Q.The two lines π₯β1 3 = βπ¦ , π§ + 1 = 0 and βπ₯ 2 = π¦+1 2 = π§ + 2 intersect at a point whose y-coordinate is 1. Find the co-ordinates of their point of intersection. Find the vector equation of a line perpendicular to both the given lines and passing through this point of intersection. 5
CBSESample paperLongΒ· 5mImportanceβ β β β β est
β Free question
Concept understanding β Mutual Perpendicularity
Perpendicular Vectors: The Dot-Product Test
Two vectors are perpendicular (orthogonal) when they meet at a right angle β like the east and north directions. But you cannot reach for a protractor in 3D, so you need an algebraic test.
The key idea: when two vectors are perpendicular, neither has any "shadow" along the other. Walk along one and you make zero progress in the direction of the other. The dot product measures exactly this overlap, so perpendicularity means the dot product vanishes.
When ΞΈ=90β, cos90β=0, so the product is zero regardless of the vectors' lengths.
Example. For a=(1,2,3) and b=(2,β1,0):
aβ b=1(2)+2(β1)+3(0)=0,
so they are perpendicular. By contrast (2,1)β (1,3)=2+3=5ξ =0, so those two are not.
Tip
In 2D, (x,y) and (y,βx) are always perpendicular β swap and negate. To build a vector perpendicular to a given a, solve aβ x=0; there are infinitely many solutions, all lying in the plane across a.
Where it shows up: proving two lines or planes meet at right angles, showing the work done by a force perpendicular to displacement is zero (W=Fβ d=0), and classic results like "the diagonals of a rhombus are perpendicular." Whenever you read "perpendicular" or "orthogonal," reach for dot product =0.
This dot-product test for perpendicular vectors is the same foundational NCERT Class 12 Vector Algebra result behind countless CBSE board and JEE Main questions on right angles in 3D. Searches like "how to check if two vectors are perpendicular" consistently lead back to this single condition, which also explains why a force perpendicular to displacement does zero work in Physics.
Concept: Mutual Perpendicularity β a line perpendicular to two given lines is parallel to the cross product of their direction vectors.
Step 1: Write both lines in symmetric form.
First line: 3xβ1β=β1yβ=0z+1β (since z+1=0 means z=β1 constant).
Direction vector: d1ββ=(3,β1,0).
Second line: 2βxβ=2y+1β=z+2 β rewrite as β2xβ=2y+1β=1z+2β.
Direction vector: d2ββ=(β2,2,1).
Step 2: Find intersection point with y=1.
From first line: y=βt, so 1=βtβt=β1. Then x=1+3t=1β3=β2, z=β1.
Check second line: for t=β1, β2xβ=β1βx=2 (mismatch). So use second line: let parameter s.
From second line: y+1=2s, so 1+1=2sβs=1. Then x=β2s=β2, z+2=sβz=β1.
The point of intersection is (β2,1,β1) and the required line is r=(β2,1,β1)+Ξ»(β1,β3,4).
The lines meet at (β2,1,β1); a line perpendicular to both has direction d1βΓd2β=βi^β3j^β+4k^, giving r=(β2i^+j^ββk^)+Ξ»(βi^β3j^β+4k^).
Line 1:3xβ1β=βy,Β z=β1. Direction d1β=(3,β1,0).
Parameterise: x=3t+1,Β y=βt,Β z=β1. With y=1βt=β1βx=β2,Β z=β1.
Line 2:β2xβ=2y+1β=1z+2β. Direction d2β=(β2,2,1).
Parameterise: x=β2s,Β y=2sβ1,Β z=sβ2. With y=1βs=1βx=β2,Β z=β1.
Both parameterisations give the same point, so the point of intersection is P(β2,1,β1).