Animated Solution for Mathematics - Matrices and Determinants: If the system of linear equations 8x+y+4z=−2, x+y+z=0, λx−3y=μ has infinitely many solutions, then the distance of the point (λ,μ,−21) from the plane 8x+y+4z+2=0 is :
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Visualized Solution
System of Equations
Given system:
8x+y+4z=−2
x+y+z=0
λx−3y=μ
Condition for infinitely many solutions: Planes intersect in a line.
Condition for Infinite Solutions
For infinitely many solutions, Cramer's rule states:
D=D1=D2=D3=0
Set up Determinant D
Coefficient Determinant D:
D=81λ11−3410
Set D=0.
Solve for λ
Expanding D along the first row:
8(0−(−3))−1(0−λ)+4(−3−λ)=0
24+λ−12−4λ=0
12−3λ=0⟹λ=4
Set up Determinant D1
Determinant D1 (replacing first column with constants):
D1=−20μ11−3410
Set D1=0.
Solve for μ
Expanding D1 along the first row:
−2(0−(−3))−1(0−μ)+4(0−μ)=0
−6+μ−4μ=0
−6−3μ=0⟹μ=−2
Identify the Point P
Point P=(λ,μ,−21)
Substituting λ=4 and μ=−2:
P=(4,−2,−21)
The Distance Formula
Target Plane Π1: 8x+y+4z+2=0
Distance d from point (x1,y1,z1) to plane ax+by+cz+d=0:
d=a2+b2+c2∣ax1+by1+cz1+d∣
Substitute Coordinates
Substituting P(4,−2,−21) into the formula:
d=82+12+42∣8(4)+1(−2)+4(−21)+2∣
Calculate Numerator and Denominator
d=64+1+16∣32−2−2+2∣
d=81∣30∣
Final Answer
d=930
d=310
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The Sigma Insight: Solution of System of Linear Equations (Matrix Method and Cramer's Rule)
Solution Diagram
Analyzing the Setup
Welcome, fellow traveler of the mathematical landscape. Today, we are not just solving a system of equations; we are exploring the architecture of 3D space.
Imagine standing in a room where three massive, flat planes intersect. Usually, they meet at a single point—a corner of a room.
But here, the problem tells us something fascinating: the system has infinitely many solutions. This means our three planes do not meet at a single point, but instead, they slice through each other to form a common line of intersection.
The Cramer's Rule Toolkit
When we face a system of linear equations with parameters like λ and μ, we need a powerful lens. Enter Cramer's Rule.
For a system to have infinitely many solutions, the 'volume' of the parallelepiped formed by the coefficients must collapse to zero. Mathematically, this means the main determinant D and the auxiliary determinants D1, D2, and D3 must all vanish.
We are looking for the condition where the system becomes dependent, where one equation is essentially a linear combination of the others.
The Algebraic Hunt
Let us set up our determinant D using the coefficients of x, y, and z:
D=81λ11−3410=0
We expand along the first row:
8(0−(−3))−1(0−λ)+4(−3−λ)=0
Simplifying this, we find 24+λ−12−4λ=0, which leads to 12−3λ=0. Thus, λ=4.
With λ secured, we repeat the process for D1 by replacing the first column with the constants −2, 0, and μ:
D1=−20μ11−3410=0
Expanding this yields:
−2(0−(−3))−1(0−μ)+4(0−μ)=0
This simplifies to −6+μ−4μ=0, giving us μ=−2. We have successfully cracked the code.
The Final Geometric Leap
Now that we have our parameters, we identify our point P as (4,−2,−21). The final challenge is to find the distance of this point from the plane 8x+y+4z+2=0.
Notice that this plane is actually the first equation from our original system. We use the classic distance formula:
d=a2+b2+c2∣ax1+by1+cz1+d∣
Substituting our coordinates, we get:
d=82+12+42∣8(4)+1(−2)+4(−21)+2∣
The numerator simplifies to ∣32−2−2+2∣=30, and the denominator is 64+1+16=81=9.
Thus, the final distance is:
d=930=310
Conclusion
Look at that result: 310. It is not just a number; it is the culmination of understanding how planes interact in space.
You navigated the determinants, handled the parameters, and applied the distance formula with precision. Keep this geometric intuition alive—it is the secret weapon of every great mathematician.