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Suppose that the position vector of a particle moving in the plane is \(\mathbf{r}=12 \sqrt{t} \mathbf{i}+t^{3 / 2} \mathbf{j}, t>0 .\) Find the minimum speed of the particle and its location when it has this speed.

Short Answer

Expert verified
Minimum speed is \(3\sqrt{2}\) at position \((24, 8)\).

Step by step solution

01

Find the Velocity Vector

The velocity vector \(\mathbf{v}\) is the derivative of the position vector \(\mathbf{r}\) with respect to time \(t\). Calculate \(\mathbf{v} = \frac{d}{dt}(12 \sqrt{t}) \mathbf{i} + \frac{d}{dt}(t^{3/2}) \mathbf{j}\).
02

Differentiate Each Component

Calculate \(\frac{d}{dt}(12 \sqrt{t}) = 12 \cdot \frac{1}{2\sqrt{t}} = \frac{6}{\sqrt{t}}\). For \(\frac{d}{dt}(t^{3/2}) = \frac{3}{2}\cdot t^{1/2}\), giving the velocity vector \(\mathbf{v} = \frac{6}{\sqrt{t}} \mathbf{i} + \frac{3}{2}t^{1/2}\mathbf{j}\).
03

Find the Magnitude of the Velocity Vector

The speed is the magnitude of the velocity vector \(\mathbf{v}\). Calculate \(|\mathbf{v}| = \sqrt{\left(\frac{6}{\sqrt{t}}\right)^2 + \left(\frac{3}{2}t^{1/2}\right)^2}\).
04

Simplify the Magnitude Expression

Simplify to get \(|\mathbf{v}| = \sqrt{\frac{36}{t} + \frac{9}{4}t}\).
05

Locate Minimum Speed with Derivative

To find the minimum speed, take the derivative of \(|\mathbf{v}|^2\) with respect to \(t\) (this avoids the square root), giving \(\frac{d}{dt}(\frac{36}{t} + \frac{9}{4}t) = -\frac{36}{t^2} + \frac{9}{4}\).
06

Set the Speed Derivative to Zero

Solve \(-\frac{36}{t^2} + \frac{9}{4} = 0\) for \(t\): Multiply through by \(4t^2\) to get \(-144 + 9t^2 = 0\) or \(9t^2 = 144\), resulting in \(t^2 = 16\). Thus, \(t = 4\) since \(t > 0\).
07

Calculate the Minimum Speed

Substitute \(t = 4\) into the speed function: \[|\mathbf{v}(4)| = \sqrt{\frac{36}{4} + \frac{9}{4} \cdot 4} = \sqrt{9 + 9} = \sqrt{18} = 3\sqrt{2}.\]
08

Find the Position Vector at Minimum Speed

For \(t = 4\), plug into the position vector \(\mathbf{r} = 12 \sqrt{4} \mathbf{i} + 4^{3/2} \mathbf{j} = 24 \mathbf{i} + 8 \mathbf{j}\).

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Key Concepts

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

Velocity Vector
In calculus, understanding the concept of a velocity vector is crucial, particularly when dealing with motion in a plane. The velocity vector \(\mathbf{v}\) represents the rate of change of the position vector \(\mathbf{r}\) with respect to time. To find it, one must differentiate each component of the position vector separately with respect to time \(t\). For example, if a position vector is given by \(\mathbf{r} = 12 \sqrt{t} \mathbf{i} + t^{3/2} \mathbf{j}\), the corresponding velocity vector is calculated as \(\mathbf{v} = \frac{d}{dt}(12 \sqrt{t}) \mathbf{i} + \frac{d}{dt}(t^{3/2}) \mathbf{j}\).
To break it down further:
  • The derivative of \(12 \sqrt{t}\) is \(\frac{6}{\sqrt{t}}\), calculated using the power rule by recognizing \(\sqrt{t} = t^{1/2}\).
  • The derivative of \(t^{3/2}\) is \(\frac{3}{2}t^{1/2}\) derived similarly.

Thus, the velocity vector becomes \(\mathbf{v} = \frac{6}{\sqrt{t}} \mathbf{i} + \frac{3}{2}t^{1/2}\mathbf{j}\). This vector describes how quickly and in what direction the position of the particle is changing at any given time \(t\).
Minimum Speed
The minimum speed of a particle is of great interest, especially in optimization problems or when analyzing the particle's movement. To find this, one must look at the magnitude of the velocity vector. The speed is the magnitude, expressed as \|\mathbf{v}| = \sqrt{\left(\frac{6}{\sqrt{t}}\right)^2 + \left(\frac{3}{2}t^{1/2}\right)^2}\.
The goal is to find when this magnitude is at its minimum. To simplify calculations, the derivative of the squared magnitude \(\|\mathbf{v}|^2\) is used instead. For our example, this would be:
  • Squared magnitude \(= \frac{36}{t} + \frac{9}{4}t\).
  • Take the derivative with respect to \(t\), resulting in \(-\frac{36}{t^2} + \frac{9}{4}\).

Set this derivative to zero to find the critical points: solving \(-\frac{36}{t^2} + \frac{9}{4} = 0\) yields \(t = 4\).
Substitute \(t = 4\) into the original magnitude function to find the minimum speed: \|\mathbf{v}(4)| = 3\sqrt{2}\. This method effectively identifies when and how the particle reaches its slowest speed.
Position Vector
A position vector describes a particle's location in space at any given time. It is given in terms of its components along \(\mathbf{i}\) and \(\mathbf{j}\) axes, which represent the horizontal and vertical directions, respectively. In our scenario, the position vector is \(\mathbf{r} = 12 \sqrt{t} \mathbf{i} + t^{3/2} \mathbf{j}\).
At the minimum speed, which we calculated occurs at \(t = 4\), we substitute back into the position vector to get:
  • \(\mathbf{r}(4) = 12 \sqrt{4} \mathbf{i} + 4^{3/2} \mathbf{j}\).
  • This simplifies to \(24 \mathbf{i} + 8 \mathbf{j}\).

Therefore, when the particle is moving slowest, it is located at the point \((24, 8)\) in the plane. This means the particle is 24 units along the x-axis and 8 units along the y-axis from the origin. Understanding how these vectors describe the particle's motion helps visualize the path taken and the position maintained over time.

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Most popular questions from this chapter

Find \(\mathrm{T}(t)\) and \(\mathrm{N}(t)\) at the given point. $$ x=\cosh t, y=\sinh t, z=t ; t=\ln 2 $$

Assume that \(s\) is an arc length parameter for a smooth vector-valued function \(\mathbf{r}(s)\) in 3 -space and that \(d \mathbf{T} / d s\) and \(d \mathbf{N} / d s\) exist at each point on the curve. (This implies that \(d \mathbf{B} / d s\) exists as well, since \(\mathbf{B}=\mathbf{T} \times \mathbf{N}\).) (a) Show that \(d \mathbf{B} / d s\) is perpendicular to \(\mathbf{B}(s)\). (b) Show that \(d \mathbf{B} / d s\) is perpendicular to \(\mathbf{T}(s)\). [Hint: Use the fact that \(\mathbf{B}(s)\) is perpendicular to both \(\mathbf{T}(s)\) and \(\mathbf{N}(s)\) and differentiate \(\mathbf{B} \cdot \mathbf{T}\) with respect to \(s .]\) (c) Use the results in parts (a) and (b) to show that \(d \mathbf{B} / d s\) is a scalar multiple of \(\mathbf{N}(s)\). The negative of this scalar is called the torsion of \(\mathbf{r}(s)\) and is denoted by \(\tau(s)\). Thus, $$ \frac{d \mathbf{B}}{d s}=-\tau(s) \mathbf{N}(s) $$ (d) Show that \(\tau(s)=0\) for all \(s\) if the graph of \(\mathbf{r}(s)\) lies in a plane. [Note: For reasons that we cannot discuss here, the torsion is related to the "twisting" properties of the curve, and \(\tau(s)\) is regarded as a numerical measure of the tendency for the curve to twist out of the osculating plane.]

Suppose that the position function of a particle moving along a circle in the \(x y\) -plane is \(\mathbf{r}=5 \cos 2 \pi t \mathbf{i}+5 \sin 2 \pi t \mathbf{j}\) (a) Sketch some typical displacement vectors over the time interval from \(t=0\) to \(t=1\). (b) What is the distance traveled by the particle during the time interval?

Calculate \(d \mathbf{r} / d \tau\) by the chain rule, and then check your result by expressing \(\mathbf{r}\) in terms of \(\tau\) and differentiating. $$ \mathbf{r}=\langle 3 \cos t, 3 \sin t\rangle ; \quad t=\pi \tau $$

In these exercises \(\mathbf{v}\) and \(\mathbf{a}\) are given at a certain instant of time. Find \(a_{T}, a_{N}, \mathbf{T}\), and \(\mathbf{N}\) at this instant. $$ \mathbf{v}=2 \mathbf{i}+2 \mathbf{j}+\mathbf{k}, \mathbf{a}=\mathbf{i}+2 \mathbf{k} $$

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