Coefficient of restitution

From Wikipedia, the free encyclopedia

A bouncing ball captured with a stroboscopic flash at 25 images per second. Ignoring air resistance, the square root of the ratio of the height of one bounce to that of the preceding bounce gives the coefficient of restitution for the ball/surface impact.
A bouncing ball captured with a stroboscopic flash at 25 images per second. Ignoring air resistance, the square root of the ratio of the height of one bounce to that of the preceding bounce gives the coefficient of restitution for the ball/surface impact.

The coefficient of restitution or COR of an object is a fractional value representing the ratio of velocities before and after an impact. An object with a COR of 1 collides elastically, while an object with a COR of 0 will collide inelastically, effectively "sticking" to the object it collides with, not bouncing at all.

Contents

[edit] Common usage

The coefficient of restitution entered the common vocabulary, among golfers at least, when golf club manufacturers began making thin-faced drivers with a so-called "trampoline effect" that creates drives of a greater distance as a result of an extra bounce off the clubface. The USGA (America's governing golfing body) has started testing drivers for COR and has placed the upper limit at 0.83. Golf balls also have a COR of about 0.78.[1] According to one article (addressing COR in tennis racquets), "[f]or the Benchmark Conditions, the coefficient of restitution used is 0.85 for all racquets, eliminating the variables of string tension and frame stiffness which could add or subtract from the coefficient of restitution."[2]

The International Table Tennis Federation specifies that the ball must have a coefficient of restitution of 0.94.[3]

[edit] Equation

The coefficient itself is given by:

C_R = \frac{V_{2f} - V_{1f}}{V_{1} - V_{2}}

for two colliding objects, where

V1f is the scalar final velocity of the first object after impact
V2f is the scalar final velocity of the second object after impact
V1 is the scalar initial velocity of the first object before impact
V2 is the scalar initial velocity of the second object before impact

Since velocity is a vector, a direction must be labeled "positive" and the opposite direction "negative". Even though the equation does not reference mass, it is important to note that it still relates to momentum since the final velocities are dependant on mass.

For an object bouncing off a stationary object, such as a floor:

C_R = \frac{V_{f}}{V_{i}}, where
Vf is the scalar velocity of the object after impact
Vi is the scalar velocity of the object before impact

The coefficient can also be found with:

C_R = \sqrt{\frac{h}{H}}

for an object bouncing off a stationary object, such as a floor, where

h is the bounce height
H is the drop height

Note that the velocities used are scalar products pointing along the direction of impact (or perpendicular to the tangential vector of the point of contact, if you prefer). For spheres, this direction would be pos2 − pos1 normalized, where posx is the position of the xth sphere. A simple dot product can then be used between this vector and the velocity vector to find the scalars.

[edit] Further details

The COR is generally a number in the range [0,1]. Qualitatively, 1 represents a perfectly elastic collision, while 0 represents a perfectly inelastic collision. A COR greater than one is theoretically possible, representing a collision that generates kinetic energy, such as land mines being thrown together and exploding. For other examples, some recent studies have clarified that COR can take a value greater than one in a special case of oblique collisions[1][2][3]. These phenomena are due to the change of rebound trajectory of a ball caused by a soft target wall. A COR less than zero is also theoretically possible, representing a collision that pulls two objects closer together instead of bouncing them apart.

An important point: the COR is a property of a collision, not necessarily an object. For example, if you had 5 different types of objects colliding, you would have {5 \choose 2} = 10 different CORs (ignoring the possible ways and orientations in which the objects collide), one for each possible collision between any two object types.

[edit] Use

The equations for collisions between elastic particles can be modified to use the COR, thus becoming applicable to inelastic collisions as well, and every possibility in between.

V_{1f}=\frac{(C_R + 1)M_{2}V_2+V_{1}(M_1-C_R M_2)}{M_1+M_2}
and
V_{2f}=\frac{(C_R + 1)M_{1}V_1+V_{2}(M_2-C_R M_1)}{M_1+ M_2}

where

V1f is the final velocity of the first object after impact
V2f is the final velocity of the second object after impact
V1 is the initial velocity of the first object before impact
V2 is the initial velocity of the second object before impact
M1 is the mass of the first object
M2 is the mass of the second object

[edit] Derivation

The above equation can be derived from the analytical solution to the system of equations generated by the definition of the COR and the law of the conservation of momentum (which holds for all collisions):

\begin{cases} M_{1}V_{1f} + M_{2}V_{2f} = (M_{1}V_{1} + M_{2}V_{2})\\ -V_{1f} + V_{2f} = C_R(V_{1} - V_{2}) \end{cases}

[edit] See also

[edit] References

  1. ^ Everything You Need to Know About COR.
  2. ^ Coefficient of Restitution.
  3. ^ Table Tennis / Essentials During Action Proper at SportsTM. Accessed January 2008.
  • Cross, Rod (2006). "The bounce of a ball". Physics Department, University of Sydney, Australia. “In this paper, the dynamics of a bouncing ball is described for several common ball types having different bounce characteristics. Results are presented for a tennis ball, a baseball, a golf ball, a superball, a steel ball bearing, a plasticene ball, and a silly putty ball.” 

[edit] External links