Chapter 11: Problem 14
A position function \(\vec{r}(t)\) is given. Sketch \(\vec{r}(t)\) on the indicated interval. Find \(\vec{v}(t)\) and \(\vec{a}(t),\) then add \(\vec{v}\left(t_{0}\right)\) and \(\vec{a}\left(t_{0}\right)\) to your sketch, with their initial points at \(\vec{r}\left(t_{0}\right)\) for the given value of \(t_{0}\). $$ \vec{r}(t)=\left\langle\frac{2 t+3}{t^{2}+1}, t^{2}\right\rangle \text { on }[-1,1] ; t_{0}=0 $$
Short Answer
Step by step solution
Understanding \\(\vec{r}(t)\\) and the Interval
Derivation of Velocity \\(\vec{v}(t)\\)
Derivation of Acceleration \\(\vec{a}(t)\\)
Evaluate at \\(t_0 = 0\\)
Sketch the Vectors
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Position Function
- \(\vec{r}(t) = \left\langle \frac{2t+3}{t^2+1}, t^2 \right\rangle\)
- The x-component \(\frac{2t+3}{t^2+1}\)
- The y-component \(t^2\)
Velocity Vector
- The derivative of the x-component, using the quotient rule, gives: \( \frac{d}{dt}\left(\frac{2t+3}{t^2+1}\right) = \frac{2-4t^2-6t}{(t^2+1)^2}\)
- The derivative of the y-component is straightforward: \(\frac{d}{dt}(t^2) = 2t\)
Acceleration Vector
- The x-component: Requires differentiating the expression from the velocity found in Step 2, often involving the quotient rule again for precise calculation.
- The y-component: Is much simpler: \(\frac{d}{dt}(2t) = 2\)
Derivative
- Rate of Change: They provide a way to calculate how fast a position or velocity is changing.
- Direction: Derivatives help determine the path or trajectory a particle takes as certain forces act upon it.
- Application: Understanding derivatives allows us to comprehend real-world scenarios, such as the dynamics of moving objects.
Vector Function Sketching
- Plot each value from the position function within the \([-1, 1]\) interval to see the path or trajectory of \(\vec{r}(t)\).
- Identify key points, such as when \(t = 0\), to evaluate and plot specific vectors.
- Visualize \(\vec{v}(0)\) and \(\vec{a}(0)\) by marking them as arrows starting from \(\vec{r}(0)\). This demonstrates the direction and magnitude of velocity and acceleration at that moment.