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Actuator Technologies                                         39


              (e.g., only when not moving, or at one-half maximum speed/torque). There
              is, however, an easily accessible metric that incorporates the ability of an
              actuator to achieve any combination of torque, position, speed, and accel-
              eration, in a compact normalizable metric. That metric is the speed ratio—the
              reciprocal of the mechanical time constant (a metric that is often reported in
              actuator specification sheets and is equal to the amount of time for an
              unloaded motor to rise to 63.2% of its final velocity after application of a
              command voltage). The speed ratio can be expressed in various forms, as
              shown in the equation below. Although not well understood and rarely
              used, the speed ratio incorporates each of those four parameters
              (Sensinger, 2010a), and can be used to streamline the design of
              biomechatronic actuators.

                                          K 2   K 2  1
                                     SR ¼   t  ¼  m  ¼
                                          J m R  J m  τ m
              where K t is the torque constant, K m is the motor constant, J m is the inertia of
              the motor, R is the resistance of the motor windings, and τ m is the mechan-
              ical time constant.


              2.2.5 Efficiency
              Efficiency is another useful metric. Efficiency is defined as the amount of
              output power (typically, mechanical) divided by the amount of input power
              (typically, electrical). Peak efficiency for electrical motors does not occur in
              the same region as peak mechanical power—it occurs at higher speeds
              (Alciatore and Histand, 2003). Although efficiency is a useful metric, its
              use as a biomechatronic design metric is often eclipsed by total weight.


              2.2.6 Total Weight
              The total weight of biomechatronic actuators is often an afterthought, but it
              is actually a powerful metric, if used properly (Sensinger, 2010a). Imagine
              that you are trying to compare a series of actuators for a given application,
              and that you have the ability to generate envelope visualizations or access to
              torque and speed densities. The mechanical properties of the task can be used
              to calculate the weight of the actuator needed to perform the task (e.g., if the
              task requires 10Nm of torque, and a particular actuator design has a torque
              density of 10Nm/kg, then your actuator weight is 1kg). The electrical
              requirements of the task can also be calculated. This energy draw can be
              multiplied by the energy density of the supply (e.g., a battery), and added
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