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Title: Haptic%20Deformation%20Modelling%20Through%20Cellular%20Neural%20Network


1
Haptic Deformation Modelling Through Cellular
Neural Network
  • YONGMIN ZHONG, BIJAN SHIRINZADEH, GURSEL ALICI,
    JULIAN SMITH

2
Abstract
  • Haptic - Pertaining to the sense of touch.
  • This paper presents a new methodology for the
    deformation of soft objects by drawing an analogy
    between cellular neural network (CNN) and elastic
    deformation.
  • The potential energy stored in an elastic body as
    a result of a deformation caused by an external
    force is propagated among mass points by
    nonlinear CNN activities.
  • The novelty of the methodology is that soft
    object deformation is carried out from the
    perspective of energy propagation, and nonlinear
    material properties are modelled with nonlinear
    CNNs, rather than geometric nonlinearity as in
    most of the existing deformation methods.

3
Abstract
  • Integration with a haptic device has been
    achieved to simulate soft object deformation with
    force feedback.
  • The proposed methodology not only predicts the
    typical behaviors of living tissues, but also
    easily accommodates isotropic, anisotropic and
    inhomogeneous materials, and local and
    large-range deformation.
  • Isotropic material A material which has the same
    mechanical properties in all directions.
  • Homogeneous material    A material for which
    local variations in composition are negligible in
    comparison with the size of the strain gage
    installed on it to measure strain.
  • Uses - Teleoperators and simulators, Games,
    Virtual Reality, Research, Medicine, Robotics,
    Art and Design.

4
Traditional Approaches
  • Real-time deformation modelling, such as
    Mass-Spring models Zhang et al, 2004 Choi et
    al, 2003 and spline surfaces used for
    deformation visualization and simulation
    Bockholt et al, 1999 Rotnes et al, 2001.
  • Advantage Computation is less time consuming and
    the algorithm is easier to be implemented.
  • Disadvantage Do not allow accurate modelling of
    material properties, and do not give realistic
    feed-back.

5
Traditional Approaches
  • Accurate deformation modelling, such as Finite
    Element Method (FEM) Cotin, 1999 Basdogan,
    2004 and Boundary Element Method (BEM) Jamesand
    Pai, 1999 Monserrat, 2001.
  • In FEM or BEM, rigorous mathematical analysis
    based on continuum mechanics is applied to
    accurately model the mechanical behaviors of soft
    objects. However, these methods are
    computationally expensive and are typically
    simulated off-line.
  • Various Techniques Used to improve computational
    performance.

6
Traditional Approaches
  • In general, most of the existing methods for soft
    object deformation are fully built on a linear
    elastic model to describe the deformation, while
    the behaviors of soft objects such as human
    tissues and organs are extremely nonlinear Fung,
    1993, Kenedi et al, 1975.
  • Advantage Simple to implement and fast to
    calculate.
  • Disadvantage FEM BEM are mainly based on linear
    elastic models.

7
CNN
  • A CNN is a dynamic nonlinear circuit composed by
    locally coupled, spatially recurrent circuit
    units called cells, which contain linear
    capacitors, linear resistors, and
    linear/nonlinear current sources.
  • Intended for image processing and pattern
    recognition.
  • Adjacent cells directly interact with each other.
  • Cells not directly connected to each other have
    indirect effect because of the propagation
    effects of the continuous-time dynamics of a CNN.

8
CNN
  • The activity of a cell is propagated to other
    cells through the local connectivity of cells
    with the evolution of time.
  • In essence, the CNN activity can be treated as a
    process of propagating electrical energy, since a
    CNN is an electrical circuit.

9
Soft Objects
  • Soft object deformation is a process of energy
    propagation. When a soft object is deformed by an
    external force, work is done by the external
    force and the potential energy is also changed.
  • The potential energy is distributed among mass
    points of the object.
  • The potential energy should be zero when the
    object is in its natural state, and the energy
    should grow larger as the object gets
    increasingly deformed away from its natural state
  • According to the law of conservation of energy,
    the change in potential energy is due to the work
    done by the external force
  • Therefore, the deformation process can be treated
    as a process of applying the energy generated by
    an external force to the object, and propagating
    the energy among mass points of the object.

10
The Model
  • The external force is transformed into the
    equivalent electrical energy at the contact
    point.
  • The potential energy stored due to a deformation
    caused by an external force is calculated and
    treated as the energy injected into the system,
    as described by the law of conservation of
    energy.
  • Energy is propagated among mass points through
    nonlinear CNN activities.

11
Local Connectivity
  • Poisson equation is a natural description of
    energy propagation according to the inherent
    property of a material, i.e. the constitutive
    coefficient.
  • Poisson equation describes many steady-state
    application problems in heat transfer, mechanics
    and electromagnetics.
  • Internal forces can be derived as the negative
    gradient of the potential with respect to the
    change in position.

12
The Model
  • When an external force is applied to a soft
    object, the contact point of the external force
    is replaced with a new position. As a result, the
    other points not influenced by the external force
    are in an unstable state.
  • The energy generated by the external force is
    propagated among mass points through the local
    connectivity of cells to establish a new
    equilibrium state by generating the corresponding
    internal forces.
  • Based on the equilibrium state, the new position
    of each point is obtained.
  • The dynamic behavior is governed by the
    Lagrangian equation of motion of each node.

13
Results
14
Results
15
Results
16
Haptic System
17
Haptic System
18
Computational Efficiency
  • The implementation of the proposed methodology
    has been carried out with an Intel Pentium (R)
    2.8GHz and 1.0G memory PC. The computational
    performance is shown in Table 1. From Table 1, it
    can be seen that the computational time is
    increased with the increment of the mesh points.
    The visually satisfactory refresh rate of 25Hz to
    maintain a realistic visual feedback Cotin et
    al, 1999 Picinbono et al, 2002 is achieved by
    meshes with less than about 1200 grid points.
    Since the correct visualization of an object such
    as the human liver requires at least 600 grid
    points Monserrat et al, 2001, it is sufficient
    to provide realistic visual feedback with the
    proposed methodology. In addition, the
    computational speed can be further improved by
    the adaptive remeshing technique Debunne et al,
    2001 and by the digital hardware implementation
    of the CNN algorithm Chua and Yang, 1988.
  • Table 1. Computational performance
  • Numbersof Points 422 602 814 1058 1192
  • GraphicsFrame Rate (Hz) 285.7 142.8 83.3 45.5
    25.6
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