{composition-setup}{composition-setup} {table:border=1|frame=void|rules=cols|cellspacing=0|cellpadding=8} {tr:valign=top} {td:width=25|bgcolor=#F2F2F2} {live-template:Left Column} {td} {td} h1. Kinetic Friction {excerpt}The specific manifestation of [friction] that is directly opposed to an object's sliding motion along a surface. The force of kinetic friction has a size independent of the speed of the object, and proportional to the [normal force] exerted on the object by the surface.{excerpt} h3. Kinetic Friction as a Force h4. Magnitude For an object that is already sliding along a surface or is accelerating from rest on a surface, the size of the friction force will be given by: {latex}\begin{large}\[ F_{k} = \mu_{k} N\]\end{large}{latex} {note}Note that the size of the kinetic friction is fixed by the normal force and the coefficient. In contrast to the case of [static friction], there is no upper limit in the expression. Thus, it is not necessary to consider the complete net force to find the friction force for the kinetic case.{note} where μ~k~ is the *coefficient of kinetic friction*. The coefficient of kinetic friction is a dimensionless number, usually less than 1.0 (but _not_ required to be less than 1.0). Rough or sticky surfaces will yield larger coefficients of friction than smooth surfaces. _N_ is the [normal force] exerted on the object _by the surface which is creating the friction_, which is a measure of the strength of the contact between the object and the surface. The coefficient of kinetic friction for a given object on a given surface will usually be *different* than the corresponding coefficient of static friction. It is usually the case that μ~k~ < μ~s~. h4. Direction There are two possibilities to consider when determining the direction of kinetic friction: # For a sliding object, the direction of the kinetic friction must be opposite to the direction of the velocity. # For an object just beginning to slide (the object still has zero velocity) then the friction must oppose the acceleration. h3. Kinetic Friction as Non-Conservative Work When an object is sliding on a surface that can be considered to be at rest in an [inertial frame of reference|inertial reference frame], kinetic friction is the prototypical [non-conservative force]. When the motion of an object sliding on a surface is viewed from a frame at rest with respect to the surface, the force of friction always opposes the object's motion, and so always does negative [work]. For the case of a constant friction force, the definition of [work] can be integrated to give: {panel:title=Work done by a Constant Friction Force}{latex}\begin{large}\[W_{f} = -F_{k}d\]\end{large}{latex}{panel} where _d_ is the *distance* traveled by the object along the surface. {info}Contrast this with a conservative force like [gravity (near-earth)], which does negative [work] on an object that is rising, and then returns energy by doing positive [work] on the object as it falls.{info} {warning}The [work] done by [friction] becomes very confusing when a reference frame is chosen in which the surface is _moving_. See the discussion of [static friction] for more details.{warning} h3. {toggle-cloak:id=examples}Example Problems involving Kinetic Friction {cloak:id=examples} {contentbylabel:kinetic_friction,example_problem|operator=AND|maxResults=50|showSpace=false|excerpt=true} {cloak:examples} {td} {tr} {table} {live-template:RELATE license} |