/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 44 A force, \(\vec{F}=(2 \hat{x}+3 ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A force, \(\vec{F}=(2 \hat{x}+3 \hat{y}) \mathrm{N},\) is applied to an object at a point whose position vector with respect to the pivot point is \(\vec{r}=(4 \hat{x}+4 \hat{y}+4 \hat{z}) \mathrm{m} .\) Calculate the torque created by the force about that pivot point.

Short Answer

Expert verified
Question: Calculate the torque created by the force \(\vec{F} = (2\hat{x} + 3\hat{y})\,\text{N}\) applied at a point with the position vector \(\vec{r} = (4\hat{x} + 4\hat{y} + 4\hat{z})\,\text{m}\) with respect to the pivot point. Answer: The torque is \(\vec{\tau} = (-12\hat{x} + 8\hat{y} + 4\hat{z})\,\text{Nm}\).

Step by step solution

01

Write down the given vectors

We are given the force vector \(\vec{F} = (2\hat{x} + 3\hat{y})\,\text{N}\) and the position vector \(\vec{r} = (4\hat{x} + 4\hat{y} + 4\hat{z})\,\text{m}\).
02

Calculate the cross product of \(\vec{r}\) and \(\vec{F}\)

To find the torque vector \(\vec{\tau}\), we need to calculate the cross product of \(\vec{r}\) and \(\vec{F}\). The cross product of two vectors is given by: \(\vec{\tau} = \vec{r} \times \vec{F} = \begin{vmatrix} \hat{x} & \hat{y} & \hat{z} \\ 4 & 4 & 4 \\ 2 & 3 & 0 \end{vmatrix}\)
03

Evaluate the cross product

Now, let's evaluate the cross product using the formula: \(\vec{\tau} = (\hat{x}(4\cdot0 - 3\cdot4) - \hat{y}(4\cdot0 - 2\cdot4) + \hat{z}(4\cdot3 - 2\cdot4))\) \(\vec{\tau} = (-12\hat{x} + 8\hat{y} + 4\hat{z})\,\text{Nm}\)
04

Write the final answer

The torque created by the force \(\vec{F}\), about the pivot point with the position vector \(\vec{r}\), is: \(\vec{\tau} = (-12\hat{x} + 8\hat{y} + 4\hat{z})\,\text{Nm}\)

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Cross Product
In physics and mathematics, the cross product is an operation performed on two vectors. It results in another vector that is perpendicular to the plane formed by the original vectors. This operation is crucial in the calculation of torque. The formula for the cross product of vectors \( \vec{A} = a_1\hat{x} + a_2\hat{y} + a_3\hat{z} \) and \( \vec{B} = b_1\hat{x} + b_2\hat{y} + b_3\hat{z} \) is given by a determinant:
  • \( \vec{A} \times \vec{B} = \begin{vmatrix} \hat{x} & \hat{y} & \hat{z} \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix} \)
The cross product is not commutative, meaning that \( \vec{A} \times \vec{B} eq \vec{B} \times \vec{A} \). Instead, \( \vec{A} \times \vec{B} = - (\vec{B} \times \vec{A}) \). This property reflects the right-hand rule used to determine the direction of the resulting vector. The magnitude of the cross product is equal to the product of the magnitudes of the two vectors and the sine of the angle between them.
  • \( |\vec{A} \times \vec{B}| = |\vec{A}| \cdot |\vec{B}| \cdot \sin\theta \)
This makes the cross product a powerful tool for vectorial calculations in 3D space, especially for torque and rotational dynamics.
Vectors
Vectors are mathematical objects used to represent quantities that have both magnitude and direction. Commonly denoted by symbols like \(\vec{A}\), vectors differ from scalars, which only possess magnitude.
  • Example: \(\vec{v} = 3\hat{x} + 4\hat{y} \)
Vectors are often represented in component form, using the unit vectors \(\hat{x}, \hat{y}, \) and \(\hat{z}\) in three-dimensional space, corresponding to the directions along the x, y, and z axes. The magnitude of a vector \(\vec{v} = a\hat{x} + b\hat{y} + c\hat{z}\) can be calculated as:
  • \( |\vec{v}| = \sqrt{a^2 + b^2 + c^2} \)
Adding or subtracting vectors involves combining their respective components. Unlike scalars, vectors follow unique rules for multiplication, such as the dot and cross products. The cross product, specifically, results in another vector perpendicular to the initial pair, while the dot product results in a scalar. Vectors are indispensable in many fields including engineering, physics, and mathematics because they provide a compact way of describing physical quantities.
Force
Force is a physical quantity that represents an interaction that changes or tends to change the motion of an object. In vector form, it has both magnitude and direction, making it a perfect candidate for vector representation. The basic unit of force in the International System of Units (SI) is the newton (N).
  • Example: A force \(\vec{F} = 2\hat{x} + 3\hat{y}\, \mathrm{N} \)
Newton's second law of motion provides a clear relationship between force, mass, and acceleration: \( \vec{F} = m \cdot \vec{a} \), where \(m\) is the mass of an object and \(\vec{a}\) its acceleration. Since forces can be combined using vector addition, understanding their vector nature helps in solving problems involving multiple forces acting on a body. When discussing torque, a force applied at a certain point with respect to a pivot creates rotational effect, which is influenced by both the magnitude of the force and its distance from the pivot, depicted by the position vector.
Position Vector
The position vector is a vector that describes the position of a point in space relative to a reference point or origin. It is often denoted by \(\vec{r}\) and can be expressed in three-dimensional space as \( \vec{r} = x\hat{x} + y\hat{y} + z\hat{z} \).
  • Example: \(\vec{r} = 4\hat{x} + 4\hat{y} + 4\hat{z}\, \mathrm{m} \)
The position vector plays a crucial role in physics and engineering, particularly when calculating torque or angular displacement. Torque, for instance, is the rotational equivalent of linear force, calculated as the cross product between the position vector and the force vector acting on a point.
  • \( \vec{\tau} = \vec{r} \times \vec{F} \)
This application demonstrates how a position vector not only locates a point in space but also aids in understanding and analyzing rotational motion. Moreover, the length of a position vector is the straight-line distance from the origin to the point, computed as \(|\vec{r}| = \sqrt{x^2 + y^2 + z^2}\). Understanding position vectors is essential for calculating many other physical phenomena like velocity and acceleration in a coordinate system.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

The turbine and associated rotating parts of a jet engine have a total moment of inertia of \(25 \mathrm{~kg} \mathrm{~m}^{2}\). The turbine is accelerated uniformly from rest to an angular speed of \(150 \mathrm{rad} / \mathrm{s}\) in a time of \(25 \mathrm{~s}\). Find a) the angular acceleration, b) the net torque required, c) the angle turned through in \(25 \mathrm{~s}\) d) the work done by the net torque, and e) the kinetic energy of the turbine at the end of the \(25 \mathrm{~s}\).

A sheet of plywood \(1.3 \mathrm{~cm}\) thick is used to make a cabinet door \(55 \mathrm{~cm}\) wide by \(79 \mathrm{~cm}\) tall, with hinges mounted on the vertical edge. A small 150 - \(\mathrm{g}\) handle is mounted \(45 \mathrm{~cm}\) from the lower hinge at the same height as that hinge. If the density of the plywood is \(550 \mathrm{~kg} / \mathrm{m}^{3},\) what is the moment of inertia of the door about the hinges? Neglect the contribution of hinge components to the moment of inertia.

A machine part is made from a uniform solid disk of radius \(R\) and mass \(M\). A hole of radius \(R / 2\) is drilled into the disk, with the center of the hole at a distance \(R / 2\) from the center of the disk (the diameter of the hole spans from the center of the disk to its outer edge). What is the moment of inertia of this machine part about the center of the disk in terms of \(R\) and \(M ?\)

A space station is to provide artificial gravity to support long-term stay of astronauts and cosmonauts. It is designed as a large wheel, with all the compartments in the rim, which is to rotate at a speed that will provide an acceleration similar to that of terrestrial gravity for the astronauts (their feet will be on the inside of the outer wall of the space station and their heads will be pointing toward the hub). After the space station is assembled in orbit, its rotation will be started by the firing of a rocket motor fixed to the outer rim, which fires tangentially to the rim. The radius of the space station is \(R=50.0 \mathrm{~m},\) and the mass is \(M=2.40 \cdot 10^{5} \mathrm{~kg} .\) If the thrust of the rocket motor is \(F=1.40 \cdot 10^{2} \mathrm{~N},\) how long should the motor fire?

An ice skater rotating on frictionless ice brings her hands into her body so that she rotates faster. Which, if any, of the conservation laws hold? a) conservation of mechanical energy and conservation of angular momentum b) conservation of mechanical energy only c) conservation of angular momentum only d) neither conservation of mechanical energy nor conservation of angular momentum

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.