Analyzing the Setup
Imagine you are standing on a vast, two-dimensional plane. You have two lines, L and K, stretching out into infinity. They are perfectly parallel, never touching, yet they are defined by the subtle interplay of their intercepts.
Unlocking the Mystery of Line L
We begin with line L, defined by the equation:
We are told it passes through the point P(13,32). In the language of coordinate geometry, this means the point P is a prisoner of this line; its coordinates must satisfy the equation.
By substituting x=13 and y=32, we get:
With a bit of algebraic finesse, we isolate the term:
Solving for b, we find b=−20. Now, our line L is fully revealed:
To make this line easier to work with, we multiply by 20 to reach the standard form:
The Parallelism of Line K
Now, consider line K, defined by:
We are told K is parallel to L. In the world of lines, parallelism is a strict condition: it means they must share the exact same slope.
From our standard form of L, 4x−y−20=0, we can see the slope is 4. For line K, the slope is −c3. Setting these equal, we have:
Substituting this back into the equation for K, we get:
Multiplying by 3, we transform this into −4x+y=3, or:
The Final Calculation
We have arrived at the climax of our journey. We have two parallel lines in their most powerful form:
The distance d between two parallel lines Ax+By+C1=0 and Ax+By+C2=0 is given by the elegant formula:
Here, A=4, B=−1, C1=−20, and C2=3. Plugging these into our formula, we calculate:
This simplifies to:
And there it is—the exact distance between these two parallel paths. The final result is: