Problem 12
Question
Create your own vectors \(\vec{u}\) and \(\vec{v}\) in \(\mathbb{R}^{3}\) and scalar \(c\) and show that \(c(\vec{u} \cdot \vec{v})=\vec{u} \cdot(c \vec{v})\)
Step-by-Step Solution
Verified Answer
The equality \(c(\vec{u} \cdot \vec{v}) = \vec{u} \cdot (c \vec{v})\) holds true.
1Step 1: Define Vectors and Scalar
Let's choose two vectors in \(\mathbb{R}^3\). Let \(\vec{u} = \langle 1, 2, 3 \rangle\) and \(\vec{v} = \langle 4, 5, 6 \rangle\). Also, choose a scalar \(c = 2\).
2Step 2: Calculate the Scalar Multiplication of the Dot Product
First, compute the dot product \(\vec{u} \cdot \vec{v}\). The dot product is calculated as: \(\vec{u} \cdot \vec{v} = 1 \times 4 + 2 \times 5 + 3 \times 6 = 32\).Next, multiply the result by the scalar \(c\): \(c(\vec{u} \cdot \vec{v}) = 2 \times 32 = 64\).
3Step 3: Scalar Multiplication with the Second Vector
Multiply the vector \(\vec{v}\) by the scalar \(c\):\(c \vec{v} = 2 \times \langle 4, 5, 6 \rangle = \langle 8, 10, 12 \rangle\).
4Step 4: Calculate the Dot Product with the Scaled Vector
Now, compute the dot product of \(\vec{u}\) with the scaled vector \(c \vec{v}\):\(\vec{u} \cdot (c \vec{v}) = 1 \times 8 + 2 \times 10 + 3 \times 12 = 64\).
5Step 5: Compare the Results
Both calculations gave the result \(64\). Therefore, we have shown that \(c(\vec{u} \cdot \vec{v}) = \vec{u} \cdot (c \vec{v})\).
Key Concepts
Scalar MultiplicationVector OperationsProperties of Dot Product
Scalar Multiplication
Scalar multiplication involves multiplying a vector by a single number, known as a scalar. This operation scales the magnitude of the vector without changing its direction. Take, for example, the vector \( \vec{v} = \langle 4, 5, 6 \rangle \). If we multiply every component of \( \vec{v} \) by the scalar \( c = 2 \), each component is scaled, resulting in a new vector: \( c \vec{v} = \langle 8, 10, 12 \rangle \).
- Identity property: Multiplying a vector by 1 gives the same vector.
- Zero vector: Multiplying by 0 results in the zero vector.
- Distributive property: Scalar multiplication distributes over vector addition.
Vector Operations
Working with vectors involves a variety of operations that allow us to analyze their properties and interactions. The essential operations include addition, subtraction, and multiplication (like the dot product).
When you add two vectors, say, \( \vec{u} = \langle 1, 2, 3 \rangle \) and \( \vec{v} = \langle 4, 5, 6 \rangle \), you add their corresponding components:
Multiplication, such as the dot product, combines vectors to yield a scalar. Understanding these operations helps in transitioning from abstract concepts to practical applications in physics and engineering.
When you add two vectors, say, \( \vec{u} = \langle 1, 2, 3 \rangle \) and \( \vec{v} = \langle 4, 5, 6 \rangle \), you add their corresponding components:
- Addition: \( \vec{u} + \vec{v} = \langle 1+4, 2+5, 3+6 \rangle = \langle 5, 7, 9 \rangle \)
Multiplication, such as the dot product, combines vectors to yield a scalar. Understanding these operations helps in transitioning from abstract concepts to practical applications in physics and engineering.
Properties of Dot Product
The dot product is a key operation in vector algebra, often used to find the angle between vectors or to project one vector onto another. It results in a scalar, not a vector.
How the dot product works: If \( \vec{u} = \langle 1, 2, 3 \rangle \) and \( \vec{v} = \langle 4, 5, 6 \rangle \), the dot product is calculated as: \( \vec{u} \cdot \vec{v} = 1 \cdot 4 + 2 \cdot 5 + 3 \cdot 6 = 32 \).Key properties include:
How the dot product works: If \( \vec{u} = \langle 1, 2, 3 \rangle \) and \( \vec{v} = \langle 4, 5, 6 \rangle \), the dot product is calculated as: \( \vec{u} \cdot \vec{v} = 1 \cdot 4 + 2 \cdot 5 + 3 \cdot 6 = 32 \).Key properties include:
- Commutative Property: \( \vec{u} \cdot \vec{v} = \vec{v} \cdot \vec{u} \)
- Distributive over Addition: \( \vec{u} \cdot (\vec{v} + \vec{w}) = \vec{u} \cdot \vec{v} + \vec{u} \cdot \vec{w} \)
- Scalar Multiplication: \( c(\vec{u} \cdot \vec{v}) = \vec{u} \cdot (c \vec{v}) \).
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