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a) Let \(\mathbf{r}(t)\) be the radius-vector of a point moving in space, \(\mathbf{r}_{0}=\mathbf{r}(0)\) the initial position of the point, and \(\mathbf{v}(t)\) the velocity vector as a function of time. Show how to recover \(\mathbf{r}(t)\) from \(\mathbf{r}_{0}\) and \(\mathbf{v}(t)\) b) Does the integration of vector-valued functions reduce to integrating realvalued functions? c) Is the criterion for integrability stated in Proposition \(2^{\prime}\) valid for vector-valued functions? d) Is Lebesgue's criterion for integrability valid for vector-valued functions? e) Which concepts and facts from this section extend to functions with complex values?

Short Answer

Expert verified
Answer: The position vector \(\mathbf{r}(t)\) can be recovered from the initial position \(\mathbf{r}_0\) and the velocity vector \(\mathbf{v}(t)\) by first integrating the velocity vector with respect to time and then adding the initial position vector. The equation is \(\mathbf{r}(t) = \int \mathbf{v}(t) dt + \mathbf{r}_0\).

Step by step solution

01

1. Recovering the position vector

To recover the position vector \(\mathbf{r}(t)\) from the initial position \(\mathbf{r}_0\) and the velocity vector \(\mathbf{v}(t)\), we need to find the connection between them. Since velocity is the derivative of position with respect to time, we can write the equation as \(\mathbf{v}(t) = \frac{d\mathbf{r}(t)}{dt}\). Now, we can integrate both sides with respect to \(t\): \(\int \mathbf{v}(t) dt = \int \frac{d\mathbf{r}(t)}{dt} dt\) Let's perform the integration: \(\int \mathbf{v}(t) dt = \mathbf{r}(t) + C\) Where \(C\) is the constant of integration. To find the value of \(C\), we use the initial position \(\mathbf{r}_0 = \mathbf{r}(0)\): \(\mathbf{r}_0 = \mathbf{r}(0) + C \Rightarrow C = \mathbf{r}_0 - \mathbf{r}(0)\) So, we get: \(\mathbf{r}(t) = \int \mathbf{v}(t) dt + \mathbf{r}_0\)
02

2. Integration of vector-valued functions

The integration of vector-valued functions can be reduced to integrating real-valued functions when the components of the vector-valued function are real-valued functions. For example, if \(\mathbf{v}(t) = \langle f(t), g(t), h(t) \rangle\), then: \(\int \mathbf{v}(t) dt = \langle \int f(t) dt, \int g(t) dt, \int h(t) dt \rangle\)
03

3. Criterion for integrability in Proposition 2'

The criterion for integrability stated in Proposition 2' can be applied to vector-valued functions, as the components of the vector-valued function are real-valued functions. If the real-valued functions satisfy the conditions of Proposition 2', then the vector-valued function is also integrable.
04

4. Lebesgue's criterion for integrability

Lebesgue's criterion for integrability is valid for vector-valued functions, as long as their components are real-valued functions. If the components are Lebesgue integrable (i.e., they are measurable and have finite integrals) then the vector-valued function as a whole is integrable.
05

5. Extension of concepts and facts to complex-valued functions

Many concepts and facts from this section can be extended to functions with complex values. Complex-valued functions can be treated similarly to vector-valued functions, where the real and imaginary parts take the place of individual components. Integration, differentiability, and continuity concepts can be applied to complex-valued functions in a similar way to real-valued and vector-valued functions.

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Key Concepts

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

Vector-Valued Functions
Vector-valued functions assign a vector to each point in a given interval or domain. These functions are particularly useful in describing physical phenomena, like the motion of objects in space. For example, if you think of a moving object, its position at any given time can be represented by a vector-valued function such as \(\mathbf{r}(t) = \langle x(t), y(t), z(t) \rangle\).
Here, \(x(t)\), \(y(t)\), and \(z(t)\) are real-valued functions representing the object's coordinates in three-dimensional space. The velocity of the object is simply the derivative of this position vector, given by \(\mathbf{v}(t) = \frac{d\mathbf{r}(t)}{dt}\).
This makes vector-valued functions an essential tool for analyzing and solving problems where multiple dimensions and variables interact.
Integration of Vector Functions
When it comes to integrating vector-valued functions, the process can often be simplified. This simplification occurs because you can treat each component of the vector independently. For example, if you have a vector function \(\mathbf{v}(t) = \langle f(t), g(t), h(t) \rangle\), you would integrate each component separately to find:
  • \(\int f(t)\,dt\)
  • \(\int g(t)\,dt\)
  • \(\int h(t)\,dt\)
Thus, the integral of the vector function can be expressed as \(\int \mathbf{v}(t) \, dt = \langle \int f(t) \, dt, \int g(t) \, dt, \int h(t) \, dt \rangle\).
This way, integrating vector-valued functions reduces to integrating simple real-valued functions for each component.
Criterion for Integrability
To determine if a vector-valued function is integrable, it's vital to check each of its components. Often, the criteria for real-valued functions also apply to each component of a vector-valued function. If each component satisfies the integrability condition, the entire vector-valued function is integrable too.
For instance, assume a proposition (let’s call it Proposition 2') states some condition for the integrability of real-valued functions. If each component of the vector satisfies this criterion individually, then the vector-valued function also satisfies it as a whole.
This principle allows a systematic approach to evaluating the integrability of more complex functions by breaking them down into simpler parts.
Lebesgue Integrability
Lebesgue integration is a powerful method for integrating complex functions. It covers broader types of functions compared to the standard Riemann integration. For vector-valued functions, the Lebesgue integrability condition applies if each component is Lebesgue integrable.
This means each component should be measurable and have a finite integral. If \(f(t)\), \(g(t)\), and \(h(t)\) in the vector \(\langle f(t), g(t), h(t) \rangle\) are all Lebesgue integrable, the vector-valued function is considered integrable under the Lebesgue criterion.
Thus, Lebesgue integration extends the capability to deal with more abstract and varied functional forms, ensuring thorough analysis and application.

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Most popular questions from this chapter

a) Show that if \(f \in \mathcal{R}[a, b]\), then \(|f|^{p} \in \mathcal{R}[a, b]\) for \(p \geq 0\). b) Starting from Hölder's inequality for sums, obtain Hölder's inequality for integrals: \(^{6}\) $$ \left|\int_{a}^{b}(f \cdot g)(x) \mathrm{d} x\right| \leq\left(\int_{a}^{b}|f|^{p}(x) \mathrm{d} x\right)^{1 / p} \cdot\left(\int_{a}^{b}|g|^{q}(x) \mathrm{d} x\right)^{1 / q} $$ if \(f, g \in \mathcal{R}[a, b], p>1, q>1\), and \(\frac{1}{p}+\frac{1}{q}=1\) c) Starting from Minkowski's inequality for sums, obtain Minkowski's inequality for integrals: $$ \left(\int_{a}^{b}|f+g|^{p}(x) \mathrm{d} x\right)^{1 / p} \leq\left(\int_{a}^{b}|f|^{p}(x) \mathrm{d} x\right)^{1 / p}+\left(\int_{a}^{b}|g|^{p}(x) \mathrm{d} x\right)^{1 / p} $$ if \(f, g \in \mathcal{R}[a, b]\) and \(p \geq 1\). Show that this inequality reverses direction if \(0<\) \(p<1\). d) Verify that if \(f\) is a continuous convex function on \(\mathbb{R}\) and \(\varphi\) an arbitrary continuous function on \(\mathbb{R}\), then Jensen's inequality $$ f\left(\frac{1}{c} \int_{0}^{\mathrm{c}} \varphi(t) \mathrm{d} t\right) \leq \frac{1}{c} \int_{0}^{\mathrm{c}} f(\varphi(t)) \mathrm{d} t $$ holds for \(c \neq 0\).

Using the integral, find a) \(\lim _{n \rightarrow \infty}\left[\frac{n}{(n+1)^{2}}+\cdots+\frac{n}{(2 n)^{2}}\right]\); b) \(\lim _{n \rightarrow \infty} \frac{1^{\alpha}+2^{\alpha}+\cdots+n^{\alpha}}{n^{\alpha+1}}\), if \(\alpha \geq 0\).

The Buffon needle problem. \(^{11}\) The number \(\pi\) can be computed in the following rather surprising way. We take a large sheet of paper, ruled into parallel lines a distance \(h\) apart and we toss a needle of length \(l

A wheel of radius \(r\) rolls without slipping over a horizontal plane at a uniform velocity \(v\). Suppose at time \(t=0\) the uppermost point \(A\) of the wheel has coordinates \((0,2 r)\) in a Cartesian coordinate system whose \(x\)-axis lies in the plane and is directed along the velocity vector. a) Write the law of motion \(t \mapsto(x(t), y(t))\) of the point \(A\). b) Find the velocity of \(A\) as a function of time. c) Describe graphically the trajectory of \(A\). (This curve is called a cycloid.) d) Find the length of one arch of the cycloid (the length of one period of this periodic curve). e) The cycloid has a number of interesting properties, one of which, discovered by Huygens \({ }^{10}\) is that the period of oscillation of a cycloidal pendulum (a ball rolling in a cycloidal well) is independent of the height to which it rises above the lowest point of the well. Try to prove this, using Example 9. (See also Problem 6 of the next section, which is devoted to improper integrals.)

Show that if \(f, g \in \mathcal{R}[a, b]\) and \(f\) and \(g\) are real-valued, then \(\max \\{f, g\\} \in\) \(\mathcal{R}[a, b]\) and \(\min \\{f, g\\} \in \mathcal{R}[a, b]\)

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