The Meandering Current Mobility Model and its Impact on Underwater Mobile Sensor Network November 25, 2008 TaeSeob ,Yun KAIST DATABASE & MULTIMEDIA LAB
The Meandering Current Mobility Model and its Impact on Underwater
Mobile Sensor Network
November 25, 2008
TaeSeob ,YunKAIST
DATABASE & MULTIMEDIA LAB
DATABASE & MULTIMEDIA LAB 2November 25, 2008
Contents
Introduction
Mobility Model
Network Model
Localization
Conclusion
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Introduction(1/4)
Needs for Underwater Environment Monitoring Military surveillance Oceanographic data collection Ecology Public safety Industry
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Introduction(2/4) Features of Underwater Envi-
ronment Immense volume of the
underwater domain Impossible to use dense
deployment Meandering currents Limitations of signal uses
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Introduction(3/4)
Ways to Perform Measurements in the Oceans Eulerian
Data is taken at positions that do not change in time
LagrangianData is taken from autonomous devices that
passively follow the ocean currents
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Introduction(4/4) Recent Work with Network Capability
Data gathering[Vas05] Synchronization[Sye06] Localization[Cha06] Routing protocols[Pom05] [Xie06] Energy minimization [Chi07] MAC [Mak06]
This paper study Underwater mobile acoustic sensor networks that consist
of free floating sensors with network capability
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Mobility Model(1/6) Mobility Model
Description of the fluid nature of the medium in which interconnected sensors move
Typical mobile sensor network Sensor move independently Random walk process Random waypoint process
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Mobility Model(2/6) Case of Fluids - the same velocity field advects all
the sensors Paths are deterministic Strong correlations between nearby sensors
Ocean forecasts Depends on the level of realism Atmospheric forcing Bottom topography Boundary conditions
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Mobility Model(3/6) Lagrangian transport [Ott89][Sam06]
Stratified movement Rotating fluid Drifter- a buoyant object floating near the surface Ignore vertical movements
Wind-driven upwelling/downwelling Exceptionally intense internal waves
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Mobility Model(4/6)
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k = number of meanders in the unit lengthc: phase speed with which they shift downstreamB: modulates the width of the meandersA: average meander widthe: amplitude of the modulationω: frequency of e(A = 1.2, c = 0.12, k = 2π/7.5, ω = 0.4, e= 0.3)
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Mobility Model(5/6)
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Mobility Model(6/6)
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Network Model(1/9)
Time varying graph G = (V(t), E(t))
V(t): sensor nodes moving in a rectangular domain at time t
E(t): communication link between sensorsCommunication link: if a node can send a packet
to another node
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Network Model(2/9) Successful reception of a transmission depends on
Received signal strength Interference caused by simultaneously transmitting
nodes Ambient noise level
Particularly affect acoustic underwater communica-tion Shadowing Reflection Scattering diffraction
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Network Model(3/9) Homogeneous sensor network
Maximum communication range (Rc=1000m)
Deployment Domain: initially, deploy in the square [0,4]x[-2,2]km
to [0,80]x[-4,4]km Scenarios
Single deployment k-phase deployments
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Network Model(4/9) LCC(Largest Connected Component)
LCC(t) is the set of sensors in the largest connected component at time t
Disruption and delay tolerant networking(DTN) can be used to overcome [Fal03] Probability that communication graph G is parti-
tioned in several connected components Communications require multiple hops
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Network Model(5/9)
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Network Model(6/9)
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Network Model(7/9) Coverage
Area Coverage The area coverage of a sensor network at time t, fa(t)
is the fraction of the geographical area covered by one or more sensors at time t
Area Coverage over a time-interval The area coverage of a mobile sensor network during
the time interval [0,t), fm(t) is the fraction of the geo-graphical area covered by at least one sensor at some point of time within [0,t)
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Network Model(8/9)
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Network Model(9/9)
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Localization(1/3)
Most underwater sensor network applications require location infor-mation for data tagging
Cannot use GPS because the high frequency sig-nal does not propagate well through water
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Localization(2/3) Use a set of initial beacons [Ero07]
Sound sources Special devices placed in the ocean emitting signals
Dive and Rise The nodes have the ability to move vertically, get the
GPS coordinates and distribute
Localization Process A beacon distributes its coordinates to its neighbors Estimates coordinates by signals from 3 beacons
Assume that z coordinate to be calculated by a pres-sure sensor
Metric: Time of Arrival(ToA)
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Localization(3/3)
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Conclusion Contribution
First physically-inspired mobility modelAnalysis of mobile underwater sensor net-
worksCould be exploited in the design of underwa-
ter sensor networks
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References [Vas05] I. Vasilescu, K. Kotay, D. Rus, M. Dunbabin, and P. Corke, “Data collection, storage,
and retrieval with an underwater sensor network,” in SenSys’05, San Diego, California, USA, 2005, pp. 154–165.
[Sye06] A. Syed and J. Heidemann, “Time synchronization for high latency acoustic net-works,” in Proc. of Infocom, Barcelona, Spain, April 2006, pp. 1–12.
[Cha06] V. Chandrasekhar, W. K. Seah, Y. S. Choo, and H. V. Ee, “Localization in underwater sensor networks: survey and challenges,” in WUWNet ’06, Los Angeles, CA, USA, 2006, pp. 33–40.
[Pom05] D. Pompili and T. Melodia, “Three-dimensional routing in underwater acoustic sensor networks,” in PE-WASUN ’05: Proc. of the 2nd ACM Int. workshop on Performance evaluation of wireless ad hoc, sensor, and ubiquitous networks, Montreal, Quebec, Canada, 2005, pp. 214–221.
[Xie06] P. Xie, J. Cui, and L. Lao, “Vbf: Vector-based forwarding protocol for underwater sen-sor networks,” in In Proc. of IFIP Networking’06, Portugual, May 2006, pp. 1216–1221.
[Chi07] N. Chirdchoo, W.-S. Soh, and K. C. Chua, “Aloha-based mac protocols with collision avoidance for underwater acoustic networks,” in INFOCOM 2007, Anchorage, Alaska, USA, May 2007, pp. 2271–2275.
[Mak06] D. Makhija, P. Kumaraswamy, and R. Roy, “Challenges and design of mac protocol for underwater acoustic sensor networks,” in 4th International Symposium on Modeling and Optimization in Mobile, Ad Hoc and Wireless Networks, Boston, Massachusetts, USA, 03-06 April 2006, pp. 1–6.
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References [Ott89] J. M. Ottino, The Kinematics of Mixing: Stretching, Chaos, and Transport, ser. Cam-
bridge Texts in Applied Mathematics. Cambridge University Press, 1989, no. 3. [Sam06] R. M. Samelson and S. Wiggins, Lagrangian Transport in Geophysical Jets and
Waves. The Dynamical Systems Approach, ser. Interdisciplinary Applied Mathematics. Springer-Verlag, 2006, no. 31
[Fal03] K. Fall, “A delay-tolerant network architecture for challenged internets,” in SIG-COMM ’03, Karlsruhe, Germany, 2003, pp. 27–34.
[Ero07] M. Erol, L. Vieira, and M. Gerla, “Localization with divenrise (dnr) beacons for un-derwater sensor networks,” in to be presented in WUWnet’07, 2007
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