Analyzing the Setup
Imagine you are standing in a vast, three-dimensional void. You see two lines, L1 and L2, which are skew lines—they are neither parallel nor intersecting.
A third line, acting as a bridge, cuts through this space to touch both L1 and L2. We are given that the direction ratios of this bridge are (2,1,2).
Our mission is to find the exact coordinates where this bridge meets the two lines.
Phase 1
The Power of Parameterization
To find these points, we use the language of parameters. For line L1, defined by x=y+a=z, we set the expression equal to a scalar λ.
This transforms the line into a set of coordinates: x=λ, y=λ−a, and z=λ. Thus, any point P on L1 is described as (λ,λ−a,λ).
For line L2, defined by x+a=2y=2z, we set the expression equal to a new parameter μ. This yields:
Consequently, any point Q on L2 is (μ−a,2μ,2μ).
Phase 2
The Bridge of Direction Ratios
We now examine the line segment PQ. The direction ratios of a line passing through two points (x1,y1,z1) and (x2,y2,z2) are given by the differences (x1−x2,y1−y2,z1−z2).
By subtracting the coordinates of Q from P, we obtain the direction ratios of our transversal:
(λ−(μ−a),(λ−a)−2μ,λ−2μ)
This simplifies to the vector (λ−μ+a,λ−a−2μ,λ−2μ). This vector represents the orientation of our bridge in space.
Phase 3
The Proportionality Constraint
The problem states that the bridge has direction ratios proportional to (2,1,2). Mathematically, this implies:
2λ−μ+a=1λ−a−2μ=2λ−2μ
We solve this by first equating the first and third ratios, which share the same denominator:
The λ terms cancel out, leaving a=2μ, which simplifies to μ=2a.
Next, we equate the second and third ratios:
Substituting μ=2a into this equation, we get:
Solving for λ, we find λ=3a.
The Final Reveal
We now substitute our parameters back into the coordinate expressions. For point P on L1:
P=(3a,3a−a,3a)=(3a,2a,3a)
For point Q on L2:
Q=(2a−a,22a,22a)=(a,a,a)
We have successfully bridged the gap. The transversal meets L1 at (3a,2a,3a) and L2 at (a,a,a).