Problem 101
Question
If the vectors \(\vec{a}=\hat{i}-\hat{j}+2 \hat{k}, \hat{b}=2 \hat{i}+4 \hat{j}+\hat{k}\) and \(\vec{c}=\lambda \hat{i}+\hat{j}\) \(+\mu \hat{k}\) are mutually orthogonal, then the tuple \((\lambda, \mu)=\) [2010] (A) \((2,-3)\) (B) \((-2,3)\) (C) \((3,-2)\) (D) \((-3,2)\)
Step-by-Step Solution
Verified Answer
(\lambda, \mu) = (-3, 2) \text{ (Option D)}.
1Step 1: Understand Mutual Orthogonality
Vectors are mutually orthogonal if the dot product between each pair of vectors is zero. So, for the vectors \(\vec{a}, \vec{b}, \vec{c}\), we have \(\vec{a} \cdot \vec{b} = 0\), \(\vec{b} \cdot \vec{c} = 0\), and \(\vec{c} \cdot \vec{a} = 0\).
2Step 2: Calculate \(\vec{a} \cdot \vec{b}\)
Compute the dot product: \(\vec{a} \cdot \vec{b} = (\hat{i} - \hat{j} + 2\hat{k}) \cdot (2\hat{i} + 4\hat{j} + \hat{k}) = 1 \times 2 + (-1) \times 4 + 2 \times 1\). This simplifies to \(2 - 4 + 2 = 0\). Thus, \(\vec{a} \cdot \vec{b} = 0\), confirming mutual orthogonality between \(\vec{a}\) and \(\vec{b}\).
3Step 3: Calculate \(\vec{b} \cdot \vec{c}\)
Compute the dot product: \(\vec{b} \cdot \vec{c} = (2\hat{i} + 4\hat{j} + \hat{k}) \cdot (\lambda\hat{i} + \hat{j} + \mu\hat{k}) = 2\lambda + 4 \times 1 + 1 \times \mu\). This simplifies to \(2\lambda + 4 + \mu = 0\).
4Step 4: Calculate \(\vec{c} \cdot \vec{a}\)
Compute the dot product: \(\vec{c} \cdot \vec{a} = (\lambda \hat{i} + \hat{j} + \mu \hat{k}) \cdot (\hat{i} - \hat{j} + 2\hat{k}) = \lambda \times 1 + 1 \times (-1) + \mu \times 2\). This simplifies to \(\lambda - 1 + 2\mu = 0\).
5Step 5: Solve the System of Equations
We have two equations: \(2\lambda + \mu = -4\) and \(\lambda + 2\mu = 1\). Solve this system to find \(\lambda\) and \(\mu\). Multiply the second equation by 2: \(2\lambda + 4\mu = 2\). Now subtract the first equation from this result: \(2\lambda + 4\mu - (2\lambda + \mu) = 2 + 4\), resulting in \(3\mu = 6\). Thus \(\mu = 2\). Substitute \(\mu = 2\) into \(\lambda + 2\mu = 1\), yielding \(\lambda + 4 = 1\) so \(\lambda = -3\).
6Step 6: Verify the Tuple
The solution is \((\lambda, \mu) = (-3, 2)\). This value satisfies both equations: \(2(-3) + 2 = -4\) and \(-3 + 2\times 2 = 1\). Therefore, the vectors are mutually orthogonal with this choice.
Key Concepts
Mutual OrthogonalityDot ProductSystem of Equations
Mutual Orthogonality
Vectors are said to be mutually orthogonal when there is no overlap in the direction they are pointing, kind of like how two paths that cross at right angles don't share any direction. In the context of vectors, this means the dot product between each pair of vectors is zero.
Consider three vectors, let's name them \(\vec{a}, \vec{b},\) and \(\vec{c}\). For these vectors to be mutually orthogonal:
This concept is extremely useful, especially in physics and engineering, where figuring out forces or components acting at right angles is essential.
Consider three vectors, let's name them \(\vec{a}, \vec{b},\) and \(\vec{c}\). For these vectors to be mutually orthogonal:
- The dot product \(\vec{a} \cdot \vec{b} = 0\)
- \(\vec{b} \cdot \vec{c} = 0\)
- \(\vec{c} \cdot \vec{a} = 0\)
This concept is extremely useful, especially in physics and engineering, where figuring out forces or components acting at right angles is essential.
Dot Product
The dot product is one of the fundamental operations you can perform with vectors. It combines two vectors into a single number. This product is heavily used to determine the angle relationship between two vectors.
The formula for the dot product of two vectors \(\vec{u} = u_1\hat{i} + u_2\hat{j} + u_3\hat{k}\) and \(\vec{v} = v_1\hat{i} + v_2\hat{j} + v_3\hat{k}\) is:
In our original exercise, the dot product helped us confirm the orthogonality of the vectors \(\vec{a}, \vec{b},\) and \(\vec{c}\), hence identifying the condition of mutual orthogonality.
The formula for the dot product of two vectors \(\vec{u} = u_1\hat{i} + u_2\hat{j} + u_3\hat{k}\) and \(\vec{v} = v_1\hat{i} + v_2\hat{j} + v_3\hat{k}\) is:
- \(\vec{u} \cdot \vec{v} = u_1v_1 + u_2v_2 + u_3v_3\)
In our original exercise, the dot product helped us confirm the orthogonality of the vectors \(\vec{a}, \vec{b},\) and \(\vec{c}\), hence identifying the condition of mutual orthogonality.
System of Equations
When solving vector problems, like finding whether vectors are mutually orthogonal, we often end up with a system of equations. A system of equations is simply multiple equations that you need to solve all at once. In our exercise, the mutual orthogonality conditions led us to two equations:
There are various methods to solve a system of equations, such as substitution, elimination, or using matrices. We used a step-by-step elimination method which involved:
- \(2\lambda + \mu = -4\)
- \(\lambda + 2\mu = 1\)
There are various methods to solve a system of equations, such as substitution, elimination, or using matrices. We used a step-by-step elimination method which involved:
- Adjusting one equation to eliminate one of the variables
- Solving for the remaining variable
- Back-substituting to find the other variable
Other exercises in this chapter
Problem 99
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