Make a sketch showing a situation in which the torque due to a single force about some location is \(20\,\,{\rm{N}} \cdot {\rm{m}}\) in the positive \(z\) direction, whereas about another location the torque is \(10\,\,{\rm{N}} \cdot {\rm{m}}\) in the negative \(z\) direction.

Short Answer

Expert verified

The force that can cause an object to twist along an axis is measured as torque. In linear kinematics, force is what causes an object to accelerate.

Step by step solution

01

Definition of Torque

The force that can cause an object to twist along an axis is measured as torque. In linear kinematics, force is what causes an object to accelerate.

02

Concept about the Torque

The relation describes the torque operating on an object at a specific point.

\(\overrightarrow \tau = \overrightarrow r \times \overrightarrow F \)……. (1)

Here,

\(\overrightarrow r \to \)Position vector of the given location

\(\overrightarrow F \to \)Force vector acting at the location

03

Figure shows the position of force and vector to create a torque

The force and position vectors to create a torque at a given place are depicted in the figure:

04

Find the torque which acting about some location which is given in figure

Let unit vectors along X, Y, X axes are \(\widehat x,\widehat y,\widehat z\)respectively. In order to get torque acting about some location is, \(\tau = 20N \cdot m\)along the positive \(z\)direction, it is essential to consider, the position vector of that location is along the positive \(X\)axis\(\overrightarrow r = (2m)\widehat x\)and force vector acting along the positive \(Y\)axis, \(\overrightarrow F = (10N)\widehat y\)

Using equation (1), torque acting about some location is given by,

\(\begin{aligned}{}\overrightarrow \tau &= \overrightarrow r \times \overrightarrow F \\ &= (2m)\widehat x \times (10N)\widehat y\\ &= (2N \cdot m)(\widehat x \times \widehat y)\\ &= (2N \cdot m)\widehat z\,\,\,\,\,\,\,\,\,\,\,\,\,\,as\,(\widehat x \times \widehat y) = \widehat z)\end{aligned}\)

In order to get torque acting about another location is, \(\tau = 10N \cdot m\)along the negative \(z\)direction, it is essential to consider, the position vector of that location is along the negative \(X\)-axis \(\overrightarrow r = (1m)( - \widehat x)\)and same force vector acting along the positive \(Y\)axis, \(\overrightarrow F = (10N)\widehat y\).

Using equation (1), torque acting about another location is given by,

\(\begin{aligned}{}\overrightarrow \tau & = \overrightarrow r \times \overrightarrow F \\ &= (1m)( - \widehat x) \times (10N)\widehat y\\ &= (10N \cdot m)( - \widehat x \times \widehat y)\\ &= (10N \cdot m)( - \widehat z)\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,As( - \widehat x \times \widehat y) &= - \widehat z)\end{aligned}\)

Torque produced on positive and negative direction is\(2\,\,{\rm{N}}\,{\rm{m}}\) and \( - 10\,\,{\rm{N}}\,{\rm{m}}\) respectively.

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 Vaia!

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 Bohr model currently predicts the main energy levels not only for atomic hydrogen but also for other “one-electron” atoms where all but one of the atomic electrons has been removed, such as in He+ (one electron removed) or (two electrons removed) Li++. (a) Predict the energy levels in for a system consisting of a nucleus containing protons and just one electron. You need no recapitulate the entire derivation for the Bohr model, but do explain the changes you have to make to take into account the factor . (b) The negative muon(μ-) behaves like a heavy electron, with the same charge as the electron but with a mass 207 times as large as the electron mass. As a moving μ- comes to rest in matter, it tends to knock electrons out of atoms and settle down onto a nucleus to form a “one-muon” atom. For a system consisting of a lead nucleus ( Pb208has 82 protons and 126 neutrons) and just one negative muon, predict the energy in of a photon emitted in a transition from the first excited state to the ground state. The high-energy photons emitted by transitions between energy levels in such “muonic atoms” are easily observed in experiments with muons. (c) Calculate the radius of the smallest Bohr orbit for a μ- bound to a lead nucleus ( Pb208has 82 protons and 126 neutrons). Compare with the approximate radius of the lead nucleus (remember that the radius of a proton or neutron is about 1×10-15m, and the nucleons are packed closely together in the nucleus).

Comments: This analysis in terms of the simple Bohr model hints at the results of a full quantum-mechanical analysis, which shows that in the ground state of the lead-muon system there is a rather high probability for finding the muon inside the lead nucleus. Nothing in quantum mechanics forbids this penetration, especially since the muon does not participate in the strong intersection. Electrons in an atom can also be found inside the nucleus, but the probability is very low, because on average the electrons are very far from the nucleus, unlike the muon.

The eventual fate of the μ- in a muonic atom is that it either decays into an electron, neutrino, and antineutrino, or it reacts through the weak interaction with a proton in the nucleus to produce a neutron and a neutrino. This “muon capture” reaction is more likely if the probability is high for the muon to be found inside the nucleus, as is the case with heavy nuclei such as lead.

At t=15s, a particle has angular momentum3,5,-2kg·m2/s relative to locationA . A constant torque10,-12,20N·m relative to locationA acts on the particle. Att=15.1s. what is the angular momentum of the particle?

At a particular instant the location of an object relative to location \(A\) is given by the vector \({\overrightarrow r _A} = \left\langle {6,6,0} \right\rangle {\rm{m}}\). At this instant the momentum of the object is \(\overrightarrow p = \left\langle { - 11,13,0} \right\rangle {\rm{kg}} \cdot {\rm{m}}/{\rm{s}}.\) What is the angular momentum of the object about location \(A\)?

A small rock passes a massive star, following the path shown in red on the diagram. When the rock is a distance 4.5×1013m(indicatedas in figure) from the center of the star, the magnitudeof its momentum is1.35×1017kg·m/sand the angle is126°12. At a later time, when the rock is a distance d2=1.3×1013mfrom the center of the star, it is heading in the -ydirection. There are no other massive objects nearby. What is the magnitude p2of the final momentum?

Review with derivation of the Bohr model of the hydrogen atom and apply this reasoning to predict the energy levels of ionized helium He+ (a helium atom with only one electron, and a nucleus containing two protons and two neutrons). What are the energies in of the ground state and the first excited state? What is the energy of a photon emitted in a transition from the first excited state to the ground state? How do these results differ from those for a hydrogen atom?

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.

Sign-up for free