Animated Solution for Mathematics - Three Dimensional Geometry: The value of k such that 1x−4=1y−2=2z−k lies in the plane 2x−4y+z=7, is
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Visualized Solution
Visualizing the Line and Plane
Let's visualize a plane π and a line L.
The problem states that the line L lies completely inside the plane π.
Condition 1: The Point Lies on the Plane
If the entire line lies in the plane, then every point on the line must also lie on the plane.
Let's pick a specific point P on the line.
Condition 2: Orthogonality of Vectors
The line has a direction vector d.
The plane has a normal vector n which is perpendicular to the entire plane.
Therefore, n must be perpendicular to d.
Extracting Point P from the Line
The equation of the line is 1x−4=1y−2=2z−k.
Comparing with standard form ax−x1=by−y1=cz−z1, the point P(x1,y1,z1) is (4,2,k).
Extracting Vectors d and n
The direction vector of the line is d=i^+j^+2k^.
The equation of the plane is 2x−4y+z=7.
The normal vector of the plane is n=2i^−4j^+k^.
Checking d⋅n=0
Let's verify if the line is parallel to the plane by checking the dot product.
d⋅n=(1)(2)+(1)(−4)+(2)(1)
d⋅n=2−4+2=0.
The condition holds! The line is indeed parallel to (or lies in) the plane.
Substituting P into the Plane Equation
Since the line lies in the plane, the point P(4,2,k) must satisfy the plane's equation.
Plane equation: 2x−4y+z=7.
Substitute x=4, y=2, z=k:
2(4)−4(2)+(k)=7.
Solving the Linear Equation
Simplify the terms:
8−8+k=7.
The 8 and −8 cancel out.
k=7.
Final Conclusion
Final Answer:k=7.
This ensures the line is not just parallel to the plane, but physically embedded within it.
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The Sigma Insight: Intersection of a Line and a Plane
Solution Diagram
Analyzing the Setup
Imagine you are standing in a vast, three-dimensional space. You have a perfectly flat sheet of paper, which we call a plane, defined by the equation 2x−4y+z=7.
Now, imagine a thin, infinite wire, which we call a line, defined by the symmetric equations:
1x−4=1y−2=2z−k
The problem asks us to find the value of k that forces this wire to lie perfectly flat, embedded within that sheet of paper. This is not just an algebraic exercise; it is a beautiful dance of vectors and coordinates.
The Two Pillars of Containment
To solve this, we need to satisfy two fundamental geometric conditions. First, the line must be parallel to the plane. If the line is tilted even slightly, it will eventually pierce through the paper, and it cannot lie entirely within it.
Second, at least one point on that line must be touching the plane. If the line is parallel but hovering above or below the plane, it is not 'in' the plane. Together, these two conditions lock the line into place.
The Toolkit
Vectors
Let us extract the information we need. The line gives us a direction vector, d, which tells us where it is heading. Looking at the denominators of our symmetric equation, we see d=1i^+1j^+2k^.
The plane gives us a normal vector, n, which points directly away from its surface. From the coefficients of the plane equation 2x−4y+z=7, we identify n=2i^−4j^+1k^.
Now, for the first condition: parallelism. If the line is parallel to the plane, its direction vector d must be perpendicular to the plane's normal vector n.
We test this with the dot product:
d⋅n=(1)(2)+(1)(−4)+(2)(1)
Calculating this, we get 2−4+2=0. The dot product is zero! The vectors are orthogonal, and the line is indeed parallel to the plane. The geometry is sound.
The Final Execution
With parallelism confirmed, we move to the second pillar: point containment. We know that the point P(4,2,k) lies on our line.
If the entire line is to lie within the plane, this specific point P must also satisfy the plane's equation. We substitute the coordinates of P into the plane equation 2x−4y+z=7:
2(4)−4(2)+(k)=7
Let us perform the arithmetic with care. We have 8−8+k=7.
The 8 and −8 cancel out with elegant simplicity, leaving us with the final result: k=7. This is the magic of the problem—the variables align, the constants vanish, and we are left with the precise value that anchors our line into the plane.