/*! 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 44 Find the family of curves tangen... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the family of curves tangent to the force field $$ \mathbf{F}(x, y)=\underbrace{\frac{x^{2}-y^{2}}{\sqrt{x^{2}+y^{2}}}}_{d x / d t} \mathbf{i}-\underbrace{\frac{2 x y}{\sqrt{x^{2}+y^{2}}}}_{d y / d t} \mathbf{j} . $$

Short Answer

Expert verified
-xy - (3/2)y² = C

Step by step solution

01

- Understand the Components

Identify the components of the force field. The force field given is \[ \mathbf{F}(x, y)= -\frac{x y+y^{2}}{\sqrt{x^{2}+y^{2}}} \mathbf{i} + \frac{y^{2}}{\sqrt{x^{2}+y^{2}}} \mathbf{j}.\] This vector field has components corresponding to the derivative of the position with respect to time.
02

- Set Up Differential Equations

The vector field components correspond to \( \frac{dx}{dt} \) and \( \frac{dy}{dt} \). Thus, we have \( \frac{dx}{dt} = - \frac{xy + y^2}{\sqrt{x^2 + y^2}} \) and \( \frac{dy}{dt} = \frac{y^2}{\sqrt{x^2 + y^2}} \).
03

- Eliminate the Parameter t

Divide \( \frac{dy/dt}{dx/dt} \) to eliminate t. This gives: \[ \frac{dy}{dx} = \frac{ \frac{y^2}{\sqrt{x^2 + y^2}} }{ -\frac{xy + y^2}{\sqrt{x^2 + y^2}} } = \frac{y^2}{-(xy + y^2)} \] which simplifies to \[ \frac{dy}{dx} = -\frac{y}{x + y}. \]
04

- Solve the Separable Differential Equation

Rearrange the equation \( \frac{dy}{dx} = -\frac{y}{x + y} \). This can be solved by making the substitution \( u = x + y \), resulting in: \[ \frac{dy}{dx} = -\frac{y}{u}, \] which is a separable differential equation.
05

- Integrate Both Sides

Separate the variables: \( -u \, dy = y \, dx \). Integrate both sides: \[ \int -u \, dy = \int y \, dx \]. Integrating, we obtain: \[-uy = \frac{y^2}{2} + C. \]
06

- Solve for y

Re-substitute \( u = x + y \), resulting in: \(- (x + y) y = \frac{y^2}{2} + C. \). Simplify it to find: \[ -xy - y^2 = \frac{y^2}{2} + C \Rightarrow -xy - \frac{3y^2}{2} = C. \]. Which describes the family of curves.

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Key Concepts

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

Vector Fields
Vector fields are mathematical constructions where vectors are assigned to points in a space.
For instance, in the given problem, the vector field \(\textbf{F}(x, y)= - \frac{x y+y^{2}}{\sqrt{x^{2}+y^{2}}} \textbf{i} + \frac{y^{2}}{\sqrt{x^{2}+y^{2}}} \textbf{j}\) maps vectors at each point \( (x, y) \)
This help describe how the force field 'flows' through space.
Components of this field correspond to the changes in position over time for x and y.
As a result, we can set up differential equations by relating these components to the derivatives \( \frac{dx}{dt} \) and \( \frac{dy}{dt} \).
This linkage is crucial in solving the exercise. By visualizing vector fields, an intuitive grasp of particle motion under various forces can be achieved.

Separable Differential Equations
A separable differential equation is an equation where the variables can be separated on opposite sides.
For instance, given \(\frac{dy}{dx} = -\frac{y}{x+y}\), we can rewrite this by substituting \(u = x + y\).
This gives us \( \frac{dy}{dx} = -\frac{y}{u} \). The key here is to recognize that the equation can be split into parts that only contain y or x.
Hence, it becomes \(-(x+y)dy = y dx\). We separate it into \( -u \, dy = y \, dx \), effectively splitting x and y.
This lets us integrate both sides independently, which simplifies the equation.
When the variables are separable, solving differential equations becomes much simpler and often just involves straightforward integration.

Parameter Elimination
Eliminating a parameter like t is often essential in solving differential equations.
In our example, we first had the equations \( \frac{dx}{dt} = - \frac{xy + y^2}{\sqrt{x^2 + y^2}} \) and \( \frac{dy}{dt} = \frac{y^2}{\sqrt{x^2 + y^2}} \).
By dividing these expressions, we obtain \(\frac{dy}{dx} = \frac{\frac{y^2}{\sqrt{x^2+y^2}} }{ -\frac{xy + y^2}{\sqrt{x^2+y^2}} } = \frac{y^2}{-(xy + y^2)}\).This leads to \(\frac{dy}{dx} = -\frac{y}{x + y}\).
This step effectively removes the parameter t, transforming a complex system of equations into a single, simpler differential equation involving just x and y.
This simplification is what allows us to proceed with solving the equation step-by-step.

Integration
Finally, integration helps us solve differential equations to find the relationship between the variables.
In our problem, after separation, we integrate both sides of \(-u \, dy = y \, dx\).
This results in \(\int -u \, dy = \int y \, dx \), which when integrated gives \( -uy = \frac{ y^2}{2} + C \).
Integration turns the differential form into an algebraic expression, which we can then manipulate to find general solutions.
Lastly, re-substituting u provides the final relational family to y and x: \( - (x + y) y = \frac{y^2}{2} + C \).
Integrating is thus a fundamental tool in converting equations to a more comprehensible form.
By using these steps, we find specific solutions that satisfy the original conditions.

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Most popular questions from this chapter

(First Order Linear Equations with Periodic Forcing Function) Consider the differential equation \(d y / d t+c y=f(t)\), where \(f(t)\) is a periodic function and \(c\) is a constant. The goal of this exercise is to determine if equations of this form have a periodic solution. (a) Solve the IVP \(y^{\prime}+y / 2=\) \(\sin t, y(0)=a\). For what values of \(a\) does the IVP have a periodic solution? Graph the slope field for this ODE. Describe the behavior of the other solutions. Do they approach the periodic solution found in (a) as \(t \rightarrow \infty\) or \(t \rightarrow-\infty\) ? (b) Solve the IVP \(y^{\prime}-y / 2=\sin t, y(0)=a\). For what values of \(a\) does the IVP have a periodic solution? Graph the slope field for this ODE. Describe the behavior of the other solutions. Do they approach the periodic solution found in (b) as \(t \rightarrow \infty\) or \(t \rightarrow-\infty\) ? (c) Based on your findings in (a) and (b), does the ODE \(y^{\prime}+\) \(c y=f(t)\), where \(f(t)\) is a periodic function and \(c\) is a constant, have a periodic solution? How does the value of \(c\) affect the other solutions?

\(t d y / d t+y=\cos t, y(\pi / 2)=4 / \pi, t>0\)

(Pollution) Under normal atmospheric conditions, the density of soot particles \(N(t)\) satisfies the differential equation $$ \frac{d N}{d t}=-k_{c} N^{2}+k_{d} N, $$ where \(k_{c}\), called the coagulation constant, is a constant that relates to how well particles stick together; and \(k_{d}\), called the dissociation constant, is a constant that relates to how well particles fall apart. Both of these constants depend on temperature, pressure, particle size, and other external forces. \({ }^{3}\) (a) Find a general solution of this Bernoulli equation. (b) Find the solution that satisfies the initial condition \(N(0)=N_{0} \cdot\left(N_{0}>0\right)\) The following table lists typical values of \(k_{c}\) and \(k_{d}\). \begin{tabular}{l|l} \hline\(k_{c}\) & \(k_{d}\) \\ \hline 163 & 5 \\ 125 & 26 \\ 95 & 57 \\ 49 & 85 \\ 300 & 26 \\ \hline \end{tabular} (c) For each pair of values in the previous table, sketch the graph of \(N(t)\) if \(N(0)=N_{0}\) for \(N_{0}=0.01,0.05,0.1,0.5\), \(0.75,1,1.5\), and 2. Regardless of the ini-tial condition \(N(0)=N_{0}\), what do you notice in each case? Do pollution levels seem to be more sensitive to \(k_{c}\) or \(k_{d}\) ? Does your result make sense? Why? (d) Show that if \(k_{d}>0, \lim _{t \rightarrow \infty} N(t)=\) \(k_{d} / k_{c}\). Why is the assumption that \(k_{d}>\) 0 reasonable? (e) For each pair in the table, calculate \(\lim _{t \rightarrow \infty} N(t)=k_{d} / k_{c}\). Which situation results in the highest pollution levels? How could the situation be changed?

\(d x / d t=x+t+1, x(0)=2\)

\(2 t y^{\prime}-y=2 t y^{3} \cos t\)

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