Problem 28
Question
Verify, from Key Idea 10.2.1, that $$ \vec{u}=\langle\sin \theta \cos \varphi, \sin \theta \sin \varphi, \cos \theta\rangle $$ is a unit vector for all angles \(\theta\) and \(\varphi\).
Step-by-Step Solution
Verified Answer
The vector \(\vec{u}\) is a unit vector because its magnitude is 1 for all \(\theta\) and \(\varphi\).
1Step 1: Understand the Definition of a Unit Vector
A unit vector is a vector that has a magnitude of 1. Therefore, to verify if \( \vec{u} \) is a unit vector, we must ensure that the magnitude of \( \vec{u} \) is equal to 1.
2Step 2: Calculate the Magnitude of \( \vec{u} \)
The magnitude of a vector \( \vec{u} = \langle a, b, c \rangle \) is calculated using the formula: \[ \| \vec{u} \| = \sqrt{a^2 + b^2 + c^2}. \] For \( \vec{u} = \langle \sin \theta \cos \varphi, \sin \theta \sin \varphi, \cos \theta \rangle \), the magnitude becomes \[ \| \vec{u} \| = \sqrt{(\sin \theta \cos \varphi)^2 + (\sin \theta \sin \varphi)^2 + (\cos \theta)^2}. \]
3Step 3: Simplify the Magnitude Expression
Expanding each term inside the square root, we have:\[ = \sqrt{(\sin^2 \theta \cos^2 \varphi) + (\sin^2 \theta \sin^2 \varphi) + \cos^2 \theta}. \] Factor out \( \sin^2 \theta \) in the first two terms:\[ = \sqrt{\sin^2 \theta (\cos^2 \varphi + \sin^2 \varphi) + \cos^2 \theta}. \] Note that \( \cos^2 \varphi + \sin^2 \varphi = 1 \), due to the Pythagorean identity, thus simplifying:\[ = \sqrt{\sin^2 \theta \cdot 1 + \cos^2 \theta}. \] This reduces further to:\[ = \sqrt{\sin^2 \theta + \cos^2 \theta}. \] Again, using the Pythagorean identity \( \sin^2 \theta + \cos^2 \theta = 1 \):\[ = \sqrt{1} = 1. \]
4Step 4: Conclusion
Since the magnitude \( \| \vec{u} \| = 1 \), \( \vec{u} \) is indeed a unit vector. This verifies that the given vector \( \langle \sin \theta \cos \varphi, \sin \theta \sin \varphi, \cos \theta \rangle \) is a unit vector for all angles \( \theta \) and \( \varphi \).
Key Concepts
Vector MagnitudePythagorean IdentityTrigonometric Functions
Vector Magnitude
When we talk about the magnitude of a vector, we're referring to its length or size in space. It's like measuring how long a vector is, representing the distance from the point of origin to the vector's endpoint. To make this measurement, we use a formula that is rooted in the essence of geometry.
The magnitude of a vector with components \( \langle a, b, c \rangle \) is calculated using the formula for the Euclidean norm:
This formula is perfectly analogous to calculating the hypotenuse of a right triangle. In our problem, we verified that the vector \( \vec{u} = \langle \sin \theta \cos \varphi, \sin \theta \sin \varphi, \cos \theta \rangle \) has a magnitude (length) of 1. Therefore, it's a unit vector since its magnitude equals 1.
The magnitude of a vector with components \( \langle a, b, c \rangle \) is calculated using the formula for the Euclidean norm:
- \( \| \vec{u} \| = \sqrt{a^2 + b^2 + c^2} \)
This formula is perfectly analogous to calculating the hypotenuse of a right triangle. In our problem, we verified that the vector \( \vec{u} = \langle \sin \theta \cos \varphi, \sin \theta \sin \varphi, \cos \theta \rangle \) has a magnitude (length) of 1. Therefore, it's a unit vector since its magnitude equals 1.
Pythagorean Identity
The Pythagorean identity is a fundamental relation in trigonometry and describes how certain combinations of trigonometric functions always yield the same value. Specifically, the Pythagorean identity states:
In our vector verification, we leveraged this identity multiple times. For example, when simplifying the expression \( \sqrt{\sin^2 \theta + \cos^2 \theta} \), the Pythagorean identity helped us conclude that this expression simplifies to 1.
- \( \sin^2 \theta + \cos^2 \theta = 1 \)
In our vector verification, we leveraged this identity multiple times. For example, when simplifying the expression \( \sqrt{\sin^2 \theta + \cos^2 \theta} \), the Pythagorean identity helped us conclude that this expression simplifies to 1.
Trigonometric Functions
Trigonometric functions underpin many aspects of mathematics, particularly when dealing with angles and periodic phenomena. In the context of vectors, these functions often help us describe components in terms of angles.
For vectors like our \( \vec{u} \), these functions help form a bridge between angular measurements and linear dimensions. The components of the vector \( \vec{u} \) are products of trigonometric functions, reflecting the angles \( \theta \) and \( \varphi \) in three-dimensional space.
This illustrates how trigonometry enables us to navigate between angles and linear space, providing solutions that are both precise and elegantly structured.
- \( \sin \theta \)
- \( \cos \theta \)
- \( \tan \theta \)
For vectors like our \( \vec{u} \), these functions help form a bridge between angular measurements and linear dimensions. The components of the vector \( \vec{u} \) are products of trigonometric functions, reflecting the angles \( \theta \) and \( \varphi \) in three-dimensional space.
This illustrates how trigonometry enables us to navigate between angles and linear space, providing solutions that are both precise and elegantly structured.
Other exercises in this chapter
Problem 28
Find the area of the triangle with the given vertices. Vertices: (5,2,-1),(3,6,2) and (1,0,4) .
View solution Problem 28
Vectors \(\vec{u}\) and \(\vec{v}\) are given. Write \(\vec{u}\) as the sum of two vectors, one of which is parallel to \(\vec{v}\) and one of which is perpendi
View solution Problem 28
Sketch the quadric surface. \(z^{2}=x^{2}+\frac{y^{2}}{4}\)
View solution Problem 29
Find the given distances. The distance between the parallel planes \(x+y+z=0\) and $$ (x-2)+(y-3)+(z+4)=0 $$
View solution