Animated Solution for Mathematics - Three Dimensional Geometry: If the straight lines 2x−1=ky+1=2z and 5x+1=2y+1=kz are coplanar, then the plane(s) containing these two lines is (are)
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Visualized Solution
Extracting Points from Lines
Line L1:2x−1=ky+1=2z
Line L2:5x+1=2y+1=kz
Point on L1: A(1,−1,0)
Point on L2: B(−1,−1,0)
Identifying Direction Vectors
Direction of L1: d1=2i^+kj^+2k^
Direction of L2: d2=5i^+2j^+kk^
Connecting the Points
Vector connecting A and B: AB=B−A
AB=(−1−1)i^+(−1−(−1))j^+(0−0)k^
AB=−2i^+0j^+0k^
Condition for Coplanarity
Three vectors AB, d1, and d2 must be coplanar.
Their scalar triple product must be zero: [ABd1d2]=0
This is equivalent to the determinant being zero.
Setting up the Determinant
−2250k202k=0
Expanding the Determinant
Expanding along the first row:
−2⋅(k⋅k−2⋅2)−0+0=0
−2(k2−4)=0
Solving for k
−2(k2−4)=0
k2−4=0
k2=4
k=2 or k=−2
Case 1: When k=2
Let's analyze the first case where k=2.
Substitute k=2 into direction vectors:
d1=2i^+2j^+2k^
d2=5i^+2j^+2k^
Finding the Normal Vector n1
The normal vector n1 is perpendicular to both d1 and d2.
n1=d1×d2=i^25j^22k^22
n1=i^(4−4)−j^(4−10)+k^(4−10)
n1=0i^+6j^−6k^
Simplifying the Normal Vector
n1=6(0i^+1j^−1k^)
For the plane equation, we can use the simpler parallel vector:
n1,simplified=0i^+1j^−1k^
Equation of Plane 1
Using point A(1,−1,0) and normal n=(0,1,−1)
Formula: a(x−x1)+b(y−y1)+c(z−z1)=0
0(x−1)+1(y−(−1))−1(z−0)=0
y+1−z=0⇒y−z=−1
Case 2: When k=−2
Now let's analyze the second case where k=−2.
Substitute k=−2 into direction vectors:
d1=2i^−2j^+2k^
d2=5i^+2j^−2k^
Finding the Normal Vector n2
n2=d1×d2=i^25j^−22k^2−2
n2=i^(4−4)−j^(−4−10)+k^(4−(−10))
n2=0i^+14j^+14k^
Simplified normal: n2,simplified=0i^+1j^+1k^
Equation of Plane 2
Using point A(1,−1,0) and normal n=(0,1,1)
0(x−1)+1(y−(−1))+1(z−0)=0
y+1+z=0⇒y+z=−1
Final Conclusion
The two possible planes containing the lines are:
1. y−z=−1
2. y+z=−1
Both options are correct depending on the value of k.
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The Sigma Insight: Equation of a Plane
Solution Diagram
The Geometry of Connection
A 3D Odyssey
My dear student, welcome to the fascinating world of 3D geometry. Today, we are not just solving a problem; we are exploring the architecture of space itself.
We have two lines, L1 and L2, floating in three-dimensional space. They seem independent, yet they are bound by the condition of being coplanar. This means they share a common home—a plane. Let us embark on this journey to find that home.
Phase 1
Extracting the DNA of the Lines
Every line in 3D space carries its own DNA: a point it passes through and a direction in which it travels. Look at the symmetric equations provided:
L1:2x−1=ky+1=2z
L2:5x+1=2y+1=kz
By inspecting the numerators, we can instantly extract a point from each line. For L1, we see the point A(1,−1,0). For L2, we find the point B(−1,−1,0). These are our anchors.
Next, we look at the denominators. These are the components of our direction vectors. For L1, the direction vector is d1=2i^+kj^+2k^. For L2, it is d2=5i^+2j^+kk^.
Notice how the mystery parameter k is woven into the very fabric of these directions. This is the variable we must unmask.
Phase 2
The Condition of Coplanarity
Imagine these two lines. To ensure they lie on the same plane, we need to connect them. Let us draw a vector AB from point A to point B.
We calculate this by subtracting the coordinates of A from B:
AB=(−1−1)i^+(−1−(−1))j^+(0−0)k^=−2i^
Now, here is the core geometric reality: if AB, d1, and d2 all lie on the same plane, the volume of the parallelepiped they form must be zero. This is the Scalar Triple Product.
We set the determinant of these three vectors to zero:
−2250k202k=0
Expanding this along the first row is our most efficient strategy. We get −2(k2−4)=0. This simplifies beautifully to k2=4, giving us two distinct possibilities: k=2 or k=−2.
Phase 3
Constructing the Planes
With k values in hand, we now have two distinct scenarios. Let us tackle Case 1: k=2.
Our direction vectors become d1=2i^+2j^+2k^ and d2=5i^+2j^+2k^. To find the plane, we need a normal vector n1, which is perpendicular to both lines.
We find this via the cross product n1=d1×d2. Calculating this, we get n1=0i^+6j^−6k^. We can simplify this to n=(0,1,−1).
Using point A(1,−1,0), the plane equation becomes 0(x−1)+1(y+1)−1(z−0)=0, which simplifies to y−z=−1.
Now, for Case 2: k=−2. Our direction vectors are d1=2i^−2j^+2k^ and d2=5i^+2j^−2k^.
Again, we find the normal vector n2=d1×d2, resulting in n2=0i^+14j^+14k^. Simplifying, we get n=(0,1,1).
Using point A(1,−1,0), the plane equation becomes 0(x−1)+1(y+1)+1(z−0)=0, leading to y+z=−1.
Conclusion
We have arrived! We found that the lines are coplanar for two specific values of k, resulting in two beautiful planes: y−z=−1 and y+z=−1.
This problem taught us that geometry is not just about shapes; it is about the relationships between vectors and the conditions that force them to align. Keep practicing, keep visualizing, and never lose your curiosity.