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In Exercises \(1-8,\) find the curve's unit tangent vector. Also, find the length of the indicated portion of the curve. $$ \mathbf{r}(t)=(t \sin t+\cos t) \mathbf{i}+(t \cos t-\sin t) \mathbf{j}, \quad \sqrt{2} \leq t \leq 2 $$

Short Answer

Expert verified
The unit tangent vector is \( \mathbf{T}(t) = (\cos t) \mathbf{i} - (\sin t) \mathbf{j} \), and the length of the curve is 1.

Step by step solution

01

Find the Derivative of the Curve

First, compute the derivative of the vector function \( \mathbf{r}(t) = (t \sin t + \cos t) \mathbf{i} + (t \cos t - \sin t) \mathbf{j} \). The derivative \( \mathbf{r}'(t) \) is found by differentiating each component separately: \[\frac{d}{dt}(t \sin t + \cos t) = \sin t + t \cos t - \sin t = t \cos t\]\[\frac{d}{dt}(t \cos t - \sin t) = \cos t - t \sin t - \cos t = -t \sin t\]Thus, \( \mathbf{r}'(t) = (t \cos t) \mathbf{i} + (-t \sin t) \mathbf{j} \).
02

Compute the Magnitude of the Derivative

Calculate the magnitude of the derivative \( \mathbf{r}'(t) = (t \cos t) \mathbf{i} + (-t \sin t) \mathbf{j} \). The magnitude is given by:\[\|\mathbf{r}'(t)\| = \sqrt{(t \cos t)^2 + (-t \sin t)^2} = \sqrt{t^2 \cos^2 t + t^2 \sin^2 t}\]Using the identity \( \cos^2 t + \sin^2 t = 1 \), this simplifies to:\[\|\mathbf{r}'(t)\| = \sqrt{t^2 (\cos^2 t + \sin^2 t)} = \sqrt{t^2} = |t|\].
03

Calculate the Unit Tangent Vector

The unit tangent vector \( \mathbf{T}(t) \) is obtained by dividing \( \mathbf{r}'(t) \) by its magnitude:\[\mathbf{T}(t) = \frac{\mathbf{r}'(t)}{\|\mathbf{r}'(t)\|} = \frac{(t \cos t) \mathbf{i} + (-t \sin t) \mathbf{j}}{|t|}\]For \(t > 0\), this simplifies to: \[\mathbf{T}(t) = (\cos t) \mathbf{i} + (-\sin t) \mathbf{j}\].
04

Determine the Length of the Curve

The arc length \( S \) from \( t = \sqrt{2} \) to \( t = 2 \) is found by integrating the magnitude of the derivative over the given interval:\[S = \int_{\sqrt{2}}^2 \|\mathbf{r}'(t)\| \, dt = \int_{\sqrt{2}}^2 |t| \, dt\]Since \(t > 0\) throughout the interval, it simplifies to:\[S = \int_{\sqrt{2}}^2 t \, dt\]Compute the integral:\[= \left[ \frac{1}{2} t^2 \right]_{\sqrt{2}}^2 = \left(\frac{1}{2} (2)^2 \right) - \left(\frac{1}{2} (\sqrt{2})^2 \right)\]\[= 2 - 1 = 1\]Thus, the length of the curve is 1.

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Key Concepts

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

Arc Length
The concept of arc length is essential in understanding the actual distance along a curve, as opposed to the straight-line distance between two points. In mathematics, arc length gives us a way to measure the extent of a curve over a specific interval. When working with parametric equations or vector functions, the arc length can be calculated using an integral.
To find the arc length, we integrate the magnitude of the derivative of the function over the given interval. This means taking the derivative of the position vector, finding its magnitude, and then integrating this value with respect to the parameter, usually denoted as 't'. In our example, the arc length from the given curve is computed over the interval \( \sqrt{2} \) to 2, and it turns out to be 1.
Understanding arc length can greatly enhance your comprehension of concepts in calculus and physics, as it relates to real-world application scenarios like distances traveled or materials used in physical structures.
Vector Calculus
Vector calculus is a branch of mathematics that deals with vectors rather than just numbers. It's central to physics and engineering as it provides tools to model three-dimensional problems. Vectors have both magnitude and direction, and vector calculus uses them to describe movements or forces in space.
In vector calculus, we work with operations like differentiation and integration in multiple dimensions. The example function given, \( \mathbf{r}(t) \), describes a path in a two-dimensional plane, with each component of the vector dependent on the parameter \( t \).
Understanding how to manipulate vector functions and calculate their derivatives, magnitudes, and integrals can help solve complex problems, such as finding the direction or length of a curve within a multi-dimensional space.
Derivative of Vector Functions
The derivative of a vector function involves differentiating each of its components separately. This concept is critical in vector calculus and is used to determine the rate at which vector quantities change.
For a vector function \( \mathbf{r}(t) = (x(t), y(t)) \), the derivative \( \mathbf{r}'(t) \) is \( (x'(t), y'(t)) \). Each component is differentiated individually with respect to \( t \). In our example, \( t \sin t + \cos t \) and \( t \cos t - \sin t \) are differentiated separately. The derivative helps in understanding the motion along the path or curve the function represents.
Calculating the derivative is a step towards finding other important properties like the unit tangent vector and can also be instrumental in motion dynamics, optimizing trajectories, or analyzing forces.
Unit Vector
A unit vector is a vector of length 1, used to indicate direction. In vector calculus, unit vectors help in identifying the orientation of lines or curves at a specific point.
To find a unit tangent vector, we first determine the derivative of the vector function to get the tangent vector. We then divide this vector by its magnitude to create a unit vector. This process normalizes the vector, changing its length to 1 while preserving its direction.
In our example, after calculating the derivative, \( \mathbf{r}'(t) \), we computed its magnitude \( \| \mathbf{r}'(t) \| \), and then divided \( \mathbf{r}'(t) \) by this magnitude to obtain the unit tangent vector \( \mathbf{T}(t) \). This unit vector provides insight into the direction of the curve at each point, which is particularly useful in physics for understanding motion and directionality.

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Most popular questions from this chapter

Component Test for Continuity at a Point Show that the vector function \(\mathbf{r}\) defined by \(\mathbf{r}(t)=f(t) \mathbf{i}+g(t) \mathbf{j}+h(t) \mathbf{k}\) is continuous at \(t=t_{0}\) if and only if \(f, g,\) and \(h\) are continuous at \(t_{0} .\)

Evaluate the integrals in Exercises \(21-26\) $$ \int_{1}^{2}\left[(6-6 t) \mathbf{i}+3 \sqrt{t} \mathbf{j}+\left(\frac{4}{t^{2}}\right) \mathbf{k}\right] d t $$

The torsion of a helix In Example \(2,\) we found the torsion of the helix $$ \mathbf{r}(t)=(a \cos t) \mathbf{i}+(a \sin t) \mathbf{j}+b t \mathbf{k}, \quad a, b \geq 0 $$ to be \(\tau=b /\left(a^{2}+b^{2}\right) .\) What is the largest value \(\tau\) can have for a given value of \(a ?\) Give reasons for your answer.

In Exercises 16 and \(17,\) two planets, planet \(A\) and planet \(B\) , are orbiting their sun in circular orbits with \(A\) being the inner planet and \(B\) being farther away from the sun. Suppose the positions of \(A\) and \(B\) at time \(t\) are $$ \mathbf{r}_{A}(t)=2 \cos (2 \pi t) \mathbf{i}+2 \sin (2 \pi t) \mathbf{j} $$ and $$ \mathbf{r}_{B}(t)=3 \cos (\pi t) \mathbf{i}+3 \sin (\pi t) \mathbf{j} $$ respectively, where the sun is assumed to be located at the origin and distance is measured in astronomical units. (Notice that planet \(A\) moves faster than planet \(B . )\) The people on planet \(A\) regard their planet, not the sun, as the center of their planetary system (their solar system). Using planet \(A\) as the origin, graph the path of planet \(B .\) This exercise illustrates the difficulty that people before Kepler's time, with an earth- centered (planet \(A\) ) view of our solar system, had in understanding the motions of the planets (i.e., planet \(B=\) Mars). See D. G. Saari's article in the American Mathematical Monthly, Vol. 97 (Feb. \(1990 ),\) pp. \(105-119\) .

Solve the initial value problems in Exercises \(27-32\) for \(r\) as a vector function of \(t .\) $$ \begin{array}{ll}{\text { Differential equation: }} & {\frac{d \mathbf{r}}{d t}=-t \mathbf{i}-t \mathbf{j}-t \mathbf{k}} \\ {\text { Initial condition: }} & {\mathbf{r}(0)=\mathbf{i}+2 \mathbf{j}+3 \mathbf{k}}\end{array} $$

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