Skip to main content Accessibility help
×
Hostname: page-component-586b7cd67f-g8jcs Total loading time: 0 Render date: 2024-11-29T02:39:45.653Z Has data issue: false hasContentIssue false

Chapter XVI - MISCELLANEOUS PROBLEMS

Published online by Cambridge University Press:  07 September 2010

Get access

Summary

16.·1. Rolling and Sliding. When sliding takes place the friction F bears a constant ratio μ to the normal reaction R but when rolling takes place the friction has generally a much smaller value.

When two bodies in contact at a point A have a relative motion the process of determining whether this motion involves rolling or sliding at A is as follows:

Write down the equations of motion which involve the friction F and the normal reaction R, and assuming

(i) that rolling takes place also write down the kinematical condition which expresses the fact that there is no relative tangential velocity at A. If from the solution of these equations we find that F/R is less than the coefficient of friction μ, the assumption that rolling takes place is justified and rolling will continue until F/R becomes greater than μ.

(ii) Assuming that sliding takes place, write μR instead of F in the equations of motion and solve the equations without the kinematical condition above referred to. If the solution shews that there is a relative tangential velocity at A and the direction of motion is opposed to what has been assumed as the direction of the friction then we have found the true motion and it will continue until relative velocity at A vanishes.

16·2. A wheel spinning about a horizontal axis is projected along a rough horizontal plane, to determine the subsequent motion.

Let m be the mass and a the radius of the wheel, mκ2 its moment of inertia about its centre G, and A the point of contact with the plane.

Type
Chapter
Information
Dynamics
A Text-Book for the Use of the Higher Divisions in Schools and for First Year Students at the Universities
, pp. 231 - 246
Publisher: Cambridge University Press
Print publication year: 2009
First published in: 1929

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

Save book to Kindle

To save this book to your Kindle, first ensure [email protected] is added to your Approved Personal Document E-mail List under your Personal Document Settings on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part of your Kindle email address below. Find out more about saving to your Kindle.

Note you can select to save to either the @free.kindle.com or @kindle.com variations. ‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi. ‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.

Find out more about the Kindle Personal Document Service.

Available formats
×

Save book to Dropbox

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Dropbox.

Available formats
×

Save book to Google Drive

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Google Drive.

Available formats
×