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A Stochastic Hybrid System Model of Collective
Transport in the Desert Ant Aphaenogaster cockerelli
GANESH P KUMAR1, AURÉLIE BUFFIN2, THEODORE P PAVLIC2,
STEPHEN C PRATT2, SPRING M BERMAN1
1FULTON SCHOOLS OF ENGINEERING / 2SCHOOL OF LIFE SCIENCES
ARIZONA STATE UNIVERSITY
Motivation for Engineers
Developing robust strategies for Multi-Robot Collective Transport
 No prior information about load or obstacles
 Applications: Construction, Search & Rescue, Manufacturing
 Swarms in nature inspire swarm robot control strategies
Khepera III Robots (K-Team) Search & Rescue
http://tiny.cc/pf4yuw
)
Construction
http://tiny.cc/204yuw
Motivation for Biologists
Understanding collective transport in certain ant species
Aphaenogaster cockerelli
carrying lexan structure
Prior Work
Collective Transport in Ants
 Berman et.al. Proc. IEEE, Sep 2011
 Czaczkes and Ratnieks, Myrmecol. News, 2013
Polynomial Stochastic Hybrid Systems (pSHS)
 Hespanha and Singh, Intl. J. Robust Nonlinear Control, Oct 2005
pSHS Models of Multi-Robot Systems
 Mather and Hsieh, Proc. RSS, June 2011
 Napp et.al, Proc. RSS, June 2009
Experiments: Ants Transporting Load
 17 Video-recorded trials of ants carrying foam-mounted dime
 Segments spanning 145s extracted from each video
 Ant positions and load trajectory tracked using ImageJ and Mtrack plugin
Observations
 Load trajectory was typically almost straight
 Random switches among 3 states: Front, Back,
Detached
 Ants lift load with force 𝐹𝐿≈2.65 mN, measured
with load cell Back
Detached
Front
Polynomial Stochastic Hybrid System Model
Front
Back
 State vector 𝐱 = 𝑁𝐹 𝑁 𝐵 𝑁 𝐷 𝑥 𝐿 𝑣 𝐿
𝑇
 Behavioural states: S = 𝐹, 𝐵, 𝐷
 Population counts: 𝑁𝑖∈𝑆
 Dynamical variables: 𝑥 𝐿, 𝑣 𝐿
 Flow equation d𝐱/d𝑡 = 0 0 0 𝑣 𝐿 𝑎 𝐿
𝑇
 6 Transitions: 𝑋𝑖 → 𝑋𝑗, with rate 𝑟𝑖𝑗
 Transition intensity: 𝜆𝑖𝑗 = 𝑟𝑖𝑗 𝑁𝑖
 Reset map: 𝑁𝑖, 𝑁𝑗 ↦ (𝑁𝑖 − 1, 𝑁𝑗 + 1)
Detached
F
BD
𝑟 𝐷𝐵, 𝑟𝐵𝐷
𝑟 𝐷𝐹, 𝑟𝐹𝐷 𝑟𝐹𝐵, 𝑟𝐵𝐹
Back Front
𝑣 𝐿
Detached
↦ 𝑥 𝐿
pSHS : Load Dynamics
 Front and back ants lift with net force:
𝐹𝑢𝑝 = 𝑁𝐹 + 𝑁 𝐵 𝐹𝐿
 Normal force: 𝐹𝑛 = 𝑚 𝐿 𝑔 − 𝐹𝑢𝑝
 Front ants pull with velocity regulation
 Proportional gain: 𝐾
 Velocity set point: 𝑣 𝐿
𝑑
 Individual pulling force: 𝐹𝑝 = 𝐾(𝑣 𝐿
𝑑
− 𝑣 𝐿)
LOAD
𝑚 𝐿 𝑔
𝑁 𝐹 𝐹𝑝𝜇𝐹𝑛
𝐹𝑟𝑜𝑛𝑡
𝐹𝑢𝑝 + 𝐹𝑛
𝐵𝑎𝑐𝑘
𝑥 𝐿 = 𝑣 𝐿
𝑚 𝐿 𝑣 𝐿 = 𝑁𝐹 𝐹𝑝 − 𝜇𝐹𝑛
Moment Dynamics
 Moments computed using extended generator 𝐿
 Key property allows moment computation for differentiable 𝜓:
𝑑
𝑑𝑡
𝐸 𝜓 . = 𝐸 𝐿𝜓
 Time evolution of expectations
𝑑𝐸 𝑁𝑖
𝑑𝑡
=
𝑖,𝑗∈𝑆,𝑖≠𝑗
(𝑟𝑖𝑗 𝐸 𝑁𝑖 − 𝑟𝑗𝑖 𝐸 𝑁𝑗 )
𝑑𝐸(𝑥 𝐿)
𝑑𝑡
= 𝐸 𝑣 𝐿
𝑑𝐸 𝑣 𝐿
𝑑𝑡
= 𝑐 𝑔 + 𝑐 𝐹 𝐸 𝑁𝐹 + 𝑐 𝐵 𝐸 𝑁 𝐵 + 𝑐 𝐹𝑣 𝐸 𝑁𝐹 𝐸(𝑣 𝐿)
 Note: 𝐸 𝑁𝐹 𝑣 𝐿 ≈ 𝐸 𝑁𝐹 𝐸 𝑣 𝐿
For our pSHS, 𝐿 is defined as:
𝐿𝜓(𝐱) ≔
𝜕𝜓
𝜕𝑥 𝐿
𝑥 𝐿 +
𝜕𝜓
𝜕𝑣 𝐿
𝑣 𝐿
+
𝑖,𝑗∈𝑆,𝑖≠𝑗
𝜓 𝜙𝑖𝑗 𝐱 − 𝜓 𝐱 𝑟𝑖𝑗 𝑁𝑖
Fitting Model Parameters
 Rates, units of 𝐬−𝟏
𝑟𝐷𝐵 = 0.0197, 𝑟𝐵𝐷 = 0.0205
𝑟𝐷𝐹 = 0, 𝑟𝐹𝐷 = 0
𝑟𝐹𝐵 = 0.0301, 𝑟𝐵𝐹 = 0.0184
 Proportional gain
𝐾 = 0.0035 N ∙ cm−1
∙s−1
 Velocity set point
𝑣 𝐿
𝑑
= 0.3185 cm∙s−1
𝐀𝐧𝐭 𝐩𝐮𝐥𝐥𝐢𝐧𝐠 𝐟𝐨𝐫𝐜𝐞
𝐹𝑝 = 𝐾 𝑣 𝐿
𝑑
− 𝑣 𝐿
Model Predictions vs. Averaged Data
Model Validation with Individual Trials
Summary
We
 Conducted experiments of ants transporting a load
 Devised a pSHS Model of Collective Transport
 Fit the model parameters to empirical data
Future Work
 Further validate the model, by
 Varying the load mass and coefficient of friction
 Fitting second and higher-order moments to data statistics
 Compare ant transport with optimal strategies
 Criteria: minimize load path variance, transit time, team size
 Extend the model, by incorporating
 Heterogeneity in ants
 State-dependent transition rates
 Two-dimensional load transport
Acknowledgements
 ONR, Wallonie-Bruxelles International: for funding
 Jessica Ebie, Ti Ericksson, Kevin Haight (ASU): for ant collection and care
 Denise Wong, Vijay Kumar (UPenn): for measurement of ant forces
 Sean Wilson (ASU): for valuable feedback on paper and presentation

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Stochastic Hybrid system model for collective transport in desert ant A.cockerelli

  • 1. A Stochastic Hybrid System Model of Collective Transport in the Desert Ant Aphaenogaster cockerelli GANESH P KUMAR1, AURÉLIE BUFFIN2, THEODORE P PAVLIC2, STEPHEN C PRATT2, SPRING M BERMAN1 1FULTON SCHOOLS OF ENGINEERING / 2SCHOOL OF LIFE SCIENCES ARIZONA STATE UNIVERSITY
  • 2. Motivation for Engineers Developing robust strategies for Multi-Robot Collective Transport  No prior information about load or obstacles  Applications: Construction, Search & Rescue, Manufacturing  Swarms in nature inspire swarm robot control strategies Khepera III Robots (K-Team) Search & Rescue http://tiny.cc/pf4yuw ) Construction http://tiny.cc/204yuw
  • 3. Motivation for Biologists Understanding collective transport in certain ant species Aphaenogaster cockerelli carrying lexan structure
  • 4. Prior Work Collective Transport in Ants  Berman et.al. Proc. IEEE, Sep 2011  Czaczkes and Ratnieks, Myrmecol. News, 2013 Polynomial Stochastic Hybrid Systems (pSHS)  Hespanha and Singh, Intl. J. Robust Nonlinear Control, Oct 2005 pSHS Models of Multi-Robot Systems  Mather and Hsieh, Proc. RSS, June 2011  Napp et.al, Proc. RSS, June 2009
  • 5. Experiments: Ants Transporting Load  17 Video-recorded trials of ants carrying foam-mounted dime  Segments spanning 145s extracted from each video  Ant positions and load trajectory tracked using ImageJ and Mtrack plugin
  • 6. Observations  Load trajectory was typically almost straight  Random switches among 3 states: Front, Back, Detached  Ants lift load with force 𝐹𝐿≈2.65 mN, measured with load cell Back Detached Front
  • 7. Polynomial Stochastic Hybrid System Model Front Back  State vector 𝐱 = 𝑁𝐹 𝑁 𝐵 𝑁 𝐷 𝑥 𝐿 𝑣 𝐿 𝑇  Behavioural states: S = 𝐹, 𝐵, 𝐷  Population counts: 𝑁𝑖∈𝑆  Dynamical variables: 𝑥 𝐿, 𝑣 𝐿  Flow equation d𝐱/d𝑡 = 0 0 0 𝑣 𝐿 𝑎 𝐿 𝑇  6 Transitions: 𝑋𝑖 → 𝑋𝑗, with rate 𝑟𝑖𝑗  Transition intensity: 𝜆𝑖𝑗 = 𝑟𝑖𝑗 𝑁𝑖  Reset map: 𝑁𝑖, 𝑁𝑗 ↦ (𝑁𝑖 − 1, 𝑁𝑗 + 1) Detached F BD 𝑟 𝐷𝐵, 𝑟𝐵𝐷 𝑟 𝐷𝐹, 𝑟𝐹𝐷 𝑟𝐹𝐵, 𝑟𝐵𝐹 Back Front 𝑣 𝐿 Detached ↦ 𝑥 𝐿
  • 8. pSHS : Load Dynamics  Front and back ants lift with net force: 𝐹𝑢𝑝 = 𝑁𝐹 + 𝑁 𝐵 𝐹𝐿  Normal force: 𝐹𝑛 = 𝑚 𝐿 𝑔 − 𝐹𝑢𝑝  Front ants pull with velocity regulation  Proportional gain: 𝐾  Velocity set point: 𝑣 𝐿 𝑑  Individual pulling force: 𝐹𝑝 = 𝐾(𝑣 𝐿 𝑑 − 𝑣 𝐿) LOAD 𝑚 𝐿 𝑔 𝑁 𝐹 𝐹𝑝𝜇𝐹𝑛 𝐹𝑟𝑜𝑛𝑡 𝐹𝑢𝑝 + 𝐹𝑛 𝐵𝑎𝑐𝑘 𝑥 𝐿 = 𝑣 𝐿 𝑚 𝐿 𝑣 𝐿 = 𝑁𝐹 𝐹𝑝 − 𝜇𝐹𝑛
  • 9. Moment Dynamics  Moments computed using extended generator 𝐿  Key property allows moment computation for differentiable 𝜓: 𝑑 𝑑𝑡 𝐸 𝜓 . = 𝐸 𝐿𝜓  Time evolution of expectations 𝑑𝐸 𝑁𝑖 𝑑𝑡 = 𝑖,𝑗∈𝑆,𝑖≠𝑗 (𝑟𝑖𝑗 𝐸 𝑁𝑖 − 𝑟𝑗𝑖 𝐸 𝑁𝑗 ) 𝑑𝐸(𝑥 𝐿) 𝑑𝑡 = 𝐸 𝑣 𝐿 𝑑𝐸 𝑣 𝐿 𝑑𝑡 = 𝑐 𝑔 + 𝑐 𝐹 𝐸 𝑁𝐹 + 𝑐 𝐵 𝐸 𝑁 𝐵 + 𝑐 𝐹𝑣 𝐸 𝑁𝐹 𝐸(𝑣 𝐿)  Note: 𝐸 𝑁𝐹 𝑣 𝐿 ≈ 𝐸 𝑁𝐹 𝐸 𝑣 𝐿 For our pSHS, 𝐿 is defined as: 𝐿𝜓(𝐱) ≔ 𝜕𝜓 𝜕𝑥 𝐿 𝑥 𝐿 + 𝜕𝜓 𝜕𝑣 𝐿 𝑣 𝐿 + 𝑖,𝑗∈𝑆,𝑖≠𝑗 𝜓 𝜙𝑖𝑗 𝐱 − 𝜓 𝐱 𝑟𝑖𝑗 𝑁𝑖
  • 10. Fitting Model Parameters  Rates, units of 𝐬−𝟏 𝑟𝐷𝐵 = 0.0197, 𝑟𝐵𝐷 = 0.0205 𝑟𝐷𝐹 = 0, 𝑟𝐹𝐷 = 0 𝑟𝐹𝐵 = 0.0301, 𝑟𝐵𝐹 = 0.0184  Proportional gain 𝐾 = 0.0035 N ∙ cm−1 ∙s−1  Velocity set point 𝑣 𝐿 𝑑 = 0.3185 cm∙s−1 𝐀𝐧𝐭 𝐩𝐮𝐥𝐥𝐢𝐧𝐠 𝐟𝐨𝐫𝐜𝐞 𝐹𝑝 = 𝐾 𝑣 𝐿 𝑑 − 𝑣 𝐿
  • 11. Model Predictions vs. Averaged Data
  • 12. Model Validation with Individual Trials
  • 13. Summary We  Conducted experiments of ants transporting a load  Devised a pSHS Model of Collective Transport  Fit the model parameters to empirical data
  • 14. Future Work  Further validate the model, by  Varying the load mass and coefficient of friction  Fitting second and higher-order moments to data statistics  Compare ant transport with optimal strategies  Criteria: minimize load path variance, transit time, team size  Extend the model, by incorporating  Heterogeneity in ants  State-dependent transition rates  Two-dimensional load transport
  • 15. Acknowledgements  ONR, Wallonie-Bruxelles International: for funding  Jessica Ebie, Ti Ericksson, Kevin Haight (ASU): for ant collection and care  Denise Wong, Vijay Kumar (UPenn): for measurement of ant forces  Sean Wilson (ASU): for valuable feedback on paper and presentation

Editor's Notes

  1. We used these theoretical moment dynamics to fit the free parameters of our model, which are the transition rates , the proportional gain and the velocity set-point.   We computed the average ant populations in each state and the average load position and velocity across trials.  We then used a Weighted Least Squares approach to fit the theoretical expectations at the sampling times to the corresponding empirical averages.  This led to the values shown.    The best-fit transition rates suggest that ants are much more likely to attach to the back of the load than to the front, and they are unlikely to detach from the front once they are there.  We will investigate these hypotheses further in the future. 
  2. /Here we have 5 plots, one for each of the state vector components. Each plot compares the observed mean value with the mean predicted from moment dynamics. The top plots show the population counts; the bottom ones show the load position and velocity.As you can see, the fits are pretty close.
  3. For further validation, we compared the experimental data with the model predictions for individual trials.  For these three sample trials, we show the observed numbers of front and back ants in the first two columns.  The the second two columns show the model predictions of the load position and velocity based on the measured ant counts and the load dynamical model with the best-fit parameters.  There are disparities but the fits are reasonably close.
  4. In summary, we conducted experiments of ants transporting an artificial payload; devise a pSHS model of collective transport, and fit the model parameters to empirical data.
  5. Self explanatory
  6. Say ASU / Upenn