Analyzing the Setup
In 3D space, a line is defined by its direction and a point it passes through. The symmetric form given,
is elegant, but it is static. To find an intersection, we must parameterize the line.
By setting the symmetric equation equal to a parameter λ, we describe any point on the line as a function of this single variable:
This serves as our coordinate on L1. As λ changes, we traverse the line. We apply the same logic to L2 using a distinct parameter μ:
The Collision
If the lines intersect at a point R, then at that specific location, the coordinates of P1 and P2 must be identical. We equate the components to find the intersection:
For the
x-coordinate:
3+λ=−5+7μ⇒λ−7μ=−8(Equation 1)
For the
y-coordinate:
−1+3λ=2−6μ⇒3λ+6μ=3
Simplifying the
y-equation by dividing by
3, we obtain:
λ+2μ=1(Equation 2)
Solving the System
We now have a clean system of two linear equations:
1) λ−7μ=−8
2) λ+2μ=1
Subtracting the first equation from the second, the λ terms vanish, leaving us with 9μ=9, which yields μ=1. Substituting this back into Equation 2, we find λ=1−2(1)=−1.
Finding the Intersection Point
With λ=−1, we determine the intersection point R by substituting the parameter back into our expression for P1:
x=3+(−1)=2
y=−1+3(−1)=−4
z=6−(−1)=7
Thus, the point of intersection is R=(2,−4,7).
The Reflection
We must now find the reflection of R in the xy-plane. Imagine the xy-plane as a mirror at z=0.
Reflecting a point across this plane preserves the (x,y) coordinates while inverting the depth (z). Thus, the transformation is defined as (x,y,z)→(x,y,−z).
Applying this to R(2,−4,7), we obtain the final reflected point:
R′=(2,−4,−7)