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Compute \(\mathbf{r}^{\prime \prime}(t)\) and \(\mathbf{r}^{\prime \prime \prime}(t)\) for the following functions. $$\mathbf{r}(t)=\left\langle e^{4 t}, 2 e^{-4 t}+1,2 e^{-t}\right\rangle$$

Short Answer

Expert verified
Question: Find the acceleration and jerk vectors of the given function: $$\mathbf{r}(t)=\left\langle e^{4 t}, 2 e^{-4 t}+1,2 e^{-t}\right\rangle$$ Answer: The acceleration (second-order derivative) and jerk (third-order derivative) vectors are as follows: Acceleration: $$\mathbf{r}^{\prime\prime} (t) = \left\langle 16e^{4t}, 32e^{-4t}, 2e^{-t} \right\rangle$$ Jerk: $$\mathbf{r}^{\prime\prime\prime} (t) = \left\langle 64e^{4t}, -128e^{-4t}, 2e^{-t} \right\rangle$$

Step by step solution

01

Compute the first-order derivative (velocity) for each component function.

To find the velocity vector, take the first derivative for each of the component functions: $$\frac{d}{dt} e^{4t}, \frac{d}{dt}(2e^{-4t} + 1), \frac{d}{dt}(2e^{-t})$$ Compute the derivatives: $$4 e^{4t}, -8e^{-4t}, -2e^{-t}$$ Now that we have the first-order derivative of each component, let's write it in a vector form: $$\mathbf{r}^\prime (t) = \left\langle 4 e^{4t}, -8e^{-4t}, -2e^{-t} \right\rangle$$
02

Compute the second-order derivative (acceleration) for each component function.

To find the acceleration vector, take the second derivative for each of the component functions: $$\frac{d^2}{dt^2} 4e^{4t}, \frac{d^2}{dt^2}(-8e^{-4t}), \frac{d^2}{dt^2}(-2e^{-t})$$ Compute the derivatives: $$16e^{4t}, 32e^{-4t}, 2e^{-t}$$ Now that we have the second-order derivative of each component, let's write it in a vector form: $$\mathbf{r}^{\prime\prime} (t) = \left\langle 16e^{4t}, 32e^{-4t}, 2e^{-t} \right\rangle$$
03

Compute the third-order derivative (jerk) for each component function.

To find the jerk vector, take the third derivative for each of the component functions: $$\frac{d^3}{dt^3} 16e^{4t}, \frac{d^3}{dt^3}(32e^{-4t}), \frac{d^3}{dt^3}(2e^{-t})$$ Compute the derivatives: $$64e^{4t}, -128e^{-4t}, 2e^{-t}$$ Now that we have the third-order derivative of each component, let's write it in a vector form: $$\mathbf{r}^{\prime\prime\prime} (t) = \left\langle 64e^{4t}, -128e^{-4t}, 2e^{-t} \right\rangle$$ Now we have both the acceleration and jerk vectors, let's write them out together: Acceleration (second-order derivative): $$\mathbf{r}^{\prime\prime} (t) = \left\langle 16e^{4t}, 32e^{-4t}, 2e^{-t} \right\rangle$$ Jerk (third-order derivative): $$\mathbf{r}^{\prime\prime\prime} (t) = \left\langle 64e^{4t}, -128e^{-4t}, 2e^{-t} \right\rangle$$

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Most popular questions from this chapter

Consider the curve \(\mathbf{r}(t)=(a \cos t+b \sin t) \mathbf{i}+(c \cos t+d \sin t) \mathbf{j}+(e \cos t+f \sin t) \mathbf{k}\) where \(a, b, c, d, e,\) and \(f\) are real numbers. It can be shown that this curve lies in a plane. Graph the following curve and describe it. $$\begin{aligned}\mathbf{r}(t)=&(2 \cos t+2 \sin t) \mathbf{i}+(-\cos t+2 \sin t) \mathbf{j} \\\&+(\cos t-2 \sin t) \mathbf{k}\end{aligned}$$

Compute the indefinite integral of the following functions. $$\mathbf{r}(t)=\left\langle t^{4}-3 t, 2 t-1,10\right\rangle$$

Relationship between \(\mathbf{r}\) and \(\mathbf{r}^{\prime}\) Consider the curve \(\mathbf{r}(t)=\langle\sqrt{t}, 1, t\rangle,\) for \(t>0 .\) Find all points on the curve at which \(\mathbf{r}\) and \(\mathbf{r}^{\prime}\) are orthogonal.

Cauchy-Schwarz Inequality The definition \(\mathbf{u} \cdot \mathbf{v}=|\mathbf{u}||\mathbf{v}| \cos \theta\) implies that \(|\mathbf{u} \cdot \mathbf{v}| \leq|\mathbf{u}||\mathbf{v}|\) (because \(|\cos \theta| \leq 1\) ). This inequality, known as the Cauchy-Schwarz Inequality, holds in any number of dimensions and has many consequences. Algebra inequality Show that $$\left(u_{1}+u_{2}+u_{3}\right)^{2} \leq 3\left(u_{1}^{2}+u_{2}^{2}+u_{3}^{2}\right)$$ for any real numbers \(u_{1}, u_{2},\) and \(u_{3} .\) (Hint: Use the CauchySchwarz Inequality in three dimensions with \(\mathbf{u}=\left\langle u_{1}, u_{2}, u_{3}\right\rangle\) and choose v in the right way.)

Motion on a sphere Prove that \(\mathbf{r}\) describes a curve that lies on the surface of a sphere centered at the origin \(\left(x^{2}+y^{2}+z^{2}=a^{2}\right.\) with \(a \geq 0\) ) if and only if \(\mathbf{r}\) and \(\mathbf{r}^{\prime}\) are orthogonal at all points of the curve.

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