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Find parametric equations of the line tangent to the graph of \(\mathbf{r}(t)\) at the point where \(t=t_{0}\). $$ \mathbf{r}(t)=\ln t \mathbf{i}+e^{-t} \mathbf{j}+t^{3} \mathbf{k} ; t_{0}=2 $$

Short Answer

Expert verified
The tangent line has parametric equations: \( x=\ln 2 + \frac{1}{2}s, y=\frac{1}{e^2} - e^{-2}s, z=8 + 12s \)."}

Step by step solution

01

Differentiate the Vector Function

First, we find the derivative of \( \mathbf{r}(t) \). This derivative \( \mathbf{r'}(t) \) gives us the direction of the tangent line. For \( \mathbf{r}(t) = \ln t \mathbf{i} + e^{-t} \mathbf{j} + t^3 \mathbf{k} \), the derivative is found by taking the derivative of each component separately:1. \( \frac{d}{dt}(\ln t) = \frac{1}{t} \)2. \( \frac{d}{dt}(e^{-t}) = -e^{-t} \)3. \( \frac{d}{dt}(t^3) = 3t^2 \)Thus, \( \mathbf{r'}(t) = \frac{1}{t} \mathbf{i} - e^{-t} \mathbf{j} + 3t^2 \mathbf{k} \).

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Key Concepts

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

Tangent Line
When studying curves in space, the tangent line is a crucial concept that helps us understand how a curve behaves at a specific point. Imagine gently touching a curve at a point with a straight line. This straight line is what we call the tangent line. It just 'kisses' the curve at one point, aiming to represent its direction without actually crossing it.
The role of a tangent line is essential when analyzing the motion along a path described by parametric equations. In general, at a given point corresponding to a parameter value, the tangent line shows the immediate direction in which the curve is headed.
To find a tangent line for a parametric curve, we need both a point on the curve and the direction of the line. The direction is given by the derivative of the parametric equation, which acts as the slope in its vector form. Once we have this information, constructing the equation of a tangent line becomes straightforward: using the point-direction form.The general formula for the tangent line to a vector function at parameter value \( t_0 \) is:
  • The point is \( \mathbf{r}(t_0) \).
  • The direction vector is \( \mathbf{r'}(t_0) \)
  • The equation becomes \( ext{Tangent line}(t) = \mathbf{r}(t_0) + \mathbf{r'}(t_0)(t-t_0) \),
with \( t \) a parameter that can vary to give the complete set of lines tangent to the curve.
Vector Function
A vector function is a powerful mathematical tool that describes curves in a multi-dimensional space. Instead of just providing a single output value like scalar functions do, vector functions give us a vector, which contains multiple components.
These components align with each of the coordinate axes of the space in question, allowing for the description of a path or trajectory. In mathematical notation, we often express a vector function as \( \mathbf{r}(t) = f(t) \mathbf{i} + g(t) \mathbf{j} + h(t) \mathbf{k} \), where \( f(t) \), \( g(t) \), and \( h(t) \) are the parametric forms for each coordinate.
For example, in three-dimensional space (3D), the vector function \( \mathbf{r}(t) \) can describe the motion of an object following a specific path. It tells you exactly where the object is in terms of its x, y, and z components at any time \( t \). Terrific, right?Usage in Calculus:
  • It connects calculus with geometry by letting you take derivatives and integrals.
  • These operations allow us to find velocities, accelerations, and other time-related phenomena.
For example, in the given exercise, the vector function \( \mathbf{r}(t) \) describes a 3D curve with natural log, exponential decay, and cubic growth.
Derivative
A derivative is a fundamental tool in calculus and is used to measure how a function changes as its input changes. It's essentially a measure of a function's rate of change or, more simply put, its slope.
Learning to differentiate a vector function means finding a new vector function that tells us the instantaneous rate of change of the original vector function's components.In single-variable calculus, the derivative of a function at a point gives the slope of the tangent line to the function's graph at that point. Similarly, for a vector function \( \mathbf{r}(t) \), the derivative \( \mathbf{r'}(t) \) gives a vector showing the curve's direction or velocity at each point.
Consider an exercise involving the vector function \( \mathbf{r}(t) = \ln t \mathbf{i} + e^{-t} \mathbf{j} + t^3 \mathbf{k} \). Its derivative \( \mathbf{r'}(t) \) is found by differentiating each component:
  • The derivative of \( \ln t \) with respect to \( t \) is \( \frac{1}{t} \).
  • The derivative of \( e^{-t} \) is \( -e^{-t} \).
  • The derivative of \( t^3 \) is \( 3t^2 \).
Thus, the derivative \( \mathbf{r'}(t) = \frac{1}{t} \mathbf{i} - e^{-t} \mathbf{j} + 3t^2 \mathbf{k} \) describes how the curve changes, giving us the direction to construct the tangent line.

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Most popular questions from this chapter

Find the velocity, speed, and acceleration at the given time t of a particle moving along the given curve. $$ x=1+3 t, y=2-4 t, z=7+t ; t=2 $$

In these exercises \(\mathbf{r}(t)\) is the position vector of a particle moving in the plane. Find the velocity, acceleration, and speed at an arbitrary time \(t .\) Then sketch the path of the particle together with the velocity and acceleration vectors at the indicated time \(t .\) $$ \mathbf{r}(t)=e^{t} \mathbf{i}+e^{-t} \mathbf{j} ; t=0 $$

As illustrated in the accompanying figure, a train is traveling on a curved track. At a point where the train is traveling at a speed of \(132 \mathrm{ft} / \mathrm{s}\) and the radius of curvature of the track is \(3000 \mathrm{ft}\), the engineer hits the brakes to make the train slow down at a constant rate of \(7.5 \mathrm{ft} / \mathrm{s}^{2}\). (a) Find the magnitude of the acceleration vector at the instant the engineer hits the brakes. (b) Approximate the angle between the acceleration vector and the unit tangent vector \(\mathbf{T}\) at the instant the engineer hits the brakes.

At time \(t=0\) a projectile is fired from a height \(h\) above level ground at an elevation angle of \(\alpha\) with a speed \(v .\) Let \(R\) be the horizontal distance to the point where the projectile hits the ground. (a) Show that \(\alpha\) and \(R\) must satisfy the equation $$ g\left(\sec ^{2} \alpha\right) R^{2}-2 v^{2}(\tan \alpha) R-2 v^{2} h=0 $$ (b) If \(g, h,\) and \(v\) are constant, then the equation in part (a) defines \(R\) implicitly as a function of \(\alpha\). Let \(R_{0}\) be the maximum value of \(R\) and \(\alpha_{0}\) the value of \(\alpha\) when \(R=R_{0} .\) Use implicit differentiation to find \(d R / d \alpha\) and show that $$ \tan \alpha_{0}=\frac{v^{2}}{g R_{0}} $$ [Hint: Assume that \(d R / d \alpha=0\) when \(R\) attains a maximum. (c) Use the results in parts (a) and (b) to show that $$ R_{0}=\frac{v}{g} \sqrt{v^{2}+2 g h} $$ and $$ \alpha_{0}=\tan ^{-1} \frac{v}{\sqrt{v^{2}+2 g h}} $$

Suppose that a particle vibrates in such a way that its position function is \(\mathbf{r}(t)=16 \sin \pi t \mathbf{i}+4 \cos 2 \pi t \mathbf{j}\), where distance is in millimeters and \(t\) is in seconds. (a) Find the velocity and acceleration at time \(t=1\) s. (b) Show that the particle moves along a parabolic curve. (c) Show that the particle moves back and forth along the curve.

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