Animated Solution for Mathematics - Differential Equations: If a curve passes through the point (1,−2) and has slope of the tangent at any point (x,y) on it as xx2−2y, then the curve also passes through the point :
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Visualized Solution
Understanding the Slope Condition
Given slope of tangent: dxdy=xx2−2y
The curve passes through the initial point (1,−2).
Rearranging to Linear Form
Separate the terms: dxdy=xx2−x2y
Rearrange to standard form: dxdy+x2y=x
This is a Linear Differential Equation of the form dxdy+P(x)y=Q(x)
Where P(x)=x2 and Q(x)=x.
Calculating the Integrating Factor
Integrating Factor (I.F.) =e∫P(x)dx
I.F. =e∫x2dx=e2lnx
Using property alnb=lnba: I.F. =elnx2
Therefore, I.F. =x2
Setting up the General Solution
General Solution: y⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C
Substitute values: y⋅x2=∫x⋅x2dx+C
yx2=∫x3dx+C
Integrating and Finding the Constant
Integrate: yx2=4x4+C
Apply initial condition (1,−2):
(−2)(1)2=4(1)4+C
−2=41+C⟹C=−2−41=−49
The Final Equation of the Curve
Substitute C back: yx2=4x4−49
Multiply by 4: 4yx2=x4−9
This is the specific equation of the curve.
Testing the Options
Check point (3,0):
LHS: 4(0)(3)2=0
RHS: (3)4−9=9−9=0
Since LHS=RHS, the point (3,0) lies on the curve.
Conclusion and Key Takeaway
Key Takeaway: Identifying the type of Differential Equation (Linear in this case) is the first step to success.
Final Answer: The curve passes through (3,0).
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The Sigma Insight: Linear Differential Equations
Solution Diagram
Analyzing the Setup
Imagine you are standing on a path defined by a curve. You do not know the equation of this path, but you know something fundamental about how it behaves: at any point (x,y), the slope of the tangent is given by:
dxdy=xx2−2y
We are given a starting point, (1,−2), which acts as our anchor in the coordinate plane. Our goal is to find the identity of this curve.
The Transformation
Recognizing the Pattern
When we first look at the equation, it feels slightly chaotic. However, we can break the fraction apart to reveal a hidden structure:
dxdy=xx2−x2y⇒dxdy=x−x2y
Now, let us bring the y term to the left side to obtain:
dxdy+x2y=x
Suddenly, the fog clears. This is the classic Linear Differential Equation of the form dxdy+P(x)y=Q(x), where P(x)=x2 and Q(x)=x.
The Magic of the Integrating Factor
To solve this, we need a special tool: the Integrating Factor (I.F.). Think of the I.F. as a mathematical catalyst that forces the left side of our equation to become the derivative of a product.
The formula is defined as:
I.F.=e∫P(x)dx=e∫x2dx
Since the integral of x2 is 2ln(x), we use the properties of logarithms to simplify:
I.F.=e2ln(x)=eln(x2)=x2
This result, x2, is the key that unlocks the door to the solution.
The Integration Journey
Now, we multiply our entire differential equation by this Integrating Factor:
x2(dxdy+x2y)=x2(x)
This simplifies to:
x2dxdy+2xy=x3
Look closely at the left side; it is exactly the derivative of the product y⋅x2. Thus, we can write:
dxd(yx2)=x3
Integrating both sides with respect to x yields:
∫dxd(yx2)dx=∫x3dx⇒yx2=4x4+C
Finding the Anchor
We have the general family of curves, but we need the specific one that passes through (1,−2). Substituting x=1 and y=−2 into our equation:
(−2)(1)2=4(1)4+C
This leads to −2=41+C, which means C=−2−41=−49. Our specific curve equation is:
yx2=4x4−49
Multiplying by 4 to clear the fractions, we arrive at the final equation:
∗∗4yx2=x4−9∗∗
The Final Verification
Finally, we test the point (3,0). Substituting x=3 and y=0 into our derived equation:
4(0)(3)2=(3)4−9
This simplifies to 0=9−9, which is 0=0. The point satisfies the equation perfectly, confirming our result.