Animated Solution for Mathematics - Three Dimensional Geometry: Let the image of the point (1,0,7) in the line 1x=2y−1=3z−2 be the point (α,β,γ). Then which one of the following points lies on the line passing through (α,β,γ) and making angles 32π and 43π with y-axis and z-axis respectively and an acute angle with x-axis ?
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Visualized Solution
Visualizing the Setup
Given point P(1,0,7).
Line L1:1x=2y−1=3z−2.
We need to find the image Q(α,β,γ) of point P in line L1.
The Foot of the Perpendicular
Let M be the foot of the perpendicular from P to L1.
Line L2 passes through Q(1,6,3) with direction cosines (21,−21,−21).
Equation of L2: 21x−1=−21y−6=−21z−3=μ.
Parametric form: x=1+2μ, y=6−2μ, z=3−2μ.
Verifying the Options
Let's test the options. Notice the x-coordinates in the options are 1 or 3.
If x=3, then 1+2μ=3⟹2μ=2⟹μ=4.
Substitute μ=4 into y and z:
y=6−24=6−2=4.
z=3−24=3−22.
The point is (3,4,3−22).
Final Conclusion
The point (3,4,3−22) lies on the required line.
This matches Option 3.
Key Concept: Image of a point involves finding the foot of the perpendicular and using the midpoint formula.
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The Sigma Insight: Equation of a Line in Space
Solution Diagram
Analyzing the Setup
Welcome, fellow explorer of the mathematical universe! Today, we are diving into the elegant world of 3D geometry. Imagine you are standing in a room, and there is a line suspended in the air.
You have a point, a specific coordinate in space, and you want to see its reflection—its image—as if that line were a mirror. This is exactly what we are tackling today. It is not just about crunching numbers; it is about visualizing the symmetry of space.
Finding the Foot of the Perpendicular
We start with point P(1,0,7) and the line L1 defined by:
1x=2y−1=3z−2
To find the image Q(α,β,γ), we need a bridge. That bridge is the foot of the perpendicular, M. Think of M as the point on the line closest to P.
Because M lies on the line, we can describe it using a single parameter, λ. By setting the line equations equal to λ, we get the general coordinates of M as (λ,1+2λ,2+3λ).
Now, we invoke the power of vectors. The vector PM connects our original point to this mystery point M. Since M is the foot of the perpendicular, PM must be perpendicular to the line itself.
The direction vector of our line is d=(1,2,3). The condition for perpendicularity is simple yet profound: the dot product PM⋅d must be zero.
Calculating PM=(λ−1,1+2λ,3λ−5), we set up the equation:
1(λ−1)+2(1+2λ)+3(3λ−5)=0
Solving this, we find λ=1. Substituting this back, we find M=(1,3,5).
The Image Revealed
With M found, the image Q is just a step away. Since M is the midpoint of PQ, we use the relation Q=2M−P.
Plugging in our coordinates, we get:
Q=(2(1)−1,2(3)−0,2(5)−7)
This simplifies to Q(1,6,3). We have successfully reflected our point!
The New Path
Now, the problem shifts. We have a new line L2 passing through Q(1,6,3). We are given the angles it makes with the axes: 32π with the y-axis and 43π with the z-axis.
We need the direction cosines l,m,n. We know:
m=cos(32π)=−21
n=cos(43π)=−21
The fundamental identity l2+m2+n2=1 is our best friend here. Substituting our values, we get:
l2+41+21=1⇒l2=41
The problem tells us the line makes an acute angle with the x-axis, so l must be positive. Thus, l=21.
The Final Verification
The equation of our new line L2 is:
1/2x−1=−1/2y−6=−1/2z−3=μ
By testing the options, we find that for the point (3,4,3−22), the parameter μ is consistent across all coordinates. We have arrived!
The beauty of this problem lies in how it weaves together reflection, vector orthogonality, and the properties of direction cosines. Keep practicing, and soon, these 3D structures will feel as natural as walking in your own home.