ y_{2}(x)=&[\cos (\ln x)]\left\\{-\frac{1}{5} x+\frac{1}{20} x^{2}+\cdots\right\\} \\ &+[\sin (\ln x)]\left\\{1-\frac{2}{5} x+\frac{1}{10} x^{2}+\cdots\right\\} \end{aligned}$$

Let \(f(x)\) and \(g(x)\) be analytic at \(x_{0} .\) Determine whether the following statements are always true or sometimes false: (a) \(3 f(x)+g(x)\) is analytic at \(x_{0}\) (b) \(f(x) / g(x)\) is analytic at \(x_{0}\) (c) \(f^{\prime}(x)\) is analytic at \(x_{0}\) (d) \([f(x)]^{3}-\int_{x_{0}}^{x} g(t) d t\) is analytic at \(x_{0}\)

\(x^{2} y^{\prime \prime}+x y^{\prime}+x^{2} y=0\)

van der Pol Equation. In the study of the vacuum tube, the following equation is encountered:$$y^{\prime \prime}+(0.1)\left(y^{2}-1\right) y^{\prime}+y=0$$ Find the Taylor polynomial of degree 4 approximating the solution with the initial values \(y(0)=1\), \(y^{\prime}(0)=0\).

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