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Jeff Koechling

dblp:58/1618 · DBLP profile ↗
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1ranked-venue papers
0as first author
0since 2021 · last 1994
—ORCID · none

Domains — the database's venue-derived domains; a paper can count in several

Artificial intelligence and machine learning · 1Systems, architecture and hardware · 1

Expertise — from the expertise taxonomy: the topics of the expert's papers under the CCF categories. A weight counts papers with recency: 1 for a paper about the topic, 0.3 when the topic is its context, halved every five years.

Computer graphics and multimedia
1 paper
Computer animation and physical simulation · 100%

Topics — the 3 heaviest of 3, each with the papers that count most for it

TopicWeightPapersLastEvidence papers
Computer animation and physical simulation › contact simulation
frictional contact
0.011994
Classifying Dynamic Behavior During Three Dimensional Frictional Rigid Body Impact · ICRA 1994
Computer animation and physical simulation › contact simulation
impact dynamics
0.011994
Classifying Dynamic Behavior During Three Dimensional Frictional Rigid Body Impact · ICRA 1994
Computer animation and physical simulation
rigid body simulation
0.011994
Classifying Dynamic Behavior During Three Dimensional Frictional Rigid Body Impact · ICRA 1994

Methods — techniques the papers use, named apart from their topics

poisson restitution · 0.0flow analysis · 0.0coulomb friction · 0.0
YearPublicationVenuePosition
1994 Classifying Dynamic Behavior During Three Dimensional Frictional Rigid Body Impact
abstract
We model and analyze three dimensional rigid body impact with Coulomb friction and Poisson restitution. The differential equations that describe the progress and outcome of the impact induce a flow in the tangent velocity space which defines the qualitatively different sliding behavior that can occur. We show that the flow patterns depend only on the inertial parameters at the point of contact. We associate each of the possible flow patterns with a distinct region in a three dimensional parameter space. By examining the mass parameters and the initial conditions, we can determine the corresponding flow pattern and the possible outcomes of the impact. The equations of motion cannot be solved in a closed form, but by analyzing the flow at the point of sticking, we can avoid instabilities in the numerical integration of the equations.>
Vivek Bhatt, Jeff Koechling
ICRA2