Problem 167
Question
A person on a hang glider is spiraling upward as a result of the rapidly rising air on a path having position vector \(\mathbf{r}(t)=(3 \cos t) \mathbf{i}+(3 \sin t) \mathbf{j}+t^{2} \mathbf{k}\). The path is similar to that of a helix, although it is not a helix. The graph is shown here: Find the following quantities: The glider's speed at any time
Step-by-Step Solution
Verified Answer
The speed of the glider is \( \sqrt{9 + 4t^2} \).
1Step 1: Understand the Problem
We are given a position vector \( \mathbf{r}(t) = (3 \cos t) \mathbf{i} + (3 \sin t) \mathbf{j} + t^2 \mathbf{k} \). The task is to find the speed of the glider, which is the magnitude of the velocity vector.
2Step 2: Calculate Velocity
The velocity vector is the derivative of the position vector with respect to time \( t \). Therefore, compute \( \mathbf{v}(t) = \frac{d}{dt} \mathbf{r}(t) \). Differentiate each component: \( \begin{align*}\frac{d}{dt}(3 \cos t) &= -3 \sin t, \\frac{d}{dt}(3 \sin t) &= 3 \cos t, \\frac{d}{dt}(t^2) &= 2t. \\end{align*}\)Thus, the velocity vector is \( \mathbf{v}(t) = (-3 \sin t) \mathbf{i} + (3 \cos t) \mathbf{j} + 2t \mathbf{k} \).
3Step 3: Calculate Speed
The speed is the magnitude of the velocity vector \( \mathbf{v}(t) \). Use the formula for the magnitude of a vector:\( \| \mathbf{v}(t) \| = \sqrt{(-3 \sin t)^2 + (3 \cos t)^2 + (2t)^2} \).
4Step 4: Simplify the Speed Expression
Simplify the expression for speed:\(\begin{align*}\| \mathbf{v}(t) \| &= \sqrt{9 \sin^2 t + 9 \cos^2 t + 4t^2} \&= \sqrt{9(\sin^2 t + \cos^2 t) + 4t^2} \&= \sqrt{9 \cdot 1 + 4t^2} \&= \sqrt{9 + 4t^2}.\end{align*}\)
5Step 5: Conclusion
The formula \( \sqrt{9 + 4t^2} \) represents the speed of the glider at any time \( t \).
Key Concepts
Velocity VectorSpeed CalculationVector MagnitudeDerivative of Position Vector
Velocity Vector
In physics and mathematics, the velocity vector is a fundamental concept, representing both the direction and speed of an object in motion. It is derived from the position vector, which defines the location of an object in space at any given time.
- The velocity vector, \( \mathbf{v}(t) \), is calculated by taking the derivative of the position vector \( \mathbf{r}(t) \) with respect to time \( t \).
- For the hang glider scenario, the position vector is \( \mathbf{r}(t) = (3 \cos t) \mathbf{i} + (3 \sin t) \mathbf{j} + t^2 \mathbf{k} \).
- When we differentiate each component separately, the resulting velocity vector is \( \mathbf{v}(t) = (-3 \sin t) \mathbf{i} + (3 \cos t) \mathbf{j} + 2t \mathbf{k} \).
Speed Calculation
Speed is the scalar measure of how fast an object is moving, irrespective of its direction. It is determined by computing the magnitude of the velocity vector.
- Given the velocity vector \( \mathbf{v}(t) = (-3 \sin t) \mathbf{i} + (3 \cos t) \mathbf{j} + 2t \mathbf{k} \), the speed is found using the formula for vector magnitude.
- The calculation involves squaring each component of \( \mathbf{v}(t) \), summing them up, and finding the square root of that sum.
Vector Magnitude
The vector magnitude is a measure of the length of a vector, providing insight into its size without considering its direction. For any vector \( \mathbf{v} = a\mathbf{i} + b\mathbf{j} + c\mathbf{k} \), the magnitude \( \| \mathbf{v} \| \) is calculated by this formula:\[\| \mathbf{v} \| = \sqrt{a^2 + b^2 + c^2}\]
- This calculation involves squaring each component of the vector, adding the squares, and then taking the square root of the result.
- For the glider's velocity vector, it results in \( \sqrt{(-3 \sin t)^2 + (3 \cos t)^2 + (2t)^2} \).
- Using trigonometric identity \( \sin^2 t + \cos^2 t = 1 \), further simplifies to \( \sqrt{9 + 4t^2} \).
Derivative of Position Vector
The derivative of a position vector is central to determining an object's velocity and, subsequently, its speed. Differentiating the position vector with respect to time provides the velocity vector.
- Each component of the vector needs to be differentiated independently.
- For \( \mathbf{r}(t) = (3 \cos t) \mathbf{i} + (3 \sin t) \mathbf{j} + t^2 \mathbf{k} \), differentiating yields each part: \(-3 \sin t \), \(3 \cos t \), and \(2t\).
Other exercises in this chapter
Problem 165
Consider the motion of a point on the circumference of a rolling circle. As the circle rolls, it generates the cycloid \(\mathbf{r}(t)=(\omega t-\sin (\omega t)
View solution Problem 166
A person on a hang glider is spiraling upward as a result of the rapidly rising air on a path having position vector \(\mathbf{r}(t)=(3 \cos t) \mathbf{i}+(3 \s
View solution Problem 169
Given that \(\mathbf{r}(t)=\left\langle e^{-5 t} \sin t, e^{-5 t} \cos t, 4 e^{-5 t}\right\rangle\) is the position vector of a moving particle, find the follow
View solution Problem 170
Given that \(\mathbf{r}(t)=\left\langle e^{-5 t} \sin t, e^{-5 t} \cos t, 4 e^{-5 t}\right\rangle\) is the position vector of a moving particle, find the follow
View solution