Animated Solution for Mathematics - Three Dimensional Geometry: If the length of the perpendicular from the point (β,0,β)(β=0) to the line 1x−1=0y−0=−1z+1 is 3/2, then β is equal to :
Select Answer:
Visualized Solution
Visual Anchor: Dimensional Reduction
Point P(β,0,β)⟹y=0
Line L:1x−1=0y−0=−1z+1⟹y=0
The problem lies entirely in the XZ-plane.
Logic Bridge: Line Equation in 2D
1x−1=−1z+1
−1(x−1)=1(z+1)
−x+1=z+1
Line L:x+z=0
Visual Anchor: Plotting the Point
Line L is z=−x
Point P is (β,β) in XZ-plane
P lies on the line z=x
Logic Bridge: The Perpendicularity Catch
Slope of L (z=−x) is −1
Slope of line z=x is 1
Product of slopes =−1⟹ Lines are perpendicular
Foot of perpendicular is the origin (0,0)
Raw Setup: Distance Formula
Distance d is from (0,0) to (β,β)
d=(β−0)2+(β−0)2
Atomic Compute: Simplifying Distance
d=β2+β2
d=2β2
d=2∣β∣
Raw Setup: Equating to Given Value
Given distance d=23
2∣β∣=23
Atomic Compute: Squaring Both Sides
Squaring both sides:
(2∣β∣)2=(23)2
2β2=23
The Way Forward: Final Answer
β2=43
β=±23
(Mathematically correct value based on given text)
00:00 / 00:00
The Sigma Insight: Equation of a Line in Space
Solution Diagram
The Illusion of 3D Complexity
Welcome, future engineer! Today, we are going to dismantle a problem that, at first glance, looks like a daunting 3D geometry nightmare.
You see a point (β,0,β) and a line in 3D space, and your brain immediately starts reaching for complex vector projection formulas. But stop! Take a deep breath.
The secret to mastering JEE Advanced is not just knowing formulas; it is knowing when to look for the hidden simplicity. Let us embark on this journey together.
Phase 1
Dimensional Reduction
Look closely at the point P(β,0,β). Its y-coordinate is 0.
Now, look at the line equation:
1x−1=0y−0=−1z+1
The presence of the 0 in the denominator for the y-term tells us that for any point on this line, y must be 0. This is our 'Aha!' moment.
The point P and the entire line L exist exclusively in the XZ-plane. We have just collapsed a 3D problem into a 2D one. We are no longer lost in space; we are just drawing on a flat sheet of paper.
Phase 2
The Geometry of the Line
Now that we are in the XZ-plane, let us define our line L. We take the x and z parts of the equation:
1x−1=−1z+1
Cross-multiplying gives us −1(x−1)=1(z+1), which simplifies to −x+1=z+1.
Rearranging this, we get the beautiful, elegant equation: x+z=0, or simply z=−x. This line passes perfectly through the origin (0,0) with a slope of −1.
Phase 3
The Perpendicularity Catch
Where is our point P? In our XZ-plane, it is at (β,β).
Now, consider the line segment connecting the origin (0,0) to P(β,β). The slope of this segment is:
m=β−0β−0=1
Look at that! The slope of our line L is −1, and the slope of the segment from the origin to P is 1.
Since (−1)×1=−1, these two lines are perfectly perpendicular. This means the foot of the perpendicular from P to L is simply the origin (0,0). The geometry has aligned perfectly for us.
Phase 4
The Final Calculation
We are now at the finish line. We need the perpendicular distance from P(β,β) to the line L.
Since the foot of the perpendicular is the origin, this is just the distance from (0,0) to (β,β). Using the distance formula:
d=(β−0)2+(β−0)2=2β2=2∣β∣
The problem states this distance is 23. So, we set up our final equation:
2∣β∣=23
Squaring both sides, we get 2β2=23, which leads to β2=43.
Thus, β=±23. You have navigated the 3D trap and found the truth through 2D clarity. Keep this mindset, and no problem will ever be too complex for you!