Animated Solution for Mathematics - Three Dimensional Geometry: The lines x=ay−1=z−2 and x=3y−2=bz−2,(ab=0) are coplanar, if :
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Visualized Solution
CoplanarLinesConcept
Two lines are coplanar if they lie in the same plane.
This implies they either intersect or are parallel, sharing the same 2D space.
ConditionforCoplanarity
The mathematical condition for coplanarity is [AB,d1,d2]=0.
This means the scalar triple product of the connecting vector and the two direction vectors is zero.
StandardizingL1
Line L1:x=ay−1=z−2
Rewrite as: 1x−0=1a(y−a1)=1z−2
Standard Form: 1x−0=a1y−a1=1z−2
Point A=(0,a1,2), Direction d1=(1,a1,1)
StandardizingL2
Line L2:x=3y−2=bz−2
Standard Form: 1x−0=31y−32=b1z−b2
Point B=(0,32,b2), Direction d2=(1,31,b1)
ConnectingtheLines
Vector AB=B−A
AB=(0−0,32−a1,b2−2)
TheDeterminantEquation
Condition: 01132−a1a131b2−21b1=0
ExpandingalongRow1
Expand along Row 1:
0−(32−a1)(b1−1)+(b2−2)(31−a1)=0
ExtractingCommonFactors
Factor out (b1−1):
(b1−1)[−(32−a1)+2(31−a1)]=0
SimplifyingtheInnerTerms
Simplify inside the bracket:
(b1−1)[−32+a1+32−a2]=0
(b1−1)(−a1)=0
Findingaandb
Since a=0, −a1=0
Therefore, b1−1=0⟹b=1
Final Condition: b=1,a∈R−{0}
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The Sigma Insight: Equation of a Line in Space
Solution Diagram
The Dance of Coplanar Lines
A Journey into 3D Geometry
Imagine you are standing in a vast, empty room. You have two thin, straight wires suspended in the air. The question is simple: can you place a single, flat sheet of paper such that both wires lie entirely on it?
This is the essence of the concept of coplanar lines. In the world of JEE Advanced, this isn't just a visualization exercise; it is a rigorous test of your ability to translate geometric intuition into algebraic precision.
Phase 1
The Trap of Non-Standard Forms
Before we can perform any calculations, we must respect the language of 3D geometry. The equations provided, x=ay−1=z−2 and x=3y−2=bz−2, are not in their standard symmetric form.
A common mistake is to blindly grab the coefficients of y and z and call them the direction ratios. The standard form is:
lx−x1=my−y1=nz−z1
where the coefficients of x,y, and z are all 1.
For L1, we rewrite x=ay−1=z−2 as:
1x−0=a1y−a1=1z−2
Now, the truth is revealed: our point A is (0,a1,2) and our direction vector d1 is (1,a1,1).
We perform the same surgery on L2, yielding point B=(0,32,b2) and direction vector d2=(1,31,b1). By standardizing, we have stripped away the confusion and exposed the core geometry.
Phase 2
The Geometry of Coplanarity
Now, how do we force these lines to share a plane? We connect them with a vector AB=B−A.
If AB, d1, and d2 all lie on the same plane, they cannot form a 3D volume. Mathematically, this means their scalar triple product must vanish:
[AB,d1,d2]=0
This is the moment where geometry meets algebra. We construct our determinant:
01132−a1a131b2−21b1=0
Notice that beautiful zero in the top-left corner? That is a gift from the problem setter. It simplifies our expansion significantly, allowing us to focus on the remaining terms without getting lost in a sea of arithmetic.
Phase 3
The Algebraic Dance
Let us expand along the first row. We have:
0−(32−a1)(b1−1)+(b2−2)(31−a1)=0
This looks intimidating, but stay calm. Look for common factors. We can rewrite b2−2 as 2(b1−1).
Suddenly, the term (b1−1) appears in both parts of the equation! We factor it out:
(b1−1)[−(32−a1)+2(31−a1)]=0
Now, simplify the expression inside the square brackets. Distributing the negative sign and the 2 gives us −32+a1+32−a2.
The constants −32 and +32 cancel out perfectly, leaving us with −a1. Our equation reduces to the elegant form:
(b1−1)(−a1)=0
Since the problem guarantees $a
eq 0$, we know that −a1 cannot be zero. Therefore, the only way for this product to be zero is if b1−1=0, which implies b=1.
And just like that, the complexity dissolves. We have found our condition: b=1, with a being any non-zero real number. You have successfully navigated the 3D space and tamed the algebra. Well done!