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Find the curvature \(K\) of the curve. $$ \mathbf{r}(t)=\langle a(\omega t-\sin \omega t), a(1-\cos \omega t)\rangle $$

Short Answer

Expert verified
The curvature \(K(t)\) of the curve is given by \(\frac{\sqrt{(\omega t - \sin \omega t)^2 + (\cos \omega t)^2}}{a^2\omega}\)

Step by step solution

01

Find the derivative of the vector function

First, we must compute the derivative of the vector function \(\mathbf{r}\), which is given by: \(\mathbf{r}'(t) = \langle a\omega(1-\cos \omega t), a\omega \sin \omega t\rangle\)
02

Calculate the second derivative of the vector function

Next, we calculate the second derivative of the vector function \(\mathbf{r}\), which should yield: \(\mathbf{r}''(t) = \langle -a\omega^2(\omega t - \sin \omega t), -a\omega^2(\cos \omega t)\rangle\)
03

Find the norm of both derivatives

Compute the magnitudes of the first and second derivative vectors. We know that the magnitude (or norm) of a vector \(\mathbf{a} = \langle x,y \rangle\) is \(\|\mathbf{a}\| = \sqrt{x^2 + y^2}\), Thus, \(|\mathbf{r}'(t)| = a\omega\) and \(|\mathbf{r}''(t)| = a\omega^2\sqrt{(\omega t - \sin \omega t)^2 + (\cos \omega t)^2}\).
04

Find the curvature of the curve

Finally, substituting the magnitudes of the first and second derivative into the curvature formula will yield \(K(t) = \frac{|\mathbf{r}''(t)|}{|\mathbf{r}'(t)|^3} = \frac{a\omega^2\sqrt{(\omega t - \sin \omega t)^2 + (\cos \omega t)^2}}{a^3\omega^3} = \frac{\sqrt{(\omega t - \sin \omega t)^2 + (\cos \omega t)^2}}{a^2\omega}\).

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Key Concepts

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

Vector Function Derivatives
When dealing with the motion of an object along a path, a vector function can represent the object's position as a function of time. In calculus, finding the derivative of a vector function is similar to finding the derivative of a standard function, but with the difference that each component of the vector is differentiated independently.

The derivative of the vector function \( \mathbf{r}(t) \) tells us about the object's velocity. For our curve \( \mathbf{r}(t) = \langle a(\omega t - \sin \omega t), a(1 - \cos \omega t) \rangle \), the first derivative \( \mathbf{r}'(t) \) signifies the instantaneous rate of change of the position, which provides information about how fast and in what direction the object is moving at any given time. In applications, understanding these derivatives is essential for predicting future positions and velocities of moving objects.
Norm of a Vector
The norm or magnitude of a vector is a measure of its length and is found by taking the square root of the sum of the squares of its components. It is denoted by \( \|\mathbf{a}\| \) for a vector \(\mathbf{a} \) with components \( x \) and \( y \) such that \( \mathbf{a} = \langle x, y \rangle \). The norm is calculated as \( \|\mathbf{a}\| = \sqrt{x^2 + y^2} \).

The concept of norm is crucial in many areas of mathematics and physics, as it quantifies the size of vectors – a fundamental concept when analyzing forces, velocities, and other vector quantities. When calculating curvature, the norm of the derivative vectors represents the speed of an object moving along the curve, which is necessary to determine how sharply the curve bends at each point.
Calculus in Motion
Calculus plays a pivotal role in describing and understanding motion. When studying the curvature of a curve, calculus offers tools to measure how an object's path bends and twists in space. To quantify this, we cannot solely rely on the object's position \( \mathbf{r}(t) \) – we also need its derivatives.

The curvature \( K \) of a curve at a given point, which is a good indicator of how rapidly the curve is changing direction at that point, is found using the derivatives. It tells us the rate of change of the tangent vector to the curve, providing insights into the curve's geometry and an object's trajectory. In essence, calculus equips us with the methods to analyze dynamic systems and the motion of an object along a curve, which is a cornerstone concept in disciplines such as physics, engineering, and robotics.

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Most popular questions from this chapter

In Exercises \(27-34,\) find the open interval(s) on which the curve given by the vector-valued function is smooth. $$ \mathbf{r}(t)=t^{2} \mathbf{i}+t^{3} \mathbf{j} $$

A projectile is launched with an initial velocity of 100 feet per second at a height of 5 feet and at an angle of \(30^{\circ}\) with the horizontal. (a) Determine the vector-valued function for the path of the projectile. (b) Use a graphing utility to graph the path and approximate the maximum height and range of the projectile. (c) Find \(\mathbf{v}(t),\|\mathbf{v}(t)\|,\) and \(\mathbf{a}(t)\) (d) Use a graphing utility to complete the table. $$ \begin{array}{|l|l|l|l|l|l|l|} \hline \boldsymbol{t} & 0.5 & 1.0 & 1.5 & 2.0 & 2.5 & 3.0 \\ \hline \text { Speed } & & & & & & \\ \hline \end{array} $$ (e) Use a graphing utility to graph the scalar functions \(a_{\mathbf{T}}\) and \(a_{\mathrm{N}} .\) How is the speed of the projectile changing when \(a_{\mathrm{T}}\) and \(a_{\mathbf{N}}\) have opposite signs?

Prove the property. In each case, assume that \(\mathbf{r}, \mathbf{u},\) and \(\mathbf{v}\) are differentiable vector-valued functions of \(t,\) \(f\) is a differentiable real-valued function of \(t,\) and \(c\) is a scalar. $$ \begin{array}{l} D_{t}\\{\mathbf{r}(t) \cdot[\mathbf{u}(t) \times \mathbf{v}(t)]\\}=\mathbf{r}^{\prime}(t) \cdot[\mathbf{u}(t) \times \mathbf{v}(t)]+ \\ \mathbf{r}(t) \cdot\left[\mathbf{u}^{\prime}(t) \times \mathbf{v}(t)\right]+\mathbf{r}(t) \cdot\left[\mathbf{u}(t) \times \mathbf{v}^{\prime}(t)\right] \end{array} $$

Use the model for projectile motion, assuming there is no air resistance. A baseball, hit 3 feet above the ground, leaves the bat at an angle of \(45^{\circ}\) and is caught by an outfielder 3 feet above the ground and 300 feet from home plate. What is the initial speed of the ball, and how high does it rise?

Consider a particle moving on a circular path of radius \(b\) described by $$ \begin{aligned} &\mathbf{r}(t)=b \cos \omega t \mathbf{i}+b \sin \omega t \mathbf{j}\\\ &\text { where } \omega=d \theta / d t \text { is the constant angular velocity. } \end{aligned} $$ (a) Show that the speed of the particle is \(b \omega\). (b) Use a graphing utility in parametric mode to graph the circle for \(b=6\). Try different values of \(\omega\). Does the graphing utility draw the circle faster for greater values of \(\omega\) ?

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