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Compute the indefinite integral of the following functions. $$\mathbf{r}(t)=\left\langle t^{4}-3 t, 2 t-1,10\right\rangle$$

Short Answer

Expert verified
Answer: The indefinite integral of the given vector-valued function is \(\mathbf{R}(t) = \left\langle \frac{t^5}{5} - \frac{3t^2}{2} + C_1, t^2 - t + C_2, 10t + C_3 \right\rangle\), where \(C_1\), \(C_2\), and \(C_3\) are constants of integration.

Step by step solution

01

Separate the components of the vector

We can represent the given vector function, \(\mathbf{r}(t)\), as three separate scalar functions: $$f(t) = t^4 - 3t,$$ $$g(t) = 2t - 1,$$ $$h(t) = 10.$$
02

Integrate each component

Now, we will find the indefinite integral of each scalar function, \(f(t)\), \(g(t)\), and \(h(t)\): $$F(t) = \int (t^4 - 3t) dt,$$ $$G(t) = \int (2t - 1) dt,$$ $$H(t) = \int 10 dt.$$
03

Find the antiderivative of each component

Now, we will find the antiderivative of each of these scalar functions: $$F(t) = \frac{t^5}{5} - \frac{3t^2}{2} + C_1,$$ $$G(t) = t^2 - t + C_2,$$ $$H(t) = 10t + C_3,$$ where \(C_1\), \(C_2\), and \(C_3\) are constants of integration.
04

Combine the components

Finally, we will combine the results of our calculations above to form the new vector-valued function, \(\mathbf{R}(t)\): $$\mathbf{R}(t) = \left\langle \frac{t^5}{5} - \frac{3t^2}{2} + C_1, t^2 - t + C_2, 10t + C_3 \right\rangle.$$ This is the indefinite integral of the given vector-valued function, \(\mathbf{r}(t)\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Indefinite Integral
When solving problems in calculus, indefinite integrals play a crucial role. An indefinite integral is the reverse operation of differentiation. It helps us find a function whose derivative is the given function. This process is also known as integration without limits.
For real-valued functions, the indefinite integral takes the form:
  • \( \int f(x) \, dx = F(x) + C \)
Here, \(F(x)\) is the antiderivative of \(f(x)\), and \(C\) represents the constant of integration. Indefinite integrals help us discover families of functions that vary by this constant. This is important because the process of differentiation loses information about constant terms in the function, which integration restores.
When dealing with vector-valued functions, we apply these integration concepts component-wise, meaning each dimension of the vector is integrated separately.
Antiderivative
The concept of an antiderivative is foundational to understanding indefinite integrals. The antiderivative works as the inverse of differentiation. It reconstructs a function from its derivative. Another way to describe it is that if \(F(x)\) is an antiderivative of \(f(x)\), then \(F'(x) = f(x)\).
Let's explore how to find one. Consider \(f(x)\) as your function, and look for some function \(F(x)\) that satisfies the following:
  • \(\frac{d}{dx}[F(x)] = f(x)\)
Remember that there are infinitely many antiderivatives for any given function. All differ by a constant. Thus, the notation \(F(x) + C\) captures this infinite family, where \(C\) is any real number. If you differentiate \(F(x) + C\), you still get \(f(x)\), as the derivative of a constant is zero.
In vector-valued functions, an antiderivative individually handles each component of the vector. This keeps each part's distinct identity while assembling the general solution.
Vector-Valued Function
Vector-valued functions expand the idea of a regular function to include output in vector form. In essence, they map a single input value, like \(t\), into a multi-dimensional vector.
These functions are represented as:
  • \( \mathbf{r}(t) = \langle f(t), g(t), h(t) \rangle \)
Where \(f(t)\), \(g(t)\), and \(h(t)\) are the component functions.
Understanding vector-valued functions involves operating on their components separately. They are embedded in contexts like physics and engineering, where motions or forces have directions represented by vectors.
To compute an indefinite integral for such functions, integrate each of the component functions one by one. Once integrated, combine the results to form the final vector, which will express the integrated relation. This step-by-step component-focused approach makes it easier to manage multifaceted problems common in real-world applications.

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Most popular questions from this chapter

Three-dimensional motion Consider the motion of the following objects. Assume the \(x\) -axis points east, the \(y\) -axis points north, the positive z-axis is vertical and opposite g. the ground is horizontal, and only the gravitational force acts on the object unless otherwise stated. a. Find the velocity and position vectors, for \(t \geq 0\). b. Make a sketch of the trajectory. c. Determine the time of flight and range of the object. d. Determine the maximum height of the object. A baseball is hit 3 ft above home plate with an initial velocity of \(\langle 30,30,80\rangle \mathrm{ft} / \mathrm{s} .\) The spin on the baseball produces a horizontal acceleration of the ball of \(5 \mathrm{ft} / \mathrm{s}^{2}\) in the northward direction.

Consider the following curves. a. Graph the curve. b. Compute the curvature. c. Graph the curvature as a ficnction of the parameter. d. Identify the points (if any) at which the curve has a maximum or minimum curvature. e. Verify that the graph of the curvature is consistent with the graph of the curve. $$\mathbf{r}(t)=\left\langle t, t^{2}\right\rangle, \text { for }-2 \leq t \leq 2 \quad \text { (parabola) }$$

Consider the curve. $$\mathbf{r}(t)=\langle a \cos t+b \sin t, c \cos t+d \sin t, e \cos t+f \sin t\rangle$$ where \(a, b, c, d, e,\) and \(f\) are real numbers. It can be shown that this curve lies in a plane. Graph the following curve and describe it. $$ \begin{aligned} \mathbf{r}(t)=&\left(\frac{1}{\sqrt{2}} \cos t+\frac{1}{\sqrt{3}} \sin t\right) \mathbf{i} \\ &+\left(-\frac{1}{\sqrt{2}} \cos t+\frac{1}{\sqrt{3}} \sin t\right) \mathbf{j}+\left(\frac{1}{\sqrt{3}} \sin t\right) \mathbf{k}\end{aligned}$$

Let \(\mathbf{u}(t)=\left\langle 1, t, t^{2}\right\rangle, \mathbf{v}(t)=\left\langle t^{2},-2 t, 1\right\rangle\) and \(g(t)=2 \sqrt{t}\). Compute the derivatives of the following functions. $$\mathbf{u}(t) \cdot \mathbf{v}(t)$$

Three-dimensional motion Consider the motion of the following objects. Assume the \(x\) -axis points east, the \(y\) -axis points north, the positive z-axis is vertical and opposite g. the ground is horizontal, and only the gravitational force acts on the object unless otherwise stated. a. Find the velocity and position vectors, for \(t \geq 0\). b. Make a sketch of the trajectory. c. Determine the time of flight and range of the object. d. Determine the maximum height of the object. A soccer ball is kicked from the point \langle 0,0,0\rangle with an initial velocity of \(\langle 0,80,80\rangle \mathrm{ft} / \mathrm{s} .\) The spin on the ball produces an acceleration of \(\langle 1.2,0,0\rangle \mathrm{ft} / \mathrm{s}^{2}\).

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