Animated Solution for Mathematics - Three Dimensional Geometry: Let A be a point on the line r=(1−3μ)i^+(μ−1)j^+(2+5μ)k^ and B(3, 2, 6) be a point in the space. Then the value of μ for which the vector AB is parallel to the plane x−4y+3z=1 is :
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Visualized Solution
Visualizing the Geometry
Given plane: x−4y+3z=1
Point A lies on the given line.
Point B is fixed at (3,2,6).
Coordinates of Point A
The line equation is r=(1−3μ)i^+(μ−1)j^+(2+5μ)k^
Any point on this line has coordinates:
A≡(1−3μ,μ−1,2+5μ)
Constructing Vector AB
Position vector of AB=B−A
AB=(3−(1−3μ))i^+(2−(μ−1))j^+(6−(2+5μ))k^
Simplifying Vector AB
x-component: 3−1+3μ=2+3μ
y-component: 2−μ+1=3−μ
z-component: 6−2−5μ=4−5μ
AB=(2+3μ)i^+(3−μ)j^+(4−5μ)k^
The Normal Vector
Plane equation: 1x−4y+3z=1
The coefficients of x,y,z give the normal vector n.
n=i^−4j^+3k^
Condition for Parallelism
We want vector AB to be parallel to the plane.
If a line is parallel to a plane, it must be perpendicular to the plane's normal vector.
Therefore, AB⊥n
Setting up the Dot Product
For perpendicular vectors, their dot product is zero: AB⋅n=0
(2+3μ)(1)+(3−μ)(−4)+(4−5μ)(3)=0
Expanding the Equation
Multiply the terms:
(2+3μ)−12+4μ+12−15μ=0
Solving for μ
Group the μ terms: 3μ+4μ−15μ=−8μ
Group the constants: 2−12+12=2
−8μ+2=0
Final Conclusion
8μ=2
μ=82=41
The value of μ is 41.
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The Sigma Insight: Intersection of a Line and a Plane
Solution Diagram
Analyzing the Setup
Imagine you are standing in a vast 3D coordinate system. You have a fixed point B at (3,2,6) and a line defined by the parameter μ, where a point A is sliding along.
We want to find the exact moment when the vector AB is perfectly parallel to the plane x−4y+3z=1. This is not just algebra; it is a dance of vectors in space.
Pinning Down Point A
First, we must define our moving target. The line equation is given as r=(1−3μ)i^+(μ−1)j^+(2+5μ)k^.
This means any point A on this line has coordinates A≡(1−3μ,μ−1,2+5μ). Think of μ as time; as μ changes, A traces out the line.
Constructing the Vector AB
Now, we define the vector AB by finding the difference between the position vectors of B and A. This is AB=B−A.
Substituting our coordinates, we get:
AB=(3−(1−3μ))i^+(2−(μ−1))j^+(6−(2+5μ))k^
Simplifying this, we find:
AB=(2+3μ)i^+(3−μ)j^+(4−5μ)k^
This vector represents the displacement from our moving point A to our fixed destination B.
The Geometric Insight
Here is the core of the problem. A vector is parallel to a plane if and only if it is perpendicular to the plane's normal vector.
The plane x−4y+3z=1 has a normal vector n=1i^−4j^+3k^. If AB is parallel to the plane, then AB⊥n.
In the language of vectors, this means their dot product must be zero:
AB⋅n=0
The Final Calculation
Let us perform the dot product:
(2+3μ)(1)+(3−μ)(−4)+(4−5μ)(3)=0
Expanding this, we get:
(2+3μ)−12+4μ+12−15μ=0
Combining the terms, we have (3μ+4μ−15μ)+(2−12+12)=0, which simplifies to:
−8μ+2=0
Solving for μ, we find 8μ=2, or:
μ=41
This is the magic value! At μ=41, the vector AB aligns perfectly to be parallel to the plane. You have successfully navigated the 3D space and solved the puzzle.