Imagine you are standing in a room, and before you hangs a perfectly flat, infinite mirror. In our problem, this mirror is a plane defined by the equation x−2y=0.
You are holding a point P(−1,3,4) in your hand, and you want to see where its reflection, P′, would appear in this mirror. This is a fundamental exploration of symmetry in three-dimensional space.
The Geometry of the Reflection
To find the image P′(x′,y′,z′), we must understand the path of light. The line connecting the object P and its image P′ must be perpendicular to the plane.
This means the line is parallel to the plane's normal vector, n=(1,−2,0). The plane acts as the perpendicular bisector of the segment PP′.
Our task is to find the point P′ such that the midpoint of PP′ lies on the plane and the vector PP′ is parallel to n.
The Power of the Formula
We use the elegant standard formula for the image of a point (x1,y1,z1) in a plane ax+by+cz+d=0:
This formula is a masterpiece of vector geometry. The term on the right is a constant ratio, which encapsulates the distance from the point to the plane.
The −2 is the key—it ensures we jump from the point, through the plane, and land exactly the same distance on the other side.
Step-by-Step Execution
First, we identify our parameters: x1=−1, y1=3, z1=4, and the plane coefficients a=1, b=−2, c=0, d=0.
Now, let's calculate the constant ratio k:
k=−212+(−2)2+021(−1)−2(3)+0(4)+0
Simplifying the numerator: 1(−1)−2(3)=−1−6=−7. The denominator is 12+(−2)2+02=1+4=5.
Thus, k=−2(5−7)=514.
Calculating Coordinates
With k in hand, we find the coordinates:
For x′:
1x′−(−1)=514⇒x′=514−1=59
For y′:
−2y′−3=514⇒y′−3=−528⇒y′=3−528=−513
For z′:
0z′−4=514
Since the denominator is zero, the numerator must be zero, so z′−4=0, which gives z′=4.
The Final Revelation
Our calculated image point is P′(59,−513,4).
In the high-stakes environment of the JEE, this is the moment where confidence in your process is your greatest asset. Do not doubt your math; trust the geometry.
The correct answer is 'None of these'. You have successfully navigated the mirror, and the physics of the reflection remains perfectly consistent.