Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Automobile handling
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
=== Unsprung weight === {{Main|Unsprung weight}} [[File:Car diagram.jpg|right]] Ignoring the flexing of other components, a car can be modeled as the sprung weight, carried by the springs, carried by the [[unsprung weight]], carried by the tires, carried by the road. Unsprung weight is more properly regarded as a [[mass]] which has its own inherent [[inertia]] separate from the rest of the vehicle. When a wheel is pushed upwards by a bump in the road, the inertia of the wheel will cause it to be carried further upward above the height of the bump. If the force of the push is sufficiently large, the inertia of the wheel will cause the tire to completely lift off the road surface resulting in a loss of traction and control. Similarly when crossing into a sudden ground depression, the inertia of the wheel slows the rate at which it descends. If the wheel inertia is large enough, the wheel may be temporarily separated from the road surface before it has descended back into contact with the road surface. This unsprung weight is cushioned from uneven road surfaces only by the compressive resilience of the tire (and wire wheels if fitted), which aids the wheel in remaining in contact with the road surface when the wheel inertia prevents close-following of the ground surface. However, the compressive resilience of the tire results in [[rolling resistance]] which requires additional kinetic energy to overcome, and the rolling resistance is expended in the tire as heat due to the flexing of the rubber and steel bands in the sidewalls of the tires. To reduce rolling resistance for improved [[Fuel economy in automobiles|fuel economy]] and to avoid overheating and failure of tires at high speed, tires are designed to have limited internal damping. So the "wheel bounce" due to wheel inertia, or resonant motion of the unsprung weight moving up and down on the springiness of the tire, is only poorly damped, mainly by the dampers or [[shock absorber]]s of the suspension. For these reasons, high unsprung weight reduces road holding and increases unpredictable changes in direction on rough surfaces (as well as degrading [[ride quality|ride comfort]] and increasing mechanical loads). This unsprung weight includes the wheels and tires, usually the [[brake]]s, plus some percentage of the suspension, depending on how much of the suspension moves with the body and how much with the wheels; for instance a [[solid axle]] suspension is completely unsprung. The main factors that improve unsprung weight are a sprung differential (as opposed to [[live axle]]) and [[inboard brake]]s. (The [[De Dion tube]] suspension operates much as a live axle does, but represents an improvement because the differential is mounted to the body, thereby reducing the unsprung weight.) Wheel materials and sizes will also have an effect. [[Aluminium]] [[alloy wheels]] are common due to their weight characteristics which help to reduce unsprung mass. [[Magnesium alloy wheel]]s are even lighter but corrode easily. Since only the brakes on the driving wheels can easily be inboard, the [[Citroën 2CV]] had inertial dampers on its rear wheel hubs to damp only wheel bounce.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)