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Find \(\mathbf{T}, \mathbf{N},\) and \(\kappa\) for the plane curves in Exercises. $$\mathbf{r}(t)=(\cos t+t \sin t) \mathbf{i}+(\sin t-t \cos t) \mathbf{j}, \quad t > 0$$

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The main derivative step is done.

Step by step solution

01

Find the Derivative of r(t)

To find the tangent vector \( \mathbf{T} \), start by finding the derivative of the vector function \( \mathbf{r}(t) \). The derivative, \( \mathbf{r}'(t) \), is obtained by taking the derivative of each component. For \( \mathbf{r}(t) = (\cos t + t \sin t) \mathbf{i} + (\sin t - t \cos t) \mathbf{j} \), we have:\( \mathbf{r}'(t) = (- \sin t + \sin t + t \cos t) \mathbf{i} + (\cos t - \cos t + t \sin t) \mathbf{j} \).Simplifying gives:\( \mathbf{r}'(t) = t \cos t \mathbf{i} + t \sin t \mathbf{j} \).

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Key Concepts

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

Curvature
Curvature is a way to measure how much a curve deviates from being a straight line—or, in simpler terms, how "curvy" it is. For a plane curve defined by a vector function \( \mathbf{r}(t) \), the curvature, denoted \( \kappa \), quantifies how sharply the curve bends at a given point. Calculating curvature involves several steps:
  • First, find the tangent vector \( \mathbf{T}(t) \), which is the unit vector in the direction of the derivative \( \mathbf{r}'(t) \).
  • The curvature is given by \( \kappa = \frac{| \mathbf{T}'(t) |}{| \mathbf{r}'(t) |} \).

This formula considers the rate of change of the tangent vector's direction with respect to the arc length of the curve. This is critical in ensuring the curvature measures only how the direction changes, not how fast we move through the curve.
Unit Normal Vector
The unit normal vector, \( \mathbf{N}(t) \), is a vector that is perpendicular to the tangent vector of a curve at a given point. It provides significant insights into the direction in which the curve is bending at that specific point.To find the unit normal vector, follow these steps:
  • First, compute the derivative of the tangent vector, \( \mathbf{T}'(t) \).
  • Normalize \( \mathbf{T}'(t) \) by dividing it by its magnitude to ensure it has a length of 1: \( \mathbf{N}(t) = \frac{\mathbf{T}'(t)}{|\mathbf{T}'(t)|} \).

By doing this, you obtain the unit normal vector which points towards the center of the curve's osculating (curvature-defining) circle, helping us understand the inherent geometry of the curve better.
Derivative
The derivative is a fundamental concept in calculus that measures the rate of change of a function. For a given vector function \( \mathbf{r}(t) \), the derivative, \( \mathbf{r}'(t) \), provides us with the velocity vector, indicating the direction and rate at which the position vector is changing.When dealing with curves, the derivative helps in finding:
  • The velocity of a moving point on the curve.
  • The tangent vector by normalizing the velocity vector.

In our exercise, finding the derivative of \( \mathbf{r}(t) \) involves differentiating each component separately. Given \( \mathbf{r}(t) = (\cos t + t \sin t) \mathbf{i} + (\sin t - t \cos t) \mathbf{j} \), the derivative becomes \( \mathbf{r}'(t) = t \cos t \mathbf{i} + t \sin t \mathbf{j} \). This results in a simpler expression, reflecting the instantaneous rate at which the position on the curve changes, and forms the first step in understanding further properties like the tangent vector, curvature, and unit normal vector.

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Most popular questions from this chapter

\(\mathbf{r}(t)\) is the position of a particle in space at time \(t\) Find the particle's velocity and acceleration vectors. Then find the particle's speed and direction of motion at the given value of \(t .\) Write the particle's velocity at that time as the product of its speed and direction. $$\mathbf{r}(t)=\left(e^{-\eta} \mathbf{i}+(2 \cos 3 t) \mathbf{j}+(2 \sin 3 t) \mathbf{k}, \quad t=0\right.$$

Projectile flights in the following exercises are to be treated as ideal unless stated otherwise. All launch angles are assumed to be measured from the horizontal. All projectiles are assumed to be launched from the origin over a horizontal surface unless stated otherwise. Beaming electrons An electron in a TV tube is beamed horizontally at a speed of \(5 \times 10^{6} \mathrm{m} /\) sec toward the face of the tube \(40 \mathrm{cm}\) away. About how far will the electron drop before it hits?

The formula $$ \kappa(x)=\frac{\left|f^{\prime \prime}(x)\right|}{\left[1+\left(f^{\prime}(x)\right)^{2}\right]^{3 / 2}} $$ derived in Exercise \(5,\) expresses the curvature \(\kappa(x)\) of a twice- differentiable plane curve \(y=f(x)\) as a function of \(x .\) Find the curvature function of each of the curves. Then graph \(f(x)\) together with \(\kappa(x)\) over the given interval. You will find some surprises. $$y=e^{x}, \quad-1 \leq x \leq 2$$

In Exercises \(1-8,\) find the curve's unit tangent vector. Also, find the length of the indicated portion of the curve. $$\mathbf{r}(t)=(t \cos t) \mathbf{i}+(t \sin t) \mathbf{j}+(2 \sqrt{2} / 3) t^{3 / 2} \mathbf{k}, \quad 0 \leq t \leq \pi$$

Find an equation for the circle of curvature of the curve \(\mathbf{r}(t)=\) \((2 \ln t) \mathbf{i}-[t+(1 / t)] \mathbf{j}, e^{-2} \leq t \leq e^{2},\) at the point (0,-2) where \(t=1\)

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