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At the instant the displacement of a \(1.50 \mathrm{~kg}\) object relative to the origin is \(\vec{d}=(2.00 \mathrm{~m}) \hat{\mathrm{i}}+(4.00 \mathrm{~m}) \hat{\mathrm{j}}-(3.00 \mathrm{~m}) \hat{\mathrm{k}}\), its velocity is \(\vec{v}=-(6.00 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{i}}+(3.00 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{j}}+(3.00 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{k}}\) and it is subject to a force \(\vec{F}=(6.00 \mathrm{~N}) \hat{\mathrm{i}}-(8.00 \mathrm{~N}) \hat{\mathrm{j}}+(4.00 \mathrm{~N}) \hat{\mathrm{k}}\). Find (a) the acceleration of the object, (b) the angular momentum of the object about the origin, (c) the torque about the origin acting on the object, and (d) the angle between the velocity of the object and the force acting on the object.

Short Answer

Expert verified
a) \((4.00 \, \text{m/s}^2 \hat{\text{i}} - 5.33 \, \text{m/s}^2 \hat{\text{j}} + 2.67 \, \text{m/s}^2 \hat{\text{k}})\); b) \([18.0 \hat{\text{i}} + 34.5 \hat{\text{j}} + 64.5 \hat{\text{k}}] \, \text{kg} \cdot \text{m}^2/\text{s}\); c) \([-36 \hat{\text{i}} - 30 \hat{\text{j}} - 40 \hat{\text{k}}] \, \text{N} \cdot \text{m}\); d) \( \theta \approx 125.3^\circ \)."

Step by step solution

01

Calculate the Acceleration

The acceleration \( \vec{a} \) can be found using Newton's second law: \( \vec{F} = m \vec{a} \). Here, \( m = 1.50 \, \text{kg} \) and \( \vec{F} = (6.00 \, \text{N}) \hat{\text{i}} - (8.00 \, \text{N}) \hat{\text{j}} + (4.00 \, \text{N}) \hat{\text{k}} \). Thus,\[ \vec{a} = \frac{\vec{F}}{m} = \frac{1}{1.50} \left((6.00 \, \text{N}) \hat{\text{i}} - (8.00 \, \text{N}) \hat{\text{j}} + (4.00 \, \text{N}) \hat{\text{k}}\right) \]Simplifying, \[ \vec{a} = (4.00 \, \text{m/s}^2) \hat{\text{i}} - (5.33 \, \text{m/s}^2) \hat{\text{j}} + (2.67 \, \text{m/s}^2) \hat{\text{k}} \].
02

Find the Angular Momentum

Angular momentum \( \vec{L} \) about the origin is given by \( \vec{L} = \vec{r} \times m \vec{v} \) where \( \vec{r} \) is the displacement vector and \( \vec{v} \) is the velocity vector.\( \vec{r} = (2.00 \, \text{m}) \hat{\text{i}} + (4.00 \, \text{m}) \hat{\text{j}} - (3.00 \, \text{m}) \hat{\text{k}} \) and \( \vec{v} = -(6.00 \, \text{m/s}) \hat{\text{i}} + (3.00 \, \text{m/s}) \hat{\text{j}} + (3.00 \, \text{m/s}) \hat{\text{k}} \).Calculate:\[ \vec{L} = \begin{vmatrix} \hat{\text{i}} & \hat{\text{j}} & \hat{\text{k}} \ 2.00 & 4.00 & -3.00 \ -9.00 & 4.50 & 4.50 \end{vmatrix} \]\[ \vec{L} = \hat{\text{i}}((4.00 \times 4.50) - (-3.00 \times 4.50)) - \hat{\text{j}}((2.00 \times 4.50) - (-3.00 \times -9.00)) + \hat{\text{k}}((2.00 \times 4.50) - (4.00 \times -9.00)) \]\[ \vec{L} = 18.0 \hat{\text{i}} + 34.5 \hat{\text{j}} + 64.5 \hat{\text{k}} \, \text{kg} \cdot \text{m}^2/\text{s} \]
03

Calculate the Torque

Torque \( \vec{\tau} \) is given by \( \vec{\tau} = \vec{r} \times \vec{F} \).Using \( \vec{r} \) and \( \vec{F} \), the cross-product is:\[ \vec{\tau} = \begin{vmatrix} \hat{\text{i}} & \hat{\text{j}} & \hat{\text{k}} \ 2.00 & 4.00 & -3.00 \ 6.00 & -8.00 & 4.00 \end{vmatrix} \]\[ \vec{\tau} = \hat{\text{i}}((4.00 \times 4.00) - (-3.00 \times -8.00)) - \hat{\text{j}}((2.00 \times 4.00) - (-3.00 \times 6.00)) + \hat{\text{k}}((2.00 \times -8.00) - (4.00 \times 6.00)) \]\[ \vec{\tau} = -36 \hat{\text{i}} - 30 \hat{\text{j}} - 40 \hat{\text{k}} \, \text{N} \cdot \text{m} \].
04

Determine the Angle Between Velocity and Force

The angle \( \theta \) between two vectors \( \vec{v} \) and \( \vec{F} \) is given by\[ \cos \theta = \frac{\vec{v} \cdot \vec{F}}{||\vec{v}|| ||\vec{F}||} \]Calculate the dot product \( \vec{v} \cdot \vec{F} = (-6.00)(6.00) + (3.00)(-8.00) + (3.00)(4.00) \) resulting in -60.Find magnitudes \(||\vec{v}|| = \sqrt{(-6.00)^2 + (3.00)^2 + (3.00)^2} = \sqrt{54} \) and\(||\vec{F}|| = \sqrt{(6.00)^2 + (-8.00)^2 + (4.00)^2} = 10 \).So, \[ \cos \theta = \frac{-60}{\sqrt{54} \times 10} = \frac{-60}{30 \cdot \sqrt{6}} \approx -0.577 \].\( \theta \approx \cos^{-1}(-0.577) \), thus \( \theta \approx 125.3^\circ \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Newton's Second Law
Newton's Second Law is a fundamental principle in physics that relates the force acting on an object to its mass and the acceleration it experiences. Expressed as \( \vec{F} = m \vec{a} \), this law means that the acceleration (\( \vec{a} \)) of an object is directly proportional to the net force (\( \vec{F} \)) acting upon it, and inversely proportional to its mass (\( m \)). The direction of the acceleration is the same as that of the net force. To solve problems involving Newton's Second Law:
  • Identify the forces acting on the object.
  • Sum up the vector components of these forces to find the net force.
  • Calculate the acceleration by dividing the net force by the mass of the object.
In our original exercise, the net force acting on the 1.50 kg object is given as a vector \( \vec{F} = (6.00 \, \text{N}) \hat{\text{i}} - (8.00 \, \text{N}) \hat{\text{j}} + (4.00 \, \text{N}) \hat{\text{k}} \). By dividing each component of this force by the mass, you determine the acceleration vector \( \vec{a} = (4.00 \, \text{m/s}^2) \hat{\text{i}} - (5.33 \, \text{m/s}^2) \hat{\text{j}} + (2.67 \, \text{m/s}^2) \hat{\text{k}} \). This calculation shows how the various components affect the object's motion in space.
Angular Momentum
Angular momentum is a concept that extends the idea of linear momentum to bodies rotating around a point or axis. It is a measure of the quantity of rotation of an object and is given by the equation \( \vec{L} = \vec{r} \times m \vec{v} \), where \( \vec{L} \) is the angular momentum, \( \vec{r} \) is the position vector (displacement from the origin), \( m \) is the mass, and \( \vec{v} \) is the velocity vector.
  • "Cross product" (\( \times \)) indicates that both the magnitude of the vectors and their direction are important.
  • The units of angular momentum are typically \( \text{kg} \cdot \text{m}^2/\text{s} \).
In our exercise, the displacement \( \vec{r} \) and velocity \( \vec{v} \) vectors are used in a vector cross product to find \( \vec{L} = 18.0 \hat{\text{i}} + 34.5 \hat{\text{j}} + 64.5 \hat{\text{k}} \, \text{kg} \cdot \text{m}^2/\text{s} \). This vector tells us how the object is rotating relative to the origin in three-dimensional space. Understanding angular momentum helps us explore rotational movement and the conservation principles, crucial for explaining phenomena like gyroscopic effects.
Torque
Torque is the measure of the force that causes an object to rotate around an axis. The math behind torque involves the cross product, which is used to calculate the torque vector \( \vec{\tau} = \vec{r} \times \vec{F} \). Here, \( \vec{r} \) is the position vector of the object and \( \vec{F} \) is the applied force.
  • The cross product implies that torque depends on the perpendicular distance from the axis to the line of action of the force, thus involving angles between vectors.
  • Torque is measured in units of \( \text{N} \cdot \text{m} \).
In our problem, the calculated torque \( \vec{\tau} = -36 \hat{\text{i}} - 30 \hat{\text{j}} - 40 \hat{\text{k}} \, \text{N} \cdot \text{m} \) indicates how effectively the force causes the object to rotate around the origin. Understanding the direction and magnitude of torque allows us to predict how systems respond to forces - essential for fields ranging from engineering to biomechanics.
Vector Analysis
Vector analysis is a critical component for solving problems involving direction and magnitude, central to physics and engineering applications. Vectors can represent various quantities, such as displacement, velocity, acceleration, force, and more. To effectively analyze vectors:
  • Break vectors down into components using unit vectors \( \hat{\text{i}} \), \( \hat{\text{j}} \), and \( \hat{\text{k}} \) along the x, y, and z axes, respectively.
  • Use operations like dot product (\( \cdot \)) to find angles between vectors or cross product (\( \times \)) to find perpendicular vectors.
In the exercise, vector analysis was used to calculate the angle between the velocity and force vectors, ultimately finding the angle of approximately 125.3 degrees. This involved using the dot product for determining cosines of angles. Vector analysis provides a method to interpret physical phenomena that have both magnitude and direction, a crucial skill for problem-solving in physics.

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Most popular questions from this chapter

The uniform rod (length \(0.60 \mathrm{~m}\), mass \(1.0 \mathrm{~kg}\) ) in Fig. 11-49 rotates in the plane of the figure about an axis through one end, with a rotational inertia of \(0.12 \mathrm{~kg} \cdot \mathrm{m}^{2}\). As the rod swings through its lowest position, it collides with a \(0.20 \mathrm{~kg}\) putty wad that sticks to the end of the rod. If the rod's angular speed just before collision is \(2.4 \mathrm{rad} / \mathrm{s}\), what is the angular speed of the rod-putty system immediately after collision?

A force \(\vec{F}=(6.00 \hat{\mathrm{i}}-4.00 \hat{\mathrm{j}}) \mathrm{N}\) acts on a particle with position vector \(\vec{r}=(-3.00 \hat{\mathrm{i}}+1.00 \hat{\mathrm{j}}) \mathrm{m}\). Find (a) the torque about the origin acting on the particle and \((b)\) the angle between \(\vec{r}\) and \(\vec{F}\).

A car travels at \(80 \mathrm{~km} / \mathrm{h}\) on a level road in the positive direction of an \(x\) axis. Each tire has a diameter of \(66 \mathrm{~cm}\). Relative to a woman riding in the car and in unit-vector notation, what are the velocity \(\vec{v}\) at the (a) center, (b) top, and (c) bottom of the tire and the magnitude \(a\) of the acceleration at the (d) center, (e) top, and (f) bottom of each tire? Relative to a hitchhiker sitting next to the road and in unit-vector notation, what are the velocity \(\vec{v}\) at the \((g)\) center, (h) top, and (i) bottom of the tire and the magnitude \(a\) of the acceleration at the \((\mathrm{j})\) center, \((\mathrm{k})\) top, and (l) bottom of each tire?

In unit vector notation, find the net torque about the origin on a particle located at \((2.0 \mathrm{~m},-2.0 \mathrm{~m},-6.0 \mathrm{~m})\) when the three forces \(\vec{F}_{1}=(6.0 \mathrm{~N}) \hat{\mathrm{j}}, \vec{F}_{2}^{t}=(1.0 \mathrm{~N}) \hat{\mathrm{i}}-(2.0 \mathrm{~N}) \hat{\mathrm{j}}\), and \(\vec{F}_{3}=(4.0 \mathrm{~N}) \hat{\mathrm{i}}+\) \((2.0 \mathrm{~N}) \hat{\mathrm{j}}-(3.0 \mathrm{~N}) \mathrm{k}\) act on the particle.

A sanding disk with rotational inertia \(8.6 \times 10^{-3} \mathrm{~kg} \cdot \mathrm{m}^{2}\) is attached to an electric drill whose motor delivers a torque of magnitude \(16 \mathrm{~N} \cdot \mathrm{m}\) about the central axis of the initially stationary disk. About that axis and with the torque applied for \(33 \mathrm{~ms}\), what is the magnitude of the (a) angular momentum and (b) angular velocity of the disk?

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