If muscles are viewed as spring-like torque generators, then the integ
ral of torque with respect to joint angle is the potential energy of t
hat muscle. An energy function for the musculoskeletal system can be d
efined by summing the energy contribution of each muscle and the poten
tial energy stored in the limb. Any local minimum in this energy lands
cape is a possible equilibrium position for the limb. The gradient of
this function with respect to joint angles is a torque field, and the
task of postural control is to find a set of muscle activations to pro
duce a desired field. We consider one technique by which this approxim
ation may be achieved: A postural module is defined as a synergy of mu
scles that produce a class of torque functions that converge at a cons
tant equilibrium position, but whose stiffness at this position varies
as a function of activation of the postural module. For a single-join
t system, we show that through control of two such modules it is possi
ble to produce any stiffness at any desired equilibrium position. To e
xtend this scheme to a multijoint system, we initially derive the mech
anical constraints on the shape of the restoring force field when a mu
ltijoint limb is displaced from equilibrium. Next, we consider volunta
ry control of the force field when the human arm is displaced from equ
ilibrium: Mussa-Ivaldi, Hogan, and Bizzi (1985) have suggested that su
bjects are unable to voluntarily change the shape and orientation of t
he field, although they can readily scale it. This suggests existence
of a limitation on the independent recruitment of arm muscles. We show
, through simulation, that the inability to voluntarily control the sh
ape and orientation of the restoring force field can be attributed to
an organization of postural modules that act as local stiffness contro
llers. We propose that through coactivation, postural modules coarsely
encode the work space and serve as an intermediate control system in
the motor control hierarchy.