Animated Solution for Mathematics - Differential Equations: The solution of the differential equation (x2+y2)dx−5xydy=0,y(1)=0, is :
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Visualized Solution
Analyze the Differential Equation
Given equation: (x2+y2)dx−5xydy=0
Initial condition: y(1)=0
Rearrange to dxdy Form
Rearranging the terms:
5xydy=(x2+y2)dx
dxdy=5xyx2+y2
Identify Homogeneity
Degree of numerator (x2+y2)=2
Degree of denominator (5xy)=2
The equation is Homogeneous.
Substitution Strategy
Let y=vx
Differentiating with respect to x:
dxdy=v+xdxdv
Apply Substitution
Substituting into dxdy=5xyx2+y2:
v+xdxdv=5x(vx)x2+(vx)2
Simplify the Expression
v+xdxdv=5x2vx2(1+v2)
v+xdxdv=5v1+v2
Isolate xdxdv
xdxdv=5v1+v2−v
xdxdv=5v1+v2−5v2
xdxdv=5v1−4v2
Separate the Variables
Separating variables:
1−4v25vdv=xdx
Integrate Both Sides
Integrating both sides:
∫1−4v25vdv=∫x1dx
−85ln∣1−4v2∣=ln∣x∣+C
Apply Logarithmic Properties
Multiply by −8:
5ln∣1−4v2∣=−8ln∣x∣+C′
ln∣1−4v2∣5=ln∣x∣−8+C′
Remove Logarithms
Taking exponential:
∣1−4v2∣5=Kx−8
x8∣1−4v2∣5=K
Back Substitution
Substitute v=xy:
x8∣1−4x2y2∣5=K
x8∣x2x2−4y2∣5=K
Final Algebraic Simplification
x8x10∣x2−4y2∣5=K
x2∣x2−4y2∣5=K
∣x2−4y2∣5=Kx2
Apply Initial Condition
Using y(1)=0:
∣12−4(0)2∣5=K(1)2
15=K(1)⟹K=1
Final Solution
Substitute K=1:
∣x2−4y2∣5=x2
This matches Option 3.
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The Sigma Insight: Homogeneous Differential Equations
Solution Diagram
The Art of the Homogeneous Transformation
Welcome, fellow JEE aspirant. Today, we are not just solving a differential equation; we are embarking on a journey of pattern recognition.
When you first look at the equation (x2+y2)dx−5xydy=0, it might seem like a chaotic jumble of variables. But to the trained eye, this is a beautiful, structured puzzle waiting to be solved.
Phase 1
The Diagnosis
Before we touch a single piece of algebra, we must diagnose the problem. Look at the terms: x2, y2, and 5xy.
Notice something? Every single term has a total degree of 2. This is the hallmark of a homogeneous differential equation.
In the world of JEE, recognizing this is half the battle. It tells us that the equation has a specific symmetry, and that symmetry is our golden ticket to a solution.
We start by rearranging the equation to isolate the derivative, dxdy:
5xydxdy=x2+y2⟹dxdy=5xyx2+y2
Phase 2
The Transformation
Now, we introduce our most powerful tool: the substitution y=vx. Why do we do this? Because it transforms a non-separable equation into a separable one.
If y=vx, then by the product rule, the derivative is:
dxdy=v+xdxdv
Let us substitute this into our equation. This is where you must be meticulous. Do not rush. Replace every y with vx:
v+xdxdv=5x(vx)x2+(vx)2
Watch the magic happen. The x2 terms in the numerator and denominator are identical. They cancel out, leaving us with a clean, manageable expression:
v+xdxdv=5v1+v2
Phase 3
The Calculus Battle
We are now in the home stretch. We need to isolate the variables. Move the v to the right side:
xdxdv=5v1+v2−v=5v1+v2−5v2=5v1−4v2
Now, separate the variables. Bring all the v terms to the left and all the x terms to the right:
1−4v25vdv=xdx
This is the moment of truth. Integrating the right side is trivial: ln∣x∣+C. But the left side requires a steady hand.
We recognize that the derivative of the denominator (1−4v2) is −8v. We have 5v in the numerator. By adjusting the constants, we get:
−85ln∣1−4v2∣=ln∣x∣+C
Phase 4
The Final Polish
We are almost at the finish line. We need to clean up these logarithms. Multiply by −8 and use the properties of logs to bring the coefficients inside as exponents:
5ln∣1−4v2∣=−8ln∣x∣+C′
Exponentiating both sides allows us to remove the logs, leading us to:
∣1−4v2∣5=Kx−8
Substituting back v=xy, we get:
1−4x2y25=Kx−8⟹x2x2−4y25=Kx−8
Simplifying this, we arrive at the general solution:
∣x2−4y2∣5=Kx2
Finally, we apply our initial condition y(1)=0. Plugging these values in, we find K=1.
Our final, elegant solution is:
∣x2−4y2∣5=x2
This matches our target option perfectly. Remember, the math is not just about the final answer; it is about the journey of transformation. You have successfully navigated the complexity of a homogeneous differential equation.