The Geometry of Skew Lines
Imagine you are standing in a vast, three-dimensional space. You see two laser beams, L1 and L2, crossing each other but never touching. These are skew lines.
We are tasked with finding the square of the distance between two points, A on L1 and B on L2, such that the line segment AB has a specific orientation defined by the direction ratios (1,−4,2). This is not just a calculation; it is a journey of finding order in the chaos of 3D space.
Phase 1
The Parametric GPS
To navigate this space, we need a way to pinpoint any location on these lines. We use the parametric form.
For line L1:3x−7=−1y−1=1z+2, we introduce a parameter λ. By setting this equal to λ, we can express any point A as (3λ+7,−λ+1,λ−2).
Similarly, for line L2:2x=3y−7=1z, we use a different parameter μ to define point B as (2μ,3μ+7,μ). Think of λ and μ as the GPS coordinates for points A and B on their respective lines.
Phase 2
The Vector Connection
Now that we have the coordinates for A and B, we need to define the line segment AB. The direction ratios of a line passing through two points (x1,y1,z1) and (x2,y2,z2) are simply the differences in their coordinates: (x2−x1,y2−y1,z2−z1).
Applying this to our points, the direction ratios of
AB are:
(3λ−2μ+7,−λ−3μ−6,λ−μ−2)
This vector represents the 'compass heading' of our segment
AB.
Phase 3
The Proportionality Trap
The problem gives us the direction ratios of AB as (1,−4,2). A common mistake is to assume these are equal to our calculated ratios.
However, direction ratios are proportional. We must set up the proportionality:
13λ−2μ+7=−4−λ−3μ−6=2λ−μ−2
This is the heart of the problem. By equating these ratios, we create a system of linear equations that will lock our points
A and
B into their correct positions.
Phase 4
Solving the System
Let's break down the algebra. Taking the first two parts of the ratio and cross-multiplying, we get:
−12λ+8μ−28=−λ−3μ−6
This simplifies beautifully to
λ−μ+2=0.
Now, taking the second and third parts, we get:
−2λ−6μ−12=−4λ+4μ+8
This simplifies to
λ−5μ−10=0.
Solving this system is straightforward: subtracting the second from the first yields 4μ+12=0, so μ=−3. Substituting this back gives λ=−5. We have found the exact parameters that define our points.
Phase 5
The Final Distance
With
λ=−5 and
μ=−3, we find the coordinates:
A=(−8,6,−7)andB=(−6,−2,−3)
The final step is to calculate the square of the distance
(AB)2=(xB−xA)2+(yB−yA)2+(zB−zA)2. Plugging in our values:
(AB)2=(−6−(−8))2+(−2−6)2+(−3−(−7))2
(AB)2=(2)2+(−8)2+(4)2=4+64+16=84
The elegance of the final result is a testament to the power of parametric geometry. The square of the distance is 84.