Animated Solution for Mathematics - Three Dimensional Geometry: The foot of the perpendicular from a point on the circle x2+y2=1,z=0 to the plane 2x+3y+z=6 lies on which one of the following curves ?
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Visualized Solution
The Setup: Circle and Point P
Circle equation: x2+y2=1 in the xy-plane (z=0).
Any point P on this circle can be written parametrically.
P=(cosθ,sinθ,0)
The Plane and Foot of Perpendicular
Plane equation: 2x+3y+z=6
Normal vector direction ratios: (2,3,1)
Let Q(x,y,z) be the foot of the perpendicular from P to the plane.
Foot of Perpendicular Formula
The line PQ is parallel to the normal vector of the plane.
Equation of line PQ: ax−x1=by−y1=cz−z1=k
Substituting the Coordinates
Substitute P(cosθ,sinθ,0) and normal (2,3,1):
2x−cosθ=3y−sinθ=1z−0=k
Finding the Constant k
Look at the z-component:
1z−0=k⟹k=z
So, 2x−cosθ=z and 3y−sinθ=z
Isolating cosθ
From 2x−cosθ=z:
x−cosθ=2z
cosθ=x−2z
Isolating sinθ
From 3y−sinθ=z:
y−sinθ=3z
sinθ=y−3z
Eliminating θ
We know the fundamental identity: cos2θ+sin2θ=1
Substitute our expressions:
(x−2z)2+(y−3z)2=1
The Role of the Plane
The point Q(x,y,z) lies on the plane 2x+3y+z=6.
We can express z in terms of x and y:
z=6−2x−3y
Substituting z into the First Term
We need to evaluate (x−2z):
x−2(6−2x−3y)
=x−12+4x+6y
=5x+6y−12
Substituting z into the Second Term
Now evaluate (y−3z):
y−3(6−2x−3y)
=y−18+6x+9y
=6x+10y−18
=2(3x+5y−9)
Final Locus Equation
Substitute these back into (x−2z)2+(y−3z)2=1:
(5x+6y−12)2+[2(3x+5y−9)]2=1
(5x+6y−12)2+4(3x+5y−9)2=1
This is our required curve, matching Option 2.
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The Sigma Insight: Intersection of a Line and a Plane
Solution Diagram
The Geometry of Projection
A Journey into 3D Space
Imagine you are standing in a vast, empty room. On the floor, there is a perfect unit circle, x2+y2=1, resting silently in the xy-plane where z=0.
Now, imagine a tilted plane hovering above this circle, defined by the equation 2x+3y+z=6. You are tasked with finding the path traced by the foot of the perpendicular dropped from every point on that circle onto the plane.
This is not just a math problem; it is a study of how shapes transform when projected into different dimensions.
Phase 1
The Parametric Dance
To begin, we must capture the essence of our circle. A point P moving along the unit circle can be described elegantly using trigonometry.
We define P as (cosθ,sinθ,0). As θ sweeps from 0 to 2π, P traces the entire circle. This parametric representation is our starting point, our anchor in the xy-plane.
Phase 2
The Normal Vector Bridge
Now, consider the plane 2x+3y+z=6. The coefficients of x,y, and z give us the normal vector to the plane: n=(2,3,1).
When we drop a perpendicular from P to the plane, the resulting line segment PQ is inherently parallel to this normal vector. This is the geometric secret that unlocks the problem.
The line PQ passing through P(cosθ,sinθ,0) with direction ratios (2,3,1) can be written in symmetric form:
2x−cosθ=3y−sinθ=1z−0=k
Here, k is our constant of proportionality. It acts as a scalar that scales the normal vector to reach from P to Q.
Phase 3
The Algebraic Bridge
Look closely at the third ratio: 1z=k. This is a gift! It tells us that k=z.
Now, we can rewrite the first two ratios using z instead of k:
2x−cosθ=z⟹cosθ=x−2z
3y−sinθ=z⟹sinθ=y−3z
We have successfully expressed the circle's parameter θ in terms of the coordinates of the foot of the perpendicular Q(x,y,z).
Phase 4
The Final Constraint
We know that cos2θ+sin2θ=1. Substituting our expressions, we get:
(x−2z)2+(y−3z)2=1
This equation describes a cylinder in 3D space. But our point Q is not just anywhere; it is constrained to the plane 2x+3y+z=6.
We can solve for z: z=6−2x−3y. Now, we substitute this into our cylinder equation.
Let's handle the terms one by one. First, (x−2z) becomes x−2(6−2x−3y)=5x+6y−12.
Next, (y−3z) becomes y−3(6−2x−3y)=6x+10y−18, which simplifies to 2(3x+5y−9).
The Elegant Conclusion
Putting it all together, our final locus equation is:
(5x+6y−12)2+[2(3x+5y−9)]2=1
(5x+6y−12)2+4(3x+5y−9)2=1
This is the curve traced by the foot of the perpendicular. It is a beautiful, precise result that perfectly matches the second option.
You have just navigated the projection of a circle onto a tilted plane, turning a complex 3D visualization into a concrete algebraic reality. Keep this intuition, and no geometry problem will ever be too daunting again!