Animated Solution for Mathematics - Three Dimensional Geometry: If the image of the point P(1,0,3) in the line joining the points A(4,7,1) and B(3,5,3) is Q(α,β,γ), then α+β+γ is equal to
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Visualized Solution
Visualizing the Geometry
Given point P(1,0,3).
Line passes through A(4,7,1) and B(3,5,3).
Let Q(α,β,γ) be the image of P in line AB.
Direction Ratios of Line AB
Direction Ratios (DRs) of line AB=(xA−xB,yA−yB,zA−zB)
DRs of line AB=(4−3,7−5,1−3)
DRs of line AB=(1,2,−2)
Equation of Line AB
Equation of line AB: 1x−3=2y−5=−2z−3=λ
General Point R on the Line
Coordinates of a general point R on the line:
x=λ+3
y=2λ+5
z=−2λ+3
R=(λ+3,2λ+5,−2λ+3)
Vector PR Calculation
Vector PR=(xR−xP,yR−yP,zR−zP)
PR=((λ+3)−1,(2λ+5)−0,(−2λ+3)−3)
PR=(λ+2,2λ+5,−2λ)
Condition for Perpendicularity
Since PR⊥AB, their dot product is zero.
PR⋅dAB=0
(λ+2)(1)+(2λ+5)(2)+(−2λ)(−2)=0
Solving for λ - Expansion
Expand the dot product equation:
(λ+2)+(4λ+10)+4λ=0
Solving for λ - Final Value
Combine like terms:
9λ+12=0
9λ=−12
λ=−912=−34
Coordinates of Foot R
Substitute λ=−34 into R:
xR=−34+3=35
yR=2(−34)+5=37
zR=−2(−34)+3=317
R=(35,37,317)
Finding the Image Q
R is the midpoint of PQ⇒R=2P+Q
Q=2R−P
α=2(35)−1=37
β=2(37)−0=314
γ=2(317)−3=325
Final Sum α+β+γ
Sum =α+β+γ
Sum =37+314+325
Sum =37+14+25=346
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The Sigma Insight: Equation of a Line in Space
Solution Diagram
Analyzing the Setup
Imagine you are standing in a vast, three-dimensional void. You have a point P(1,0,3) floating in space, and a line AB defined by the points A(4,7,1) and B(3,5,3).
You are tasked with finding the 'image' of P in this line. Think of this line as a mirror. If you were to look into this mirror, where would the reflection Q(α,β,γ) appear?
Defining the Mirror
Before we can find the reflection, we must understand the mirror itself. A line in 3D space is defined by a point and a direction.
The direction ratios of our line are the differences in the coordinates of A and B:
d=(4−3,7−5,1−3)=(1,2,−2)
This vector acts as the compass for our line. We can now write the equation of the line in its symmetric form:
1x−3=2y−5=−2z−3=λ
This parameter λ is our key. It allows us to represent any point R on the line as a function of a single variable:
R=(λ+3,2λ+5,−2λ+3)
The Perpendicular Connection
The line segment connecting the original point P to its image Q must be perpendicular to the mirror line AB. Furthermore, the point of intersection R must be the midpoint of PQ.
To find R, we look for the specific value of λ that makes the vector PR perpendicular to the line's direction vector d. We calculate PR=R−P:
PR=((λ+3)−1,(2λ+5)−0,(−2λ+3)−3)=(λ+2,2λ+5,−2λ)
For PR to be perpendicular to the line, their dot product must vanish:
PR⋅d=0
Substituting our values, we get:
(λ+2)(1)+(2λ+5)(2)+(−2λ)(−2)=0
Expanding this, we find:
λ+2+4λ+10+4λ=0
This simplifies to 9λ+12=0, which yields the parameter:
λ=−34
The Final Symmetry
With λ=−34, we locate the foot of the perpendicular R: