Animated Solution for Mathematics - Three Dimensional Geometry: Let (α,β,γ) be the image of the point (8,5,7) in the line 2x−1=3y+1=5z−2. Then α+β+γ is equal to :
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Visualized Solution
Visualizing the Setup
Given point A(8,5,7)
Line equation: 2x−1=3y+1=5z−2
Goal: Find image A′(α,β,γ)
Defining a General Point M
Let 2x−1=3y+1=5z−2=λ
General point M on the line:
M=(2λ+1,3λ−1,5λ+2)
Constructing Vector AM
Vector AM=(xM−xA,yM−yA,zM−zA)
AM=(2λ+1−8,3λ−1−5,5λ+2−7)
AM=(2λ−7,3λ−6,5λ−5)
The Perpendicularity Condition
Direction vector of line d=(2,3,5)
Condition: AM⋅d=0
Setting up the Dot Product
AM=(2λ−7,3λ−6,5λ−5)
d=(2,3,5)
(2λ−7)(2)+(3λ−6)(3)+(5λ−5)(5)=0
Solving for λ
4λ−14+9λ−18+25λ−25=0
38λ−57=0
λ=3857=23
Finding the Coordinates of M
xM=2(23)+1=4
yM=3(23)−1=27
zM=5(23)+2=219
M=(4,27,219)
The Midpoint Property
M is the midpoint of A and A′
2α+8=4
2β+5=27
2γ+7=219
Calculating Image Coordinates
α+8=8⟹α=0
β+5=7⟹β=2
γ+7=19⟹γ=12
Image A′=(0,2,12)
Final Summation
Calculate α+β+γ
Sum =0+2+12=14
Final Answer: 14
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The Sigma Insight: Equation of a Line in Space
Solution Diagram
The Mirror in 3D Space
A Geometric Journey
Imagine you are standing in a room, and before you lies a mirror. But this is not a flat, two-dimensional mirror; this is a mirror that exists as a line in three-dimensional space.
You have a point A(8,5,7) floating in this space, and your goal is to find its reflection, A′(α,β,γ), on the other side of this line. This is the essence of 3D geometry—a beautiful, logical dance of vectors and parameters.
Phase 1
The Parametric Leap
To find the reflection, we first need to find the point where the perpendicular from A hits the line. Let's call this point M, the foot of the perpendicular.
The line is given by the equation:
2x−1=3y+1=5z−2
In 3D geometry, we love parameters. By setting this entire expression equal to a variable λ, we can describe any point on this line as a function of λ.
Thus, M becomes (2λ+1,3λ−1,5λ+2). This is our anchor, allowing us to represent an infinite number of points on the line with just one variable.
Phase 2
The Perpendicularity Dance
Now, we need to find the specific λ that places M exactly where the perpendicular from A lands. We construct the vector AM by subtracting the coordinates of A from M:
AM=(2λ+1−8,3λ−1−5,5λ+2−7)=(2λ−7,3λ−6,5λ−5)
Here is the magic: the vector AM is perpendicular to the line. The direction vector of our line, d, is simply the denominators of the line equation: (2,3,5).
Because AM is perpendicular to the line, their dot product must be zero:
AM⋅d=0
(2λ−7)(2)+(3λ−6)(3)+(5λ−5)(5)=0
Solving this, we get:
4λ−14+9λ−18+25λ−25=0
38λ−57=0
λ=3857=23
Phase 3
The Midpoint Bridge
With λ=23, we can find the exact coordinates of M:
xM=2(23)+1=4
yM=3(23)−1=27
zM=5(23)+2=219
So, M=(4,27,219). Now, the final step: the mirror line bisects the segment AA′. This means M is the midpoint of A and A′.
Using the midpoint formula, 2A+A′=M, we solve for A′(α,β,γ):
For the x-coordinate: 2α+8=4⇒α=0.
For the y-coordinate: 2β+5=27⇒β=2.
For the z-coordinate: 2γ+7=219⇒γ=12.
Conclusion
The Final Sum
We have found the image A′(0,2,12). The question asks for the sum α+β+γ.
Adding them up, 0+2+12=14.
The final result is 14. It is a simple, elegant conclusion to a journey through 3D space. Remember, geometry is not just about formulas; it is about visualizing the relationship between points, lines, and the space they inhabit.