Animated Solution for Mathematics - Three Dimensional Geometry: If the line, 2x−3=−1y+2=3z+4 lies in the plane, lx+my−z=9, then l2+m2 is equal to :
Select Answer:
Visualized Solution
Visualizing the Setup
Given Line: 2x−3=−1y+2=3z+4
Given Plane: lx+my−z=9
The line lies completely inside the plane.
Point on the Line
Standard line equation: ax−x1=by−y1=cz−z1
Comparing, we get a point on the line: P(3,−2,−4)
Satisfying the Plane Equation
Since P(3,−2,−4) lies on the plane lx+my−z=9:
Substitute x=3, y=−2, z=−4
l(3)+m(−2)−(−4)=9
Forming Equation (i)
3l−2m+4=9
3l−2m=5…(i)
Vectors of Line and Plane
Line's direction vector: b=2i^−j^+3k^
Plane's normal vector: n=li^+mj^−k^
Orthogonality Condition
Since the line lies in the plane, b⊥n
Therefore, their dot product is zero: b⋅n=0
Calculating the Dot Product
b⋅n=(2)(l)+(−1)(m)+(3)(−1)=0
Forming Equation (ii)
2l−m−3=0
2l−m=3…(ii)
Solving for l and m
From (ii): m=2l−3
Substitute into (i): 3l−2(2l−3)=5
Calculating l
3l−4l+6=5
−l=5−6=−1
l=1
Calculating m
Substitute l=1 into m=2l−3
m=2(1)−3
m=−1
Finding l2+m2
We need to find l2+m2
(1)2+(−1)2
1+1=2
00:00 / 00:00
The Sigma Insight: Intersection of a Line and a Plane
Solution Diagram
Analyzing the Setup
Imagine you are standing in a vast, empty room. You have a thin, perfectly straight laser beam (our line) and a massive, flat sheet of glass (our plane). The problem asks us to consider a scenario where this laser beam is not just passing through the glass, but is resting perfectly flush against its surface.
This is the essence of the condition: the line lies in the plane.
The Anchor Point
Every line in 3D space is defined by a direction and a starting point. Looking at our line equation,
2x−3=−1y+2=3z+4
we can immediately extract a point that the line passes through. By setting the ratios to zero, we find the anchor point P(3,−2,−4).
If the entire line is contained within the plane lx+my−z=9, then this point P must also be a point on the plane. It must satisfy the plane's equation. Substituting our coordinates, we get:
l(3)+m(−2)−(−4)=9
Simplifying this, we arrive at our first vital constraint: 3l−2m=5. This is our first anchor equation. We have successfully locked down one relationship between the variables l and m.
The Orthogonality of Directions
Now, let's think about the orientation. A plane is defined by its 'normal'—a vector n that points straight out from its surface. For our plane lx+my−z=9, the normal vector is n=li^+mj^−1k^.
Meanwhile, our line has a direction vector b=2i^−1j^+3k^. If the line is lying flat on the plane, it must be perpendicular to the normal vector. In the language of vectors, this means their dot product must vanish:
b⋅n=0
Calculating this, we get (2)(l)+(−1)(m)+(3)(−1)=0, which simplifies beautifully to 2l−m=3. This is our second constraint. We have now captured the 'soul' of the geometry in two simple algebraic equations.
The Elegant Resolution
We are left with a system of two linear equations:
1) 3l−2m=5
2) 2l−m=3
From the second equation, we can easily see that m=2l−3. Substituting this into the first equation, we get:
3l−2(2l−3)=5
Expanding this, we find 3l−4l+6=5, which leads us to −l=−1, or simply l=1. With l in hand, finding m is a breeze: m=2(1)−3=−1.
Final Calculation
We have found our variables! The final step is to calculate l2+m2. Plugging in our values, we get: