Abstract
In gravity below Earth normal, a person should be able to take higher leaps in running. We asked ten subjects to run on a treadmill in five levels of simulated reduced gravity and optically tracked center of mass kinematics. Subjects consistently reduced ballistic height compared to running in normal gravity. We explain this trend by considering the vertical takeoff velocity (defined as maximum vertical velocity). Energetically optimal gaits should balance energetic costs of ground-contact collisions (favouring lower takeoff velocity), and step frequency penalties such as leg swing work (favouring higher takeoff velocity, but less so in reduced gravity). Measured vertical takeoff velocity scaled with the square root of gravitational acceleration, following energetic optimality predictions and explaining why ballistic height decreases in lower gravity. The success of work-based costs in predicting this behaviour challenges the notion that gait adaptation in reduced gravity results from an unloading of the stance phase. Only the relationship between takeoff velocity and swing cost changes in reduced gravity; the energetic cost of the down-to-up transition for a given vertical takeoff velocity does not change with gravity. Because lower gravity allows an elongated swing phase for a given takeoff velocity, the motor control system can relax the vertical momentum change in the stance phase, so reducing ballistic height, without great energetic penalty to leg swing work. While it may seem counterintuitive, using less “bouncy” gaits in reduced gravity is a strategy to reduce energetic costs, to which humans seem extremely sensitive.
Summary Statement During running, humans take higher leaps in normal gravity than in reduced gravity, in order to optimally balance the competing costs of stance and leg-swing work.
List of Symbols
- θ
- leg angle (radians)
- ω0
- vertical natural angular frequency in the spring-mass model (radians s−1)
- A
- proportionality constant in the relationship Efreq = Afk (J sk)
- B
- proportionality constant in the relationship
- Ecol
- energetic cost of collisions (J)
- Efreq
- energetic cost related to step-frequency (J)
- Eswing
- energetic cost of leg swing work (J)
- Etot
- total energetic cost (Ecol + Efreq or Ecol + Eswing, in J)
- f
- step frequency (Hz)
- fn
- natural pendular frequency (Hz)
- g
- gravitational acceleration (m s−2)
- G
- Earth-normal gravitational acceleration (9.8 m s−2)
- Gr
- Groucho number (≡ νw0/g)
- H
- ballistic height (m)
- I
- leg moment of inertia about the hip (kg m2)
- k
- exponent in proportionality Efreq ∝ fk
- l
- leg length (m)
- m
- total subject mass (kg)
- r
- length change from leg rest length (m)
- t
- time after toe-down (s)
- t*
- time at which maximum vertical speed is achieved (s)
- tm
- time at which maximum vertical velocity is achieved (s)
- ts
- stance period (s)
- U
- average horizontal speed (m s−1)
- ν
- vertical velocity at toe-off (m s−1)
- V
- vertical velocity at takeoff (maximum vertical velocity,in m s−1)
- V*
- optimal and predicted vertical takeoff velocity (m s−1)