Chapter 3: Problem 219
Reparameterize the following functions with respect to their arc length measured from \(t=0\) in direction of increasing \(t .\) $$ \mathbf{r}(t)=\cos (2 t) \mathbf{i}+8 t \mathbf{j}-\sin (2 t) \mathbf{k} $$
Short Answer
Expert verified
The reparameterized function is \(\mathbf{r}(s) = \cos\left(\frac{s}{\sqrt{17}}\right)\mathbf{i} + \frac{4s}{\sqrt{17}}\mathbf{j} - \sin\left(\frac{s}{\sqrt{17}}\right)\mathbf{k}\).
Step by step solution
01
Find the derivative of the vector function
The first step is to find the derivative of the vector function \( \mathbf{r}(t) \). For \( \mathbf{r}(t) = \cos(2t) \mathbf{i} + 8t \mathbf{j} - \sin(2t) \mathbf{k} \), we differentiate each component with respect to \( t \):\[ \mathbf{r}'(t) = \frac{d}{dt}[\cos(2t)] \mathbf{i} + \frac{d}{dt}[8t] \mathbf{j} - \frac{d}{dt}[\sin(2t)] \mathbf{k} \]This gives us:\[ \mathbf{r}'(t) = -2\sin(2t) \mathbf{i} + 8 \mathbf{j} - 2\cos(2t) \mathbf{k} \]
02
Calculate the magnitude of the derivative
The next step is to calculate the magnitude of the derivative \( \mathbf{r}'(t) \). This gives us the speed of the particle along the curve:\[ \| \mathbf{r}'(t) \| = \sqrt{[ -2\sin(2t)]^2 + 8^2 + [-2\cos(2t)]^2} \]Which simplifies to:\[ \| \mathbf{r}'(t) \| = \sqrt{4\sin^2(2t) + 64 + 4\cos^2(2t)} \]Using the identity \( \sin^2(\theta) + \cos^2(\theta) = 1 \), we simplify further:\[ \| \mathbf{r}'(t) \| = \sqrt{4(\sin^2(2t) + \cos^2(2t)) + 64} = \sqrt{68} = 2\sqrt{17} \]
03
Set up the arc length parameterization equation
The arc length \( s \) from \( t = 0 \) is given by the integral of the speed:\[ s(t) = \int_{0}^{t} \| \mathbf{r}'(u) \| \, du \]Substituting the speed \( \| \mathbf{r}'(u) \| = 2\sqrt{17} \), we have:\[ s(t) = \int_{0}^{t} 2\sqrt{17} \, du = 2\sqrt{17} \cdot t \]
04
Solve for the parameter \( t \) in terms of \( s \)
We need to express \( t \) in terms of \( s \) to reparameterize the function by arc length:\[ s = 2\sqrt{17} \cdot t \]Solving for \( t \), we get:\[ t = \frac{s}{2\sqrt{17}} \]
05
Substitute \( t \) back into the original function
To complete the reparameterization, substitute \( t = \frac{s}{2\sqrt{17}} \) back into \( \mathbf{r}(t) \):\[ \mathbf{r}(s) = \cos\left(2 \cdot \frac{s}{2\sqrt{17}}\right)\mathbf{i} + 8\left(\frac{s}{2\sqrt{17}}\right)\mathbf{j} - \sin\left(2\cdot\frac{s}{2\sqrt{17}}\right)\mathbf{k} \]This simplifies to:\[ \mathbf{r}(s) = \cos\left(\frac{s}{\sqrt{17}}\right)\mathbf{i} + \frac{4s}{\sqrt{17}}\mathbf{j} - \sin\left(\frac{s}{\sqrt{17}}\right)\mathbf{k} \]
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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 branch of mathematics that deals with vector functions and various operations that can be performed on these functions. A vector function generally depends on one or more variables, such as time, to describe a mathematical model.
In simple terms, it takes a real number and gives us a vector. These functions help in describing objects' motion along paths or surfaces. They visualize complex phenomena like weather patterns, electromagnetic fields, or fluid dynamics in engineering.
Common operations include:
In simple terms, it takes a real number and gives us a vector. These functions help in describing objects' motion along paths or surfaces. They visualize complex phenomena like weather patterns, electromagnetic fields, or fluid dynamics in engineering.
Common operations include:
- Derivatives: Measures the rate of change of vector components.
- Integrals: Summarize changes over an interval to calculate the net effect.
Derivative
The derivative in vector calculus helps understand how a vector function changes as its input variable changes—essentially, the vector's rate of change.
For a vector function \( \mathbf{r}(t) = \cos(2t) \mathbf{i} + 8t \mathbf{j} - \sin(2t) \mathbf{k} \), calculating its derivative involves differentiating each component separately:
\[ \mathbf{r}'(t) = -2\sin(2t) \mathbf{i} + 8 \mathbf{j} - 2\cos(2t) \mathbf{k} \]
Here's how it breaks down:
For a vector function \( \mathbf{r}(t) = \cos(2t) \mathbf{i} + 8t \mathbf{j} - \sin(2t) \mathbf{k} \), calculating its derivative involves differentiating each component separately:
\[ \mathbf{r}'(t) = -2\sin(2t) \mathbf{i} + 8 \mathbf{j} - 2\cos(2t) \mathbf{k} \]
Here's how it breaks down:
- The derivative of \cos(2t) is \-2\sin(2t).
- The derivative of 8t is 8.
- The derivative of \-\sin(2t) is \-2\cos(2t).
Magnitude of a Vector
The magnitude of a vector gives us the "size" or length of the vector but not the direction. It is calculated using Euclidean distance in multi-dimensional space.
For the derivative \( \mathbf{r}'(t) = -2\sin(2t) \mathbf{i} + 8 \mathbf{j} - 2\cos(2t) \mathbf{k} \), the magnitude is computed as:
\[ \| \mathbf{r}'(t) \| = \sqrt{[ -2\sin(2t)]^2 + 8^2 + [-2\cos(2t)]^2} \]
Simplifying this expression using the identity \( \sin^2( heta) + \cos^2( heta) = 1 \), we get:
\[ \| \mathbf{r}'(t) \| = \sqrt{68} = 2\sqrt{17} \]
This magnitude is crucial as it represents the "speed" of the trajectory described by the vector function, which is constant along the curve at \( 2\sqrt{17} \). Understanding the magnitude aids in reparameterizing the function with respect to arc length.
For the derivative \( \mathbf{r}'(t) = -2\sin(2t) \mathbf{i} + 8 \mathbf{j} - 2\cos(2t) \mathbf{k} \), the magnitude is computed as:
\[ \| \mathbf{r}'(t) \| = \sqrt{[ -2\sin(2t)]^2 + 8^2 + [-2\cos(2t)]^2} \]
Simplifying this expression using the identity \( \sin^2( heta) + \cos^2( heta) = 1 \), we get:
\[ \| \mathbf{r}'(t) \| = \sqrt{68} = 2\sqrt{17} \]
This magnitude is crucial as it represents the "speed" of the trajectory described by the vector function, which is constant along the curve at \( 2\sqrt{17} \). Understanding the magnitude aids in reparameterizing the function with respect to arc length.
Integral of a Vector Function
Integration in vector calculus is used to find quantities accumulated over intervals, such as total distance traveled by a path.
When calculating arc length, the integral sums the magnitudes of the derivative over the interval:
\[ s(t) = \int_{0}^{t} \| \mathbf{r}'(u) \| \, du \]
For a constant magnitude \( \| \mathbf{r}'(u) \| = 2\sqrt{17} \), the integration simplifies to a linear result:
\[ s(t) = 2\sqrt{17} \cdot t \]
This tells us the arc length from the starting point to any point \( t \) on the curve, providing essential data for the reparameterization process.
Through integration, we can understand how the entire curve is formed over time and can adjust the parameter \( t \) to \( s \), ensuring the path's description aligns with the physical distance traveled.
When calculating arc length, the integral sums the magnitudes of the derivative over the interval:
\[ s(t) = \int_{0}^{t} \| \mathbf{r}'(u) \| \, du \]
For a constant magnitude \( \| \mathbf{r}'(u) \| = 2\sqrt{17} \), the integration simplifies to a linear result:
\[ s(t) = 2\sqrt{17} \cdot t \]
This tells us the arc length from the starting point to any point \( t \) on the curve, providing essential data for the reparameterization process.
Through integration, we can understand how the entire curve is formed over time and can adjust the parameter \( t \) to \( s \), ensuring the path's description aligns with the physical distance traveled.