Problem 37
Question
\(33-38\) Find the tangential and normal components of the acceleration vector. $$\mathbf{r}(t)=e^{t} \mathbf{i}+\sqrt{2} t \mathbf{j}+e^{-t} \mathbf{k}$$
Step-by-Step Solution
Verified Answer
Tangential and Normal components are \( a_T \) and \( a_N \) respectively as calculated.
1Step 1: Find Velocity Vector
The velocity vector \( \mathbf{v}(t) \) is the derivative of the position vector \( \mathbf{r}(t) \) with respect to \( t \). So, compute the derivative:\[ \mathbf{v}(t) = \frac{d}{dt}(e^t \mathbf{i} + \sqrt{2}t \mathbf{j} + e^{-t} \mathbf{k}) = e^t \mathbf{i} + \sqrt{2} \mathbf{j} - e^{-t} \mathbf{k}\]
2Step 2: Find Acceleration Vector
The acceleration vector \( \mathbf{a}(t) \) is the derivative of the velocity vector \( \mathbf{v}(t) \). So, compute the derivative:\[ \mathbf{a}(t) = \frac{d}{dt}(e^t \mathbf{i} + \sqrt{2} \mathbf{j} - e^{-t} \mathbf{k}) = e^t \mathbf{i} + e^{-t} \mathbf{k}\]
3Step 3: Magnitude of Velocity Vector
Compute the magnitude of the velocity vector \( \mathbf{v}(t) \):\[ \| \mathbf{v}(t) \| = \sqrt{(e^t)^2 + (\sqrt{2})^2 + (-e^{-t})^2} = \sqrt{e^{2t} + 2 + e^{-2t}}\]
4Step 4: Tangential Component of Acceleration
The tangential component of acceleration \( a_T \) is given by the derivative of the magnitude of the velocity:\[ a_T = \frac{d}{dt}\| \mathbf{v}(t) \|\]Compute by differentiating the magnitude expression:\[ a_T = \frac{d}{dt} \sqrt{e^{2t} + 2 + e^{-2t}} = \frac{e^{2t} - e^{-2t}}{\sqrt{e^{2t} + 2 + e^{-2t}}}\]
5Step 5: Normal Component of Acceleration
The normal component of acceleration \( a_N \) can be computed using the formula:\[ a_N = \sqrt{\| \mathbf{a}(t) \|^2 - a_T^2}\]First, compute the magnitude of the acceleration vector \( \mathbf{a}(t) \):\[ \| \mathbf{a}(t) \| = \sqrt{(e^t)^2 + (e^{-t})^2} = \sqrt{e^{2t} + e^{-2t}}\]Then compute \( a_N \):\[ a_N = \sqrt{e^{2t} + e^{-2t} - \left(\frac{e^{2t} - e^{-2t}}{\sqrt{e^{2t} + 2 + e^{-2t}}}\right)^2}\]
Key Concepts
Tangential ComponentsNormal ComponentsAcceleration VectorDerivative Calculations
Tangential Components
The tangential component of acceleration refers to how much of an object's acceleration is directed along the path or trajectory. In simpler terms, it indicates how fast the object speeds up or slows down along its path.
We then derive this function with respect to time \( t \) to get \( a_T = \frac{d}{dt} \sqrt{e^{2t} + 2 + e^{-2t}} = \frac{e^{2t} - e^{-2t}}{\sqrt{e^{2t} + 2 + e^{-2t}}} \). This formula shows changes in speed along the path and is crucial for understanding motion dynamics.
- To find this, first determine the magnitude of the velocity vector.
- The tangential component, denoted as \( a_T \), is calculated by taking the derivative of this magnitude.
We then derive this function with respect to time \( t \) to get \( a_T = \frac{d}{dt} \sqrt{e^{2t} + 2 + e^{-2t}} = \frac{e^{2t} - e^{-2t}}{\sqrt{e^{2t} + 2 + e^{-2t}}} \). This formula shows changes in speed along the path and is crucial for understanding motion dynamics.
Normal Components
Normal components measure how much of the acceleration vector is directed perpendicular to the velocity vector's path. This is crucial for understanding how paths curve or bend.
- The normal component of acceleration, denoted as \( a_N \), can be conceptualized as the force pushing you towards or away from the center of a curve.
- It's calculated using the magnitude of the velocity and acceleration vectors, excluding tangential effects.
Acceleration Vector
The acceleration vector explains how the velocity of an object changes over time. It is the derivative of the velocity vector and shows desolation or speeding up in direction.
The result is the acceleration vector \( \mathbf{a}(t) = e^t \mathbf{i} + e^{-t} \mathbf{k} \).This vector tells us how velocity in each direction evolves and is key to understanding motion dynamics.
- In the given exercise, the acceleration vector, \( \mathbf{a}(t) \), is simply the derivative of the velocity vector, \( \mathbf{v}(t) \).
- This computation reveals how each component of motion (in the \( \mathbf{i}, \mathbf{j}, \mathbf{k} \) directions) changes as time progresses.
The result is the acceleration vector \( \mathbf{a}(t) = e^t \mathbf{i} + e^{-t} \mathbf{k} \).This vector tells us how velocity in each direction evolves and is key to understanding motion dynamics.
Derivative Calculations
Derivative calculations are essential in finding how quantities change, especially in motion.
They are foundational to discuss rates, like velocity and acceleration, by describing how one variable changes with respect to another.
The process of differentiation gives exact, real-time insights into motion dynamics, enabling predictions and analysis of an object's trajectory.
They are foundational to discuss rates, like velocity and acceleration, by describing how one variable changes with respect to another.
- In calculus, the derivative provides the rate of change, which for our purposes translates to velocity and acceleration.
- In the exercise, we computed derivatives for both the position and velocity vectors to find velocity and acceleration.
The process of differentiation gives exact, real-time insights into motion dynamics, enabling predictions and analysis of an object's trajectory.
Other exercises in this chapter
Problem 36
\(36-38\) Find a vector function that represents the curve of intersection of the two surfaces. The cylinder \(x^{2}+y^{2}=4\) and the surface \(z=x y\)
View solution Problem 37
Evaluate the integral. $$ \int\left(e^{\prime} \mathbf{i}+2 t \mathbf{j}+\ln t \mathbf{k}\right) d t $$
View solution Problem 37
\(36-38\) Find a vector function that represents the curve of intersection of the two surfaces. The cone \(z=\sqrt{x^{2}+y^{2}}\) and the plane \(z=1+y\)
View solution Problem 38
Evaluate the integral. $$ \int(\cos \pi t \mathbf{i}+\sin \pi t \mathbf{j}+t \mathbf{k}) d t $$
View solution