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Find the unit tangent vector at the given value of t for the following parameterized curves. $$\mathbf{r}(t)=\langle\cos 2 t, 4,3 \sin 2 t\rangle, \text { for } 0 \leq t \leq \pi ; t=\pi / 2$$

Short Answer

Expert verified
Answer: The unit tangent vector at \(t = \frac{\pi}{2}\) is \(\mathbf{T}(t) = \left\langle0, 0, -1\right\rangle\).

Step by step solution

01

Find the derivative of the curve

To find the unit tangent vector, we first need to calculate the derivative of the curve with respect to t. We can do this by finding the derivative of each component function in the parameterized curve. $$ \mathbf{r}(t)=\langle\cos 2t, 4, 3 \sin 2t\rangle $$ Taking the derivative with respect to t, we get: $$ \mathbf{r}'(t)=\left\langle\frac{d}{dt} (\cos 2t), \frac{d}{dt}(4), \frac{d}{dt}(3 \sin 2t)\right\rangle $$ $$ \mathbf{r}'(t)=\left\langle-2 \sin 2t, 0, 6 \cos 2t\right\rangle $$
02

Evaluate the derivative at the given value of t

Now that we have the derivative, we need to evaluate it at the given value of t, which is \(t = \frac{\pi}{2}\). Plugging in this value into the derivative, we get: $$ \mathbf{r}'\left(\frac{\pi}{2}\right) = \left\langle-2 \sin 2\left(\frac{\pi}{2}\right), 0, 6 \cos 2\left(\frac{\pi}{2}\right)\right\rangle $$ $$ \mathbf{r}'\left(\frac{\pi}{2}\right) = \left\langle-2 \sin \pi, 0, 6 \cos \pi\right\rangle $$ $$ \mathbf{r}'\left(\frac{\pi}{2}\right) = \left\langle0, 0, -6\right\rangle $$
03

Find the magnitude of the derivative evaluated at the given value of t

Next, we need to find the magnitude of the derivative vector at \(t = \frac{\pi}{2}\): $$ \|\mathbf{r}'\left(\frac{\pi}{2}\right)\| = \sqrt{(0)^2+(0)^2+(-6)^2} = \sqrt{0+0+36} = \sqrt{36} = 6 $$
04

Find the unit tangent vector

Finally, to find the unit tangent vector, we need to divide the derivative vector evaluated at \(t = \frac{\pi}{2}\) by its magnitude: $$ \mathbf{T}(t) = \frac{\mathbf{r}'\left(\frac{\pi}{2}\right)}{\|\mathbf{r}'\left(\frac{\pi}{2}\right)\|} $$ $$ \mathbf{T}(t) = \frac{\left\langle0, 0, -6\right\rangle}{6} = \left\langle0, 0, -1\right\rangle $$ Thus, the unit tangent vector at \(t = \frac{\pi}{2}\) is \(\mathbf{T}(t) = \left\langle0, 0, -1\right\rangle\).

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Key Concepts

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

Parameterized Curves
When we talk about parameterized curves, we're referring to a way of representing a curve through equations that express each coordinate as a function of a single variable, often denoted as t. These parameterizations are incredibly useful in fields like physics and engineering, where they can describe the path of a moving point over time.

For a curve in three-dimensional space, a parameterization would typically look like: \[\mathbf{r}(t)=\langle f(t), g(t), h(t)\rangle\],where \(f(t)\), \(g(t)\), and \(h(t)\) are the component functions that describe the curve's position along the x, y, and z axes, respectively, given the parameter \(t\). In our exercise, we see a parameterized curve described by \(\mathbf{r}(t)=\langle\cos 2t, 4, 3 \sin 2t\rangle\).

Understanding parameterized curves is fundamental because they provide the foundation to explore other concepts, such as the derivative of a curve and the curvature of the path, which lead to a deeper understanding of the curve's geometry and dynamics.
Derivative of a Curve
Taking the derivative of a curve is one way to explore the curve's behavior. When we differentiate a parameterized curve, we find the rate at which the curve's position changes with respect to the parameter -- often this parameter is time. The derivative of a parameterized curve is a vector that represents the direction and speed of the curve's motion at each point.

In mathematical terms, the derivative of the curve \(\mathbf{r}(t)\) is a vector given by: \[\mathbf{r}'(t)=\left\langle\frac{d}{dt} (f(t)), \frac{d}{dt}(g(t)), \frac{d}{dt}(h(t))\right\rangle\]. Applying this to our exercise, we differentiated each component to get \(\mathbf{r}'(t)=\langle-2 \sin 2t, 0, 6 \cos 2t\rangle\). This derivative describes the instantaneous velocity of a point moving along the curve at any time \(t\), which is essential for finding the unit tangent vector, as is the goal in the given exercise.
Magnitude of a Vector
The magnitude of a vector is a measure of its length. In a geometric sense, if you were to draw the vector as an arrow, the magnitude would be the length of this arrow. Mathematically, you can find the magnitude of a vector \(\mathbf{v}=\langle v_x, v_y, v_z \rangle\) with the formula:\[\|\mathbf{v}\| = \sqrt{v_x^2 + v_y^2 + v_z^2}\].

In the context of our problem, we calculated the magnitude of the derivative of the curve to be 6, using the vector from step 2. This is critical for computing the unit tangent vector, which requires us to normalize the derivative vector by its magnitude—suggesting division by the scalar value representing the vector's length. Thus, the magnitude gives us a crucial bridge from the raw directional information of the derivative to the refined directional guidance of the unit vector that points tangentially along the curve.

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Most popular questions from this chapter

Hexagonal circle packing The German mathematician Gauss proved that the densest way to pack circles with the same radius in the plane is to place the centers of the circles on a hexagonal grid (see figure). Some molecular structures use this packing or its three-dimensional analog. Assume all circles have a radius of 1 and let \(\mathbf{r}_{i j}\) be the vector that extends from the center of circle \(i\) to the center of circle \(j,\) for \(i, j=0,1, \ldots, 6\) a. Find \(\mathbf{r}_{0 j},\) for \(j=1,2, \ldots, 6\) b. Find \(\mathbf{r}_{12}, \mathbf{r}_{34},\) and \(\mathbf{r}_{61}\) c. Imagine circle 7 is added to the arrangement as shown in the figure. Find \(\mathbf{r}_{07}, \mathbf{r}_{17}, \mathbf{r}_{47},\) and \(\mathbf{r}_{75}\)

Suppose the vector-valued function \(\mathbf{r}(t)=\langle f(t), g(t), h(t)\rangle\) is smooth on an interval containing the point \(t_{0} .\) The line tangent to \(\mathbf{r}(t)\) at \(t=t_{0}\) is the line parallel to the tangent vector \(\mathbf{r}^{\prime}\left(t_{0}\right)\) that passes through \(\left(f\left(t_{0}\right), g\left(t_{0}\right), h\left(t_{0}\right)\right) .\) For each of the following functions, find an equation of the line tangent to the curve at \(t=t_{0} .\) Choose an orientation for the line that is the same as the direction of \(\mathbf{r}^{\prime}\). $$\mathbf{r}(t)=\left\langle e^{t}, e^{2 t}, e^{3 t}\right\rangle ; t_{0}=0$$

Motion on a sphere Prove that \(\mathbf{r}\) describes a curve that lies on the surface of a sphere centered at the origin \(\left(x^{2}+y^{2}+z^{2}=a^{2}\right.\) with \(a \geq 0\) ) if and only if \(\mathbf{r}\) and \(\mathbf{r}^{\prime}\) are orthogonal at all points of the curve.

Suppose water flows in a thin sheet over the \(x y\) -plane with a uniform velocity given by the vector \(\mathbf{v}=\langle 1,2\rangle ;\) this means that at all points of the plane, the velocity of the water has components \(1 \mathrm{m} / \mathrm{s}\) in the \(x\) -direction and \(2 \mathrm{m} / \mathrm{s}\) in the \(y\) -direction (see figure). Let \(C\) be an imaginary unit circle (that does not interfere with the flow). a. Show that at the point \((x, y)\) on the circle \(C\), the outwardpointing unit vector normal to \(C\) is \(\mathbf{n}=\langle x, y\rangle\) b. Show that at the point \((\cos \theta, \sin \theta)\) on the circle \(C,\) the outwardpointing unit vector normal to \(C\) is also \(\mathbf{n}=\langle\cos \theta, \sin \theta\rangle\) c. Find all points on \(C\) at which the velocity is normal to \(C\). d. Find all points on \(C\) at which the velocity is tangential to \(C\). e. At each point on \(C\), find the component of \(\mathbf{v}\) normal to \(C\). Express the answer as a function of \((x, y)\) and as a function of \(\theta\) f. What is the net flow through the circle? That is, does water accumulate inside the circle?

Use vectors to show that the midpoint of the line segment joining \(P\left(x_{1}, y_{1}\right)\) and \(Q\left(x_{2}, y_{2}\right)\) is the point \(\left(\frac{x_{1}+x_{2}}{2}, \frac{y_{1}+y_{2}}{2}\right)\) (Hint: Let \(O\) be the origin and let \(M\) be the midpoint of \(P Q\). Draw a picture and show that $$\left.\overrightarrow{O M}=\overrightarrow{O P}+\frac{1}{2} \overrightarrow{P Q}=\overrightarrow{O P}+\frac{1}{2}(\overrightarrow{O Q}-\overrightarrow{O P}) \cdot\right)$$

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