Animated Solution for Mathematics - Differential Equations: Let the solution curve of the differential equation xdy−ydx=x2+y2dx,x>0,y(1)=0, be y=y(x). Then y(3) is equal to
Select Answer:
Visualized Solution
Analyze the Differential Equation
Given Equation: xdy−ydx=x2+y2dx
Initial Condition: y(1)=0
Goal: Find y(3)
Rearranging to Standard Form
Divide by dx: xdxdy−y=x2+y2
Rearrange: xdxdy=y+x2+y2
Substitution for Homogeneous DE
Let y=vx
Differentiating with respect to x: dxdy=v+xdxdv
Substituting into the Equation
Substitute: x(v+xdxdv)=vx+x2+(vx)2
Simplify RHS: xv+x2dxdv=vx+x1+v2
Simplifying the Expression
Cancel vx: x2dxdv=x1+v2
Divide by x: xdxdv=1+v2
Variable Separation
Separate variables: 1+v2dv=xdx
Integration Step
Integrate: ∫1+v2dv=∫xdx
Result: ln(v+1+v2)=lnx+C
Applying Initial Condition
At x=1,y=0⟹v=10=0
Substitute: ln(0+1+0)=ln1+C
ln(1)=ln(1)+C⟹C=0
Finding the General Solution
ln(v+1+v2)=lnx
v+1+v2=x
Substitute v=xy: xy+1+x2y2=x
Multiply by x: y+x2+y2=x2
Solving for y(3)
Put x=3: y+32+y2=32
y+9+y2=9
Rearrange: 9+y2=9−y
Square both sides: 9+y2=(9−y)2
Final Calculation
Expand: 9+y2=81+y2−18y
Cancel y2: 9=81−18y
Rearrange: 18y=72
Final Answer: y=4
Conclusion and Takeaway
Key Takeaway: For equations of form M(x,y)dx+N(x,y)dy=0 where M,N are homogeneous, use y=vx.
The solution curve is a parabola: y=2x2−1
Final Value: y(3)=4
00:00 / 00:00
The Sigma Insight: Homogeneous Differential Equations
Solution Diagram
Analyzing the Setup
Welcome, fellow traveler of the JEE journey. Today, we stand before a differential equation that might look like a tangled knot of variables, but it is a masterpiece of symmetry waiting to be unraveled.
We are looking at the equation xdy−ydx=x2+y2dx. At first glance, the presence of xdy−ydx and the radical x2+y2 might feel intimidating.
However, observe the homogeneity; every term here has a degree of one. This is our signal, our 'green light' to deploy the powerful substitution y=vx.
The Transformation
To begin, we rearrange our equation into the standard form:
dxdy=xy+x2+y2
By setting y=vx, we invoke the product rule: dxdy=v+xdxdv. When we substitute this into our equation, the vx terms on both sides cancel out.
This leaves us with xdxdv=1+v2. This is the moment where the complexity collapses into a beautiful, separable form.
The Integration
Now, we separate our variables by bringing all the v terms to one side and the x terms to the other:
∫1+v2dv=∫xdx
This integral is a classic in the JEE repertoire. The left side integrates to ln(v+1+v2), and the right side is simply ln∣x∣+C.
Applying our initial condition y(1)=0 is where we find our constant. Since v=xy, at x=1 and y=0, we find v=0.
Substituting these into our integrated equation, we get ln(0+1+0)=ln(1)+C, which simplifies to 0=0+C. Thus, C=0.
The Final Reveal
The elegance of this result is breathtaking—the constant vanishes, leaving us with the relationship ln(v+1+v2)=lnx. By exponentiating both sides, we strip away the logarithms to reveal:
v+1+v2=x
Substituting v=xy back into the equation, we get xy+1+x2y2=x. Multiplying through by x, we arrive at the final curve equation:
y+x2+y2=x2
Now, we reach the final act: finding y(3). Plugging x=3 into our equation, we get y+9+y2=9.
Rearranging this to 9+y2=9−y and squaring both sides, the y2 terms vanish: