Problem 54
Question
Solution of \(\frac{x d x+y d y}{x d y-y d x}=\frac{\sqrt{1-\left(x^{2}+y^{2}\right)}}{\sqrt{x^{2}+y^{2}}}\) is (A) \(\sin ^{-1} \sqrt{x^{2}+y^{2}}=c\) (B) \(\tan ^{-1} \frac{y}{x}=c\) (C) \(\sin ^{-1 \sqrt{x^{2}+y^{2}}}=\tan ^{-1 \frac{y}{x}}+c\) (D) None of these
Step-by-Step Solution
Verified Answer
Option (C) is correct: \( \sin ^{-1 \sqrt{x^{2}+y^{2}}} = \tan ^{-1 \frac{y}{x}} + c \).
1Step 1: Rearranging the Differential Equation
The given equation \( \frac{x \, dx + y \, dy}{x \, dy - y \, dx} = \frac{\sqrt{1-(x^2+y^2)}}{\sqrt{x^2+y^2}} \) needs to be simplified by setting \( R = \sqrt{x^2+y^2} \). This simplifies the equation into polar coordinates.
2Step 2: Transform into Polar Coordinates
Setting \( x = R \cos \theta \) and \( y = R \sin \theta \), differentiate these: \( dx = \cos \theta \, dR - R \sin \theta \, d\theta \), \( dy = \sin \theta \, dR + R \cos \theta \, d\theta \). Substitute these into the equation.
3Step 3: Simplify the Equation
The numerator becomes \( R \cos \theta \, dR - R \sin \theta \, d\theta + R \sin \theta \, dR + R \cos \theta \, d\theta \) and the denominator becomes \( R \sin \theta \, dR + R \cos \theta \, d\theta - R \cos \theta \, dR + R \sin \theta \, d\theta \). This simplifies to \( dR \) over \( R^2 \, d\theta \).
4Step 4: Separate Variables
We now have \( \frac{dR}{R} = \tan \theta \, d\theta \). These can be integrated separately: \( \int \frac{dR}{R} = \ln R + C_1 \) and \( \int \tan \theta \, d\theta = -\ln |\cos \theta| + C_2 \).
5Step 5: Solve Integrals
Solving \( \ln R = -\ln |\cos \theta| + C \), where \( C = C_2 - C_1 \). This simplifies to \( R \cos \theta = e^C \), implying \( \sqrt{x^2 + y^2} \cos \theta = C \).
6Step 6: Formulate General Solution
With the equation reformulated, it implies \( \sqrt{x^2+y^2} = \sin^{-1}(C) \), which combines the given conditions.
Key Concepts
Polar CoordinatesIntegrationVariable Separation
Polar Coordinates
Polar coordinates are a system where a point in a plane is determined by a distance from a reference point and an angle from a reference direction. This system is particularly helpful when dealing with problems involving circular or rotational symmetry, often simplifying equations that are complex in Cartesian coordinates.
In the context of the differential equation given in the exercise, converting to polar coordinates assists in simplifying the equation. Instead of expressing points using the usual Cartesian system
In the context of the differential equation given in the exercise, converting to polar coordinates assists in simplifying the equation. Instead of expressing points using the usual Cartesian system
- where values are given as \( (x, y) \),
- the radius \( R = \sqrt{x^2 + y^2} \)
- and the angle \( \theta \), with formulas \( x = R \cos \theta \) and \( y = R \sin \theta \).
Integration
Integration is a fundamental concept in calculus that helps in finding functions from given derivatives, commonly recognized as finding the area under curves. In the exercise, once the differential equation has been rearranged into polar coordinates, we reach a point where integration becomes essential.
After separating variables, we obtain an expression with the differentials \( \frac{dR}{R} \) and \( \tan \theta \, d\theta \). By
It is important to acknowledge that the constants of integration \( C_1 \) and \( C_2 \) capture the arbitrary nature of antiderivatives, permitting a range of functions that satisfy the equation in different contexts.
After separating variables, we obtain an expression with the differentials \( \frac{dR}{R} \) and \( \tan \theta \, d\theta \). By
- integrating \( \frac{dR}{R} \),
- integrating \( \tan \theta \, d\theta \)
It is important to acknowledge that the constants of integration \( C_1 \) and \( C_2 \) capture the arbitrary nature of antiderivatives, permitting a range of functions that satisfy the equation in different contexts.
Variable Separation
Variable separation is a method commonly employed in solving differential equations. It involves rearranging the equation so that all terms involving one variable can be placed on one side, and those involving another variable on the other side. This allows each side to be integrated independently, simplifying the process of solving the equation.
In the given problem, after transforming into polar coordinates and simplifying, we arrive at the separated form \( \frac{dR}{R} = \tan \theta \, d\theta \).
This enables us to integrate each side independently:
In the given problem, after transforming into polar coordinates and simplifying, we arrive at the separated form \( \frac{dR}{R} = \tan \theta \, d\theta \).
This enables us to integrate each side independently:
- \( \int \frac{dR}{R} \) yields \( \ln R \),
- while \( \int \tan \theta \, d\theta \) results in \(-\ln |\cos \theta|\).
Other exercises in this chapter
Problem 52
Solution of the differential equation \(y d x+\left(x+x^{2} y\right)\) \(d y=0\) is (A) \(\log y=C x\) (B) \(-\frac{1}{x y}+\log y=C\) (C) \(\frac{1}{x y}+\log
View solution Problem 53
The equation of the curve for which the square of the ordinate is twice the rectangle contained by the abscissa and the \(x\)-intercept of the normal and passin
View solution Problem 55
The solution of the differential equation \((x \cos x-\sin\) \(\left.x+y x^{2}\right) d x+x^{3} d y=0\) is equal to (A) \(\frac{\sin x}{x}+x y=c\) (B) \(\frac{\
View solution Problem 56
Solution of the differential equation \(\left[y\left(1+x^{-1}\right)+\sin y\right] d x+(x+\log x+x \cos y) d y=0\) is (A) \(x y+y \log x=c\) (B) \(x y+x \sin y=
View solution