Analyzing the Setup
Imagine you are standing in a vast, three-dimensional space. You see a point P(1,2,a) suspended in the air, and below it, a line L defined by the equation:
We are tasked with finding the distance from P to L along two specific, predefined paths, L1 and L2, under the condition that these distances are equal.
The First Encounter
Finding Point A
Let us focus on the first path, L1, defined by:
Any point on this line can be described by the parameter λ. Let the intersection point be A, with coordinates (3λ+1,4λ+2,bλ+a).
Because A also lies on the line L, its coordinates must satisfy the equation of L. Substituting these coordinates into the equation of L, we get:
1(3λ+1)−1=24λ+2=1(bλ+a)−1
Simplifying this, we find:
By equating the first two terms, 3λ=2λ+1, we find that λ=1. Substituting λ=1 into the third term, we discover the elegant relation a+b=4. Our point A is now fixed at (4,6,4).
The Second Encounter
Finding Point B
Now, we repeat this process for the second path, L2, defined by:
Let the intersection point be B, with coordinates (μ+1,4μ+2,cμ+a). Since B lies on L, we substitute its coordinates into the equation of L:
1(μ+1)−1=24μ+2=1(cμ+a)−1
This simplifies to:
Equating the first two terms, μ=2μ+1, we find μ=−1. Substituting μ=−1 into the third term, we get −1=−c+a−1, which simplifies to a=c. Our point B is (0,−2,0).
The Climax
The Distance Equality
The problem states that the distances from P to L along these two paths are equal, meaning PA=PB. To make our calculations cleaner, we work with the squares of the distances: PA2=PB2.
Using the distance formula:
PA2=(4−1)2+(6−2)2+(4−a)2=25+(4−a)2
PB2=(0−1)2+(−2−2)2+(0−a)2=17+a2
Setting them equal, we have:
The a2 terms cancel out, leaving us with 41−8a=17, or 8a=24. Thus, a=3.
With a=3, we find b=4−3=1 and c=3. The final sum is:
We have navigated the 3D space, solved the intersections, and arrived at the elegant solution of 7.