Analyzing the Setup
Imagine you are standing at the origin of a coordinate plane, watching a line L rotate like the hand of a clock. As it sweeps through the plane, it slices through two parallel lines, x+y=1 and x+y=3.
These two lines are our fixed stage, and the rotating line L is our dynamic actor. Our goal is to track the intersection point R of two other lines, L1 and L2, which are born from the points of intersection P and Q.
The Stage and the Actor
First, let us define our stage. We have two parallel lines, x+y=1 and x+y=3. Because they share the same slope, they remain perfectly equidistant.
Now, our actor, the line L, passes through the origin. We define its equation as y=mx, where m is the variable slope. As m changes, the line L rotates, and the points P and Q slide along our parallel lines.
Finding the Coordinates
To find the intersection point P, we solve y=mx and x+y=1 simultaneously. Substituting y=mx into the line equation gives x+mx=1, which simplifies to x(1+m)=1.
Thus, the coordinates of
P are:
P=(1+m1,1+mm)
Applying the same logic to
Q with the line
x+y=3, we find
x(1+m)=3. This gives us the coordinates of
Q as:
Q=(1+m3,1+m3m)
Notice the elegance here: Q is simply 3P. The origin acts as a center of scaling, a beautiful geometric symmetry.
The New Paths
Now, we draw L1 through P with a slope of 2 (parallel to 2x−y=5) and L2 through Q with a slope of −3 (parallel to 3x+y=5). Let the intersection of these two lines be R(X,Y).
Using the point-slope form, the equation for
L1 is:
Y−1+mm=2(X−1+m1)
Similarly, for
L2, we have:
Y−1+m3m=−3(X−1+m3)
The Algebraic Symphony
Now, we face the challenge: eliminating the parameter
m. Let us rearrange the equation for
L1:
Y−2X=1+mm−1+m2=1+mm−2
By writing
m−2 as
(m+1)−3, we get
Y−2X=1−1+m3. This gives us the isolated term:
1+m3=1−Y+2X
Now, let us look at
L2:
Y+3X=1+m3m+1+m9=1+m3m+9
Writing
3m+9 as
3(m+1)+6, we get
Y+3X=3+1+m6. This gives us:
1+m6=Y+3X−3
The Grand Finale
Here is the moment of truth. We observe that
1+m6=2×(1+m3). Substituting our expression from
L1 into
L2, we get:
Y+3X−3=2(1−Y+2X)
Expanding this, we find:
Y+3X−3=2−2Y+4X
Bringing all terms to one side, we arrive at the final locus:
X−3Y+5=0
The parameter m has vanished, leaving us with a clean, linear equation. The locus of R is a straight line. You have successfully navigated the complexity and found the underlying simplicity. The final answer is X−3Y+5=0.