Animated Solution for Mathematics - Differential Equations: A particle is moving in the xy-plane along a curve C passing through the point (3,3). The tangent to the curve C at the point P meets the x-axis at Q. If the y-axis bisects the segment PQ, then C is a parabola with
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Visualized Solution
Visualizing the Curve and Point P
Let the curve be C.
Consider a general point P(x,y) on the curve.
The curve passes through the fixed point (3,3).
Equation of the Tangent at P
The equation of the tangent line at point P(x,y) is given by:
Y−y=dxdy(X−x)
Here, (X,Y) are the coordinates of any point on the tangent.
Finding Point Q on the x-axis
The tangent meets the x-axis at point Q.
To find Q, substitute Y=0 into the tangent equation.
0−y=dxdy(X−x)
Coordinates of Point Q
Rearranging to solve for X:
−y=y′(X−x)
X−x=−y′y
X=x−y′y
So, Q is (x−y′y,0).
The Bisection Property
The y-axis bisects the line segment PQ.
This means the midpoint of PQ lies exactly on the y-axis.
Therefore, the x-coordinate of the midpoint must be 0.
Applying the Midpoint Formula
Midpoint x-coordinate formula: 2xP+xQ=0
Substitute xP=x and xQ=x−y′y:
2x+(x−y′y)=0
Forming the Differential Equation
Multiply by 2 to clear the denominator:
2x−y′y=0
Rearrange the terms:
2x=y′y
2x=dxdyy
Separating the Variables
Replace y′ with dxdy:
2x=y⋅dydx
Separate the variables x and y to opposite sides:
ydy=2xdx
Integrating Both Sides
Integrate both sides:
∫y1dy=∫2x1dx
ln∣y∣=21ln∣x∣+C
Let the constant C=lnc:
lny=ln(x1/2)+lnc
Simplifying the Equation
Combine the logarithmic terms:
lny=ln(cx)
Remove the logarithms:
y=cx
Square both sides to get the family of curves:
y2=c2x
Let k=c2, so y2=kx.
Finding the Constant k
We know the curve passes through the point (3,3).
Substitute x=3 and y=3 into y2=kx:
32=k(3)
The Final Equation of the Curve
Solve for k:
9=3k⟹k=3
Substitute k back into the equation:
y2=3x
This is the exact equation of our curve C.
Analyzing the Parabola
Compare y2=3x with the standard parabola y2=4ax.
4a=3⟹a=43
The length of the latus rectum is 4a=3.
The focus is at (a,0)=(43,0).
Notice that option C is (34,0), which is a trap! The correct option is A.
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The Sigma Insight: Variable Separable Method
Solution Diagram
Analyzing the Setup
Imagine you are standing on the xy-plane, watching a particle trace an invisible path. We are given a curve C that passes through the point (3,3).
At any point P(x,y) on this curve, a tangent is drawn, and it meets the x-axis at a point Q. The problem states that the y-axis acts as a perfect mirror, bisecting the segment PQ. This geometric constraint dictates the very shape of the curve.
The Tangent and the Intercept
For any point P(x,y) on the curve, the slope of the tangent is given by the derivative y′=dxdy. The equation of this tangent line, using the point-slope form, is:
Y−y=y′(X−x)
Here, (X,Y) are the coordinates of any point on the line. We are interested in the point Q where this tangent meets the x-axis. At the x-axis, the y-coordinate is zero, so we set Y=0.
This gives us −y=y′(X−x). Solving for X, we find:
X=x−y′y
Thus, the coordinates of Q are (x−y′y,0).
The Midpoint Magic
Now, we apply the bisection property. The y-axis bisects the segment PQ, meaning the midpoint of PQ lies on the y-axis. The x-coordinate of the midpoint is the average of the x-coordinates of P and Q.
Mathematically, this is:
2xP+xQ=0
Substituting xP=x and xQ=x−y′y, we get:
2x+(x−y′y)=0
Simplifying this, we obtain 2x−y′y=0, or:
2x=y′y
This is the differential equation that governs our curve.
Solving the Differential Equation
We can rewrite y′ as dxdy, giving us 2x=y⋅dydx. Rearranging to separate the variables, we get:
ydy=2xdx
Integrating both sides, we have:
∫y1dy=∫2x1dx
This yields ln∣y∣=21ln∣x∣+C. By setting C=lnc, we can combine the logarithms to get lny=ln(cx), which simplifies to y=cx. Squaring both sides, we find the family of curves:
y2=kx
where k=c2. This is indeed a parabola.
The Final Reveal
We know the curve passes through (3,3). Substituting these values into y2=kx, we get:
32=k(3)⇒9=3k⇒k=3
The equation of our curve is y2=3x.
Comparing this to the standard form y2=4ax, we see that 4a=3. The length of the latus rectum is 3, and the focus is at (3/4,0). We have successfully navigated the geometry and calculus to reveal the true nature of the curve.