The Capacity of Wireless Networks

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Presentation transcript:

The Capacity of Wireless Networks Chi Zhang Wireless Networks Laboratory (WINET) Department of Electrical & Computer Engineering University of Florida

Outline The Capacity of Arbitrary Networks The Capacity of Random Geometric Networks References: P. Gupta and P. R. Kumar, The Capacity of Wireless Networks, IEEE Transactions on Information Theory, vol. 46, no. 2, pp. 388-404, March 2000. A. Agarwal and P. R. Kumar, Capacity bounds for ad hoc and hybrid wireless networks, ACM SIGCOMM Computer Communications Review, vol. 34, no. 3, pp.71-81, July 2004. F. Xue and P. R. Kumar, Scaling Laws for Ad Hoc Wireless Networks: An Information Theoretic Approach, NOW Publishers, Delft, The Netherlands, 2006.

Corrections to the Capacity Paper

Arbitrary Networks Node location is arbitrary: n nodes are arbitrarily located in a disk of area A m2 in the plane. Traffic pattern is arbitrary: each node has an arbitrarily chosen destination to which it wishes to send traffic at an arbitrary rate. Transmission power is arbitrary: each node can choose an arbitrary range or power level for each transmission.

Models for Successful Reception in MAC Layer The protocol model: specifies the condition of successful transmission in terms of geometry. The physical model: specifies the condition of successful transmission in terms of SINR. The physical model

Protocol Model

Physical Model

Generalized Physical Model Data rate is generalized to be continuous in SINR, based on Shannon's capacity formula for the additive Gaussian noise channel.

Transport Capacity of arbitrary Networks

Transport Capacity of arbitrary Networks

Transport Capacity of arbitrary Networks The transport capacity of arbitrary networks is achieved when the network is jointly optimized. Only the distance between the original source and the final destination counts. We do not consider multicast or broadcast cases.

Main Results for Arbitrary Networks For Protocol Model

Main Results for Arbitrary Networks For Physical Model

Upper-Bound under the Protocol Model Main ideas behind the proof: The essential idea to upper-bound the transport capacity in the proof below is to observe that successful transmissions consume area as they happen. Moreover the radius of such a consumed area is proportional to the transmission range. Since the sum of such areas is upper-bounded by the limited total area A, it follows from invoking the convexity of quadratic function, that one can transform this upper-bound into an upper-bound for the bit-meters per second --- the transport capacity.

Upper-Bound under the Protocol Model

Upper-Bound under the Protocol Model

Upper-Bound under the Protocol Model

Upper-Bound under the Protocol Model Sum of areas of exclusion disks is upper-bounded by A.

Upper-Bound under the Protocol Model

Lower-Bound under the Protocol Model A Constructive Lower Bound on Transport Capacity for Arbitrary Networks under the Protocol Model We need to show the upper-bound just obtained is a tight one, which means we need to give an example to show that this upper-bound is achievable.

Lower-Bound under the Protocol Model

Discussion on the result

Transport Capacity under the Physical Model we consider a more physical criterion for successful reception specified by the requirement on the signal to interference plus noise ratio (SINR) --- called the Physical Model. Since common radio technology for decoding a packet works only if the SINR is sufficiently large, this model is more faithful to physical considerations. The Protocol Model stipulates local, geometric constraints, while in the Physical Model every transmission influences every reception. They thus seem very different from each other, but, interestingly, as shown by the following result, there is a correspondence between them.

Upper-Bounds under the Physical Model General Cases

Upper-Bounds under the Physical Model

Upper-Bounds under the Physical Model

Upper-Bounds under the Physical Model

Lower-Bound under the Physical Model