Problem 47
Question
In Problems 45-50, give a proof of the indicated property for two-dimensional vectors. Use \(\mathbf{u}=\left\langle u_{1}, u_{2}\right\rangle, \mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\), and \(\mathbf{w}=\left\langle w_{1}, w_{2}\right\rangle\). $$ c(\mathbf{u} \cdot \mathbf{v})=(c \mathbf{u}) \cdot \mathbf{v} $$
Step-by-Step Solution
Verified Answer
Both sides simplify to \(cu_1 \cdot v_1 + cu_2 \cdot v_2\), proving the property.
1Step 1: Understand the Dot Product
The dot product for two-dimensional vectors \(\mathbf{u} = \langle u_1, u_2 \rangle\) and \(\mathbf{v} = \langle v_1, v_2 \rangle\) is calculated as \(\mathbf{u} \cdot \mathbf{v} = u_1 \cdot v_1 + u_2 \cdot v_2\). We need to show that multiplying the dot product by a scalar \(c\) is equivalent to multiplying \(\mathbf{u}\) by \(c\) first and then taking the dot product with \(\mathbf{v}\).
2Step 2: Simplify the Left Side
The left side of the equation is \(c(\mathbf{u} \cdot \mathbf{v})\). Using the definition of the dot product, this becomes \(c(u_1 \cdot v_1 + u_2 \cdot v_2)\), which can be distributed to get \(cu_1 \cdot v_1 + cu_2 \cdot v_2\).
3Step 3: Simplify the Right Side
The right side of the equation is \((c \mathbf{u}) \cdot \mathbf{v}\). First, multiply \(\mathbf{u}\) by the scalar \(c\) to get \(c \mathbf{u} = \langle cu_1, cu_2 \rangle\). Then, take the dot product with \(\mathbf{v}\): \(\langle cu_1, cu_2 \rangle \cdot \langle v_1, v_2 \rangle = cu_1 \cdot v_1 + cu_2 \cdot v_2\).
4Step 4: Compare Both Sides
From Steps 2 and 3, we saw that the left side simplifies to \(cu_1 \cdot v_1 + cu_2 \cdot v_2\) and the right side also simplifies to \(cu_1 \cdot v_1 + cu_2 \cdot v_2\). Since both sides are equal, the property \(c(\mathbf{u} \cdot \mathbf{v}) = (c \mathbf{u}) \cdot \mathbf{v}\) is proven.
Key Concepts
Dot ProductScalar MultiplicationVector Properties
Dot Product
The dot product is a key concept in vector calculus. It takes two vectors and results in a scalar, essentially a single number. For two-dimensional vectors like \(\mathbf{u} = \langle u_1, u_2 \rangle\) and \(\mathbf{v} = \langle v_1, v_2 \rangle\), the dot product is calculated as:
- \(\mathbf{u} \cdot \mathbf{v} = u_1 \cdot v_1 + u_2 \cdot v_2\)
Scalar Multiplication
Scalar multiplication is a simple yet crucial operation in vector mathematics. It involves multiplying a vector by a scalar (a single number). For example, if you have a vector \(\mathbf{u} = \langle u_1, u_2 \rangle\) and a scalar \(c\), the resulting vector after scalar multiplication is:
- \(c \mathbf{u} = \langle cu_1, cu_2 \rangle\)
Vector Properties
Vectors are incredibly versatile mathematical objects with distinct properties that differentiate them from other mathematical entities like numbers. Some fundamental properties of vectors include:
- Magnitude: The length or size of the vector, calculated using the Pythagorean theorem for two-dimensional vectors \( \mathbf{u} = \langle u_1, u_2 \rangle\) as \( \sqrt{u_1^2 + u_2^2} \).
- Direction: The orientation of the vector, which remains unchanged during scalar multiplication (excluding the possible direction reversal when the scalar is negative).
- Equality: Two vectors are equal if their corresponding components are equal. For instance, \(\mathbf{u} = \mathbf{v}\) if and only if \(u_1 = v_1\) and \(u_2 = v_2\).
- Addition: Adding two vectors is done component-wise. For two vectors \(\mathbf{u}\) and \(\mathbf{v}\), their sum is \(\langle u_1 + v_1, u_2 + v_2 \rangle\).
Other exercises in this chapter
Problem 45
The solid spheres \((x-1)^{2}+(y-2)^{2}+(z-1)^{2} \leq 4\) and \((x-2)^{2}+(y-4)^{2}+(z-3)^{2} \leq 4\) intersect in a solid. Find its volume.
View solution Problem 46
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(x(t)=1+3 t
View solution Problem 47
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}
View solution Problem 47
Describe in general terms the following "helical" type motions: (a) \(\mathbf{r}(t)=\sin t \mathbf{i}+\cos t \mathbf{j}+t \mathbf{k}\) (b) \(\mathbf{r}(t)=\sin
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