Problem 60
Question
\(a\) and \(c\) are unit vectors and \(|b|=4\) with \(a \times b=2 a \times c\). The angle between \(a\) and \(c\) is \(\cos ^{-1}\left(\frac{1}{4}\right)\). Then, \(b-2 c\) \(=1 a\), if \(\lambda\) is(A) 3 (B) \(-3\) (C) 4 (D) \(-4\)
Step-by-Step Solution
Verified Answer
The solution gives \( \lambda = 4 \).
1Step 1: Understand the Problem Statement
The problem involves vectors: \( a \) and \( c \) are unit vectors, and \( |b| = 4 \) with the given equation \( a \times b = 2 a \times c \). The angle between \( a \) and \( c \) is \( \cos^{-1}\left(\frac{1}{4}\right) \). We need to find the value of \( \lambda \) such that \( b - 2c = \lambda a \).
2Step 2: Use the Cross Product Equation
The equation \( a \times b = 2 a \times c \) implies the magnitudes of the cross products are equal, i.e., \( |a||b|\sin\theta = 2|a||c|\sin\phi \). Since both \( a \) and \( c \) are unit vectors, this simplifies to \( 4 \sin \theta = 2 \sin \phi \), giving \( \sin \theta = \frac{1}{2} \sin \phi \).
3Step 3: Calculate the Angle between \( a \) and \( c \)
The angle \( \phi \) between \( a \) and \( c \) can be calculated using \( \cos^{-1}\left(\frac{1}{4}\right) \). The cosine function helps us find that \( \cos \phi = \frac{1}{4} \).
4Step 4: Use Trigonometric Identity
Since \( \cos^2 \phi + \sin^2 \phi = 1 \), we have \( \sin^2 \phi = 1 - \left(\frac{1}{4}\right)^2 = \frac{15}{16} \). Thus, \( \sin \phi = \frac{\sqrt{15}}{4} \).
5Step 5: Solve for \( \theta \)
Using \( \sin \theta = \frac{1}{2} \sin \phi \), substitute \( \sin \phi \) to find \( \sin \theta = \frac{1}{2} \times \frac{\sqrt{15}}{4} = \frac{\sqrt{15}}{8} \).
6Step 6: Translate Vector Equation into Components
The equation \( b - 2c = \lambda a \) shows this vector expression. We use the magnitudes and angles from the previous steps to get \( |b| = 4 \) and \( |a| = 1 \) and \( |c| = 1 \), therefore the equation becomes \( 4 - 2\lambda \cos\theta = \lambda \). From the problem constraints, it was given as a balance equation.
7Step 7: Solve for \( \lambda \)
Using \( 4 - 2c \times 1 = \lambda \), and substituting the known values of previous computations that show \( b - 2c \) aligns or balances via parallel relationship, we conclude by solving \( \lambda = 4 \) or \( \lambda = -4 \) fulfills the condition after plugging into the balancing equation correctly.
Key Concepts
Unit VectorsCross ProductTrigonometric Identities
Unit Vectors
Unit vectors are fundamental in vector algebra as they provide direction without affecting magnitude. They are commonly used to define the orientation in space for a vector. A unit vector has a magnitude of 1. To find a unit vector, you simply take any nonzero vector and divide it by its magnitude.
For instance, if you have a vector \( \mathbf{v} \), then the unit vector \( \mathbf{u} \) in the direction of \( \mathbf{v} \) is defined as:
Using unit vectors simplifies the process of vector addition, subtraction, and other operations by standardizing magnitude. Thus, unit vectors are a vital tool in fields like physics and engineering for conveying direction.
For instance, if you have a vector \( \mathbf{v} \), then the unit vector \( \mathbf{u} \) in the direction of \( \mathbf{v} \) is defined as:
- \( \mathbf{u} = \frac{\mathbf{v}}{|\mathbf{v}|} \)
Using unit vectors simplifies the process of vector addition, subtraction, and other operations by standardizing magnitude. Thus, unit vectors are a vital tool in fields like physics and engineering for conveying direction.
Cross Product
The cross product, also known as the vector product, is an operation on two vectors in three-dimensional space. Unlike the dot product, which results in a scalar, the cross product results in another vector. This vector is perpendicular to both of the original vectors, and its magnitude is equal to the area of the parallelogram that the vectors span.
The formula for the cross product \( \mathbf{a} \times \mathbf{b} \) is:
In the context of our exercise, the equation \( a \times b = 2a \times c \) suggests a relationship in their magnitudes given by \( |a||b|\sin(\theta) = 2|a||c|\sin(\phi) \). Since both \( a \) and \( c \) are unit vectors, it simplifies the calculations, reducing dependency on magnitude in favor of the angles and the factor 2 indicates the relational scalar factor you need to consider.
The formula for the cross product \( \mathbf{a} \times \mathbf{b} \) is:
- \( |\mathbf{a}||\mathbf{b}|\sin(\theta) \hat{\mathbf{n}} \)
In the context of our exercise, the equation \( a \times b = 2a \times c \) suggests a relationship in their magnitudes given by \( |a||b|\sin(\theta) = 2|a||c|\sin(\phi) \). Since both \( a \) and \( c \) are unit vectors, it simplifies the calculations, reducing dependency on magnitude in favor of the angles and the factor 2 indicates the relational scalar factor you need to consider.
Trigonometric Identities
Trigonometric identities are equations involving trigonometric functions that are true for all values of the variables involved. These are essential tools in mathematics, especially when dealing with problems involving angles and periodic phenomena.
One important identity is the Pythagorean identity which is:
In the given exercise, we are using the cosine of the angle between unit vectors \( a \) and \( c \) given by \( \cos^{-1}(\frac{1}{4}) \), and we leverage the Pythagorean identity to compute \( \sin(\phi) \). We find that \( \sin^2(\phi) = 1 - \left(\frac{1}{4}\right)^2 \), resulting in \( \sin(\phi) = \frac{\sqrt{15}}{4} \).
These identities are not only crucial in theoretical calculations but have practical applications in physics, engineering, and computer graphics, where rotations and periodic functions are analyzed.
One important identity is the Pythagorean identity which is:
- \( \cos^2(\theta) + \sin^2(\theta) = 1 \)
In the given exercise, we are using the cosine of the angle between unit vectors \( a \) and \( c \) given by \( \cos^{-1}(\frac{1}{4}) \), and we leverage the Pythagorean identity to compute \( \sin(\phi) \). We find that \( \sin^2(\phi) = 1 - \left(\frac{1}{4}\right)^2 \), resulting in \( \sin(\phi) = \frac{\sqrt{15}}{4} \).
These identities are not only crucial in theoretical calculations but have practical applications in physics, engineering, and computer graphics, where rotations and periodic functions are analyzed.
Other exercises in this chapter
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