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

Short Answer

Expert verified
Answer: The indefinite integral of the vector function \( \mathbf{r}(t) \) is given by \( \mathbf{R}(t) = \left\langle \frac{1}{4}t^4 - \frac{3}{2}t^2 + C_1, \ t^2 - t + C_2, \ 10t + C_3 \right\rangle \), where \( C_1 \), \( C_2 \) and \( C_3 \) are constants of integration.

Step by step solution

01

Identify Components

The provided vector function has three components: 1. \(x(t) = t^3 - 3t\) 2. \(y(t) = 2t - 1\) 3. \(z(t) = 10\)
02

Integrate Each Component

Integrate each component with respect to \(t\): 1. \(\int (t^3-3t) dt\) 2. \(\int (2t-1) dt\) 3. \(\int 10 dt\)
03

Solve Component Integrals

After solving each integral, we get: 1. \(\int (t^3-3t) dt = \frac{1}{4}t^4 - \frac{3}{2}t^2 + C_1\) 2. \(\int (2t-1) dt = t^2 - t + C_2\) 3. \(\int 10 dt = 10t + C_3\)
04

Write the Indefinite Integral

Combine these component integrals to form the final indefinite integral: $$ \mathbf{R}(t) = \left\langle \frac{1}{4}t^4 - \frac{3}{2}t^2 + C_1, \ t^2 - t + C_2, \ 10t + C_3 \right\rangle $$

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Key Concepts

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

Vector Calculus
Vector calculus is a field of mathematics that deals with vector fields and the differentiation and integration of vector functions. In this exercise, we dealt with a vector function \( \mathbf{r}(t) = \langle t^3 - 3t, 2t - 1, 10 \rangle \). Vector functions like \( \mathbf{r}(t) \) are composed of multiple component functions—each representing a different dimension in space. Vector calculus allows us to analyze these functions and understand their behavior in multi-dimensional space.

Common operations in vector calculus include differentiation and integration of vector functions, just like we do with scalar functions. Here, our task was to compute the indefinite integrals of each component of \( \mathbf{r}(t) \), bringing us to the realm of vector integration. This enables us to find a function that represents the accumulation of change along a vector field.
Component Integration
Component integration is a technique used when working with vector functions. Since vector functions are composed of multiple individual functions, each corresponding to a component of the vector, they must be integrated separately.

In our exercise, the vector function \( \mathbf{r}(t) = \langle t^3 - 3t, 2t - 1, 10 \rangle \) was broken down into three components:
  • \( x(t) = t^3 - 3t \)
  • \( y(t) = 2t - 1 \)
  • \( z(t) = 10 \)

Each component is integrated separately with respect to \( t \). This method ensures each part of the vector is accurately processed:
  • \( \int (t^3 - 3t) \ dt = \frac{1}{4}t^4 - \frac{3}{2}t^2 + C_1 \)
  • \( \int (2t - 1) \ dt = t^2 - t + C_2 \)
  • \( \int 10 \ dt = 10t + C_3 \)

Remember to add constants of integration \( C_1, C_2, C_3 \) since these integrals are indefinite.
Integration Technique
The integration technique used in this exercise is straightforward but crucial for solving indefinite integrals for vector fields. In simple terms, integration is the process of finding a function that describes the accumulation of quantities. Here, we focus on the indefinite integral, which results in a function plus a constant (or constants, in the vector case).

To integrate functions like \( \int (t^3 - 3t) \ dt \) or \( \int (2t - 1) \ dt \), we apply basic integration rules such as the power rule and linearity of integration:
  • The power rule states that \( \int t^n \ dt = \frac{1}{n+1}t^{n+1} + C \), which is applied when integrating terms like \( t^3 \).
  • For linear terms such as \( 2t \), you simply adjust constants, giving \( \int 2t \ dt = t^2 + C \).
  • Constant terms are integrated by multiplying by \( t \), as in \( \int 10 \ dt = 10t + C \).

By integrating each component separately using these basic techniques, you can reconstruct the vector's indefinite integral, maintaining the initial vector's structure but accounting for the cumulative effect over a variable \( t \).

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Most popular questions from this chapter

Suppose an object moves on the surface of a sphere with \(|\mathbf{r}(t)|\) constant for all \(t\) Show that \(\mathbf{r}(t)\) and \(\mathbf{a}(t)=\mathbf{r}^{\prime \prime}(t)\) satisfy \(\mathbf{r}(t) \cdot \mathbf{a}(t)=-|\mathbf{v}(t)|^{2}\)

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A baseball leaves the hand of a pitcher 6 vertical feet above home plate and \(60 \mathrm{ft}\) from home plate. Assume that the coordinate axes are oriented as shown in the figure. a. In the absence of all forces except gravity, assume that a pitch is thrown with an initial velocity of \(\langle 130,0,-3\rangle \mathrm{ft} / \mathrm{s}\) (about \(90 \mathrm{mi} / \mathrm{hr}\) ). How far above the ground is the ball when it crosses home plate and how long does it take for the pitch to arrive? b. What vertical velocity component should the pitcher use so that the pitch crosses home plate exactly \(3 \mathrm{ft}\) above the ground? c. A simple model to describe the curve of a baseball assumes that the spin of the ball produces a constant sideways acceleration (in the \(y\) -direction) of \(c \mathrm{ft} / \mathrm{s}^{2}\). Assume a pitcher throws a curve ball with \(c=8 \mathrm{ft} / \mathrm{s}^{2}\) (one-fourth the acceleration of gravity). How far does the ball move in the \(y\) -direction by the time it reaches home plate, assuming an initial velocity of (130,0,-3) ft/s? d. In part (c), does the ball curve more in the first half of its trip to the plate or in the second half? How does this fact affect the batter? e. Suppose the pitcher releases the ball from an initial position of (0,-3,6) with initial velocity \((130,0,-3) .\) What value of the spin parameter \(c\) is needed to put the ball over home plate passing through the point (60,0,3)\(?\)

For the following vectors u and \(\mathbf{v}\) express u as the sum \(\mathbf{u}=\mathbf{p}+\mathbf{n},\) where \(\mathbf{p}\) is parallel to \(\mathbf{v}\) and \(\mathbf{n}\) is orthogonal to \(\mathbf{v}\). \(\mathbf{u}=\langle-2,2\rangle, \mathbf{v}=\langle 2,1\rangle\)

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