Problem 37
Question
Given \(\mathbf{r}(t)=\langle t+\cos t, t-\sin t\rangle\), find the velocity and the speed at any time.
Step-by-Step Solution
Verified Answer
The velocity is \(\langle 1 - \sin t, 1 - \cos t \rangle\) and the speed is \(\sqrt{3 - 2(\sin t + \cos t)}\)."
1Step 1: Define the Velocity Vector
The velocity vector is the derivative of the position vector with respect to time. Given \(\mathbf{r}(t)=\langle t+\cos t, t-\sin t\rangle\), we need to differentiate each component with respect to \(t\).
2Step 2: Differentiate the Components
Differentiate the first component: \(t + \cos t\) gives \(1 - \sin t\). Differentiate the second component: \(t - \sin t\) gives \(1 - \cos t\). Thus, the velocity vector is \(\mathbf{v}(t) = \langle 1 - \sin t, 1 - \cos t \rangle\).
3Step 3: Define Speed
The speed is the magnitude of the velocity vector. We use the formula for the magnitude of a vector: \(\|\mathbf{v}(t)\| = \sqrt{(v_1(t))^2 + (v_2(t))^2}\) where \(v_1(t)\) and \(v_2(t)\) are the components of the velocity vector.
4Step 4: Calculate the Magnitude
Substitute the components of \(\mathbf{v}(t)\): \(\|\mathbf{v}(t)\| = \sqrt{(1 - \sin t)^2 + (1 - \cos t)^2}\). Expand the squared terms: \((1 - \sin t)^2 = 1 - 2\sin t + \sin^2 t\) and \((1 - \cos t)^2 = 1 - 2\cos t + \cos^2 t\).
5Step 5: Simplify the Expression
Combine the terms: \(\|\mathbf{v}(t)\| = \sqrt{2 - 2(\sin t + \cos t) + \sin^2 t + \cos^2 t}\). Recall from trigonometric identities that \(\sin^2 t + \cos^2 t = 1\), so substitute it in: \(\|\mathbf{v}(t)\| = \sqrt{3 - 2(\sin t + \cos t)}\).
Key Concepts
Derivative of Position VectorMagnitude of VelocityTrigonometric Identities
Derivative of Position Vector
Understanding the concept of derivative is crucial in the study of motion. A position vector, denoted as \( \mathbf{r}(t) \), describes the location of a point in space as a function of time \( t \). When we differentiate this position vector with respect to time, we find the velocity vector. This tells us not only how fast but also in what direction the position is changing at any given moment.
In our exercise, the position vector is given by:
In our exercise, the position vector is given by:
- \( \mathbf{r}(t) = \langle t + \cos t, t - \sin t \rangle \)
- For \( t + \cos t \), the derivative is \( 1 - \sin t \).
- For \( t - \sin t \), the derivative is \( 1 - \cos t \).
- \( \mathbf{v}(t) = \langle 1 - \sin t, 1 - \cos t \rangle \)
Magnitude of Velocity
The magnitude of velocity, often referred to as speed, measures how fast an object is moving regardless of its direction. Once we have the velocity vector, we can find its magnitude using the formula:
- \( \|\mathbf{v}(t)\| = \sqrt{(v_1(t))^2 + (v_2(t))^2} \)
- \( \|\mathbf{v}(t)\| = \sqrt{(1 - \sin t)^2 + (1 - \cos t)^2} \)
- \( (1 - \sin t)^2 = 1 - 2\sin t + \sin^2 t \)
- \( (1 - \cos t)^2 = 1 - 2\cos t + \cos^2 t \)
- \( \|\mathbf{v}(t)\| = \sqrt{3 - 2(\sin t + \cos t)} \)
Trigonometric Identities
Trigonometric identities are mathematical equations that relate the trigonometric functions sine, cosine, and tangent to one another. They can simplify complex mathematical expressions and are especially helpful in calculus and physics.
In the exercise, a key trigonometric identity used to find the speed of the object is:
Instead of dealing with two squared terms, we combined them into a simpler expression that directly linked to the object's motion.
Trigonometric identities like this can also help:
In the exercise, a key trigonometric identity used to find the speed of the object is:
- \( \sin^2 t + \cos^2 t = 1 \)
Instead of dealing with two squared terms, we combined them into a simpler expression that directly linked to the object's motion.
Trigonometric identities like this can also help:
- Simplify derivatives and integrals involving trigonometric functions
- Identify relationships between components of vectors in multidimensional space
Other exercises in this chapter
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