Problem 27
Question
At one instant, force \(\vec{F}=4.0 \mathrm{j} \mathrm{N}\) acts on a \(0.25 \mathrm{~kg}\) object that has position vector \(\vec{r}=(2.0 \mathrm{i}-2.0 \mathrm{k}) \mathrm{m}\) and velocity vector \(\vec{v}=(-5.0 \hat{i}+5.0 \mathrm{k}) \mathrm{m} / \mathrm{s}\). About the origin and in unit-vector notation, what are (a) the object's angular momentum and (b) the torque acting on the object?
Step-by-Step Solution
Verified Answer
(a) \( \vec{L} = \vec{0} \), (b) \( \vec{\tau} = 8.0 \hat{i} + 8.0 \hat{k} \).\)
1Step 1: Find Angular Momentum
Angular momentum \( \vec{L} \) is given by \( \vec{L} = \vec{r} \times \vec{p} \), where \( \vec{p} \) is the linear momentum. First, calculate \( \vec{p} \) using \( \vec{p} = m \vec{v} \). Thus, \( \vec{p} = 0.25 \times (-5.0 \hat{i} + 5.0 \hat{k}) = -1.25 \hat{i} + 1.25 \hat{k} \). Now, compute \( \vec{L} \): \[ \vec{L} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 2.0 & 0 & -2.0 \ -1.25 & 0 & 1.25 \end{vmatrix} \] Evaluating the determinant gives: \[ \vec{L} = \hat{j} (2.0 \times 1.25 - (-2.0) \times (-1.25)) = \hat{j} (2.5 - 2.5) = \vec{0} \]. Therefore, the angular momentum is \( \vec{L} = \vec{0} \).
2Step 2: Find the Torque
Torque \( \vec{\tau} \) is given by \( \vec{\tau} = \vec{r} \times \vec{F} \). Given \( \vec{F} = 4.0 \hat{j} \) and \( \vec{r} = 2.0 \hat{i} - 2.0 \hat{k} \), calculate \( \vec{\tau} \): \[ \vec{\tau} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 2.0 & 0 & -2.0 \ 0 & 4.0 & 0 \end{vmatrix} \] Evaluating the determinant gives: \[ \vec{\tau} = \hat{i} (0 \times 0 - 4 \times (-2.0)) + \hat{j} (-2.0 \times 0 - 2.0 \times 0) + \hat{k} (2.0 \times 4.0 - 0 \times 0) \]\[ \vec{\tau} = \hat{i} (8.0) + \hat{k} (8.0) = 8.0 \hat{i} + 8.0 \hat{k} \] Thus, the torque is \( \vec{\tau} = 8.0 \hat{i} + 8.0 \hat{k} \).
Key Concepts
TorqueCross ProductLinear MomentumDeterminant Evaluation
Torque
Torque is a fundamental concept in physics, often symbolized by \( \vec{\tau} \). It describes the tendency of a force to rotate an object around an axis. You can think of it as a twist or a rotational equivalent of force.
The equation for torque is \( \vec{\tau} = \vec{r} \times \vec{F} \), where \( \vec{r} \) is the position vector (the distance and direction from the pivot point to the point of force application) and \( \vec{F} \) is the force vector.
The equation for torque is \( \vec{\tau} = \vec{r} \times \vec{F} \), where \( \vec{r} \) is the position vector (the distance and direction from the pivot point to the point of force application) and \( \vec{F} \) is the force vector.
- The greater the distance (magnitude of \( \vec{r} \)), the larger the torque if the force is applied perpendicularly.
- If the force is aligned with \( \vec{r} \), the torque is zero.
- The direction of \( \vec{\tau} \) is given by the right-hand rule, which is useful for determining the sense of rotation.
Cross Product
The cross product is a mathematical operation, often used in physics, that takes two vectors and produces another vector that is perpendicular to both. In terms of two vectors \( \vec{A} \) and \( \vec{B} \), the cross product \( \vec{A} \times \vec{B} \) is calculated as:
\[\vec{A} \times \vec{B} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix}\]
Here, \( a_1, a_2, a_3 \) and \( b_1, b_2, b_3 \) are the components of \( \vec{A} \) and \( \vec{B} \). The determinant is used to calculate the resulting vector perpendicular to \( \vec{A} \) and \( \vec{B} \).
\[\vec{A} \times \vec{B} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix}\]
Here, \( a_1, a_2, a_3 \) and \( b_1, b_2, b_3 \) are the components of \( \vec{A} \) and \( \vec{B} \). The determinant is used to calculate the resulting vector perpendicular to \( \vec{A} \) and \( \vec{B} \).
- The magnitude of the cross product is given by \( |\vec{A}| |\vec{B}| \sin(\theta) \), where \( \theta \) is the angle between \( \vec{A} \) and \( \vec{B} \).
- Vector direction: follow the right-hand rule to determine the direction of the result.
Linear Momentum
Linear momentum is a measure of an object's motion, denoted by \( \vec{p} \). It is the product of an object's mass and its velocity expressed as \( \vec{p} = m \vec{v} \). This means:
In physics, linear momentum is conserved in isolated systems, meaning \( \vec{p} \) remains the same if no external forces act on the system.
In the exercise, calculating linear momentum was used to find angular momentum, showcasing its role in linking linear and rotational dynamics.
- Mass \( (m) \): how much matter is in the object.
- Velocity \( (\vec{v}) \): the speed and direction of the object's motion.
In physics, linear momentum is conserved in isolated systems, meaning \( \vec{p} \) remains the same if no external forces act on the system.
In the exercise, calculating linear momentum was used to find angular momentum, showcasing its role in linking linear and rotational dynamics.
Determinant Evaluation
Determinant evaluation is a crucial mathematical technique used in this context to compute the cross product of vectors. This method involves calculating the determinant of a 3x3 matrix comprised of the unit vectors \( \hat{i}, \hat{j}, \hat{k} \) and the components of the vectors involved.
For example, for two vectors \( \vec{r} = (r_1, r_2, r_3) \) and \( \vec{F} = (f_1, f_2, f_3) \):
\[\begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ r_1 & r_2 & r_3 \ f_1 & f_2 & f_3 \end{vmatrix}\]
For example, for two vectors \( \vec{r} = (r_1, r_2, r_3) \) and \( \vec{F} = (f_1, f_2, f_3) \):
\[\begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ r_1 & r_2 & r_3 \ f_1 & f_2 & f_3 \end{vmatrix}\]
- Determine the product for each part by using the formula \( \text{Det} = \hat{i}(b_2c_3 - b_3c_2) - \hat{j}(a_1c_3 - a_3c_1) + \hat{k}(a_1b_2 - a_2b_1) \).
- Each term involves computations between components alongside applying sign changes.
Other exercises in this chapter
Problem 24
In unit-vector notation, what is the torque about the origin on a jar of jalapeno peppers located at coordinates \((3.0 \mathrm{~m},-2.0 \mathrm{~m}\), \(4.0 \m
View solution Problem 25
Force \(\vec{F}=(-8.0 \mathrm{~N}) \hat{\mathrm{i}}+(6.0 \mathrm{~N}) \mathrm{j}\) acts on a particle with position vector \(\vec{r}=(3.0 \mathrm{~m}) \mathrm{i
View solution Problem 28
A \(2.0 \mathrm{~kg}\) particle-like object moves in a plane with velocity components \(v_{x}=30 \mathrm{~m} / \mathrm{s}\) and \(v_{y}=60 \mathrm{~m} / \mathrm
View solution Problem 30
At the instant the displacement of a \(2.00 \mathrm{~kg}\) object relative to the origin is \(\vec{d}=(2.00 \mathrm{~m}) \hat{i}+(4.00 \mathrm{~m}) \mathrm{j}-(
View solution