SLIDE 1 Transport Capacity and Spectral Efficiency of Large Wireless CDMA Ad Hoc Networks
Yi Sun Department of Electrical Engineering The City College of City University of New York Acknowledgement: supported by ARL CTA Program
SLIDE 2
Wireless Ad Hoc Network
SLIDE 3 A Fundamental Question
What is the information-theoretical limit
Transport capacity (packet-meters/slot/node) Spectral efficiency (bit-meters/Hz/second/m2)
SLIDE 4 Gupta-Kumar Model (2000)
Assumption
Achievable rate on each link is fixed Effective communications are confined to
nearest neighbors
SLIDE 5
Gupta-Kumar Model (2000)
For an ad hoc network on a unit square, if node density
is D, the number of nodes on a path equals about D½
SLIDE 6 Gupta-Kumar Scaling Law (2000)
Scaling law
As node density D → ∞, transport capacity
converges to zero at rate O(1/D½)
Large scale wireless ad hoc networks are
incapable of information transportation – a pessimistic conclusion
SLIDE 7
Can Scaling Law be Overcome?
SLIDE 8
Gupta-Kumar Model
Communications are confined in nearest
neighbors
Radio frequency bandwidth is not considered
in the model
Spectral efficiency is unknown
SLIDE 9
Observation I
If communications are not confined to nearest
neighbors, transport capacity can be increased
SLIDE 10
Observation II
If CDMA channel is considered and spreading gain (or
bandwidth) is large compared with node density, then communications are not necessary to be confined in nearest neighbors
SLIDE 11
A wireless CDMA ad hoc network may overcome the scaling law
SLIDE 12
Our Model
Large Wireless CDMA Ad Hoc Networks
SLIDE 13
CDMA
Nodes access each other through a common
CDMA channel
Spreading sequences are random, i.i.d. (long
sequences)
Spreading gain N = WTb All nodes have same transmission power P0 No power control is employed
SLIDE 14 Power Decay Model
Power decays in distance r
P0 is transmission power, r0 > 0, β > 2
β
) 1 / ( ) ( + = r r P r P
SLIDE 15
Network Topology
Nodes are distributed on entire 2-D plane Node locations can be regular or arbitrary
SLIDE 16
Node Distributions
Nodes are uniformly distributed At any time t, a percentage ρ of nodes are
sending
Sending nodes are also uniformly distributed For each N, node density is dN, or
dN/N (nodes/Hz/second/m2)
Traffic intensity
ρdN/N (sending nodes/Hz/second/m2)
SLIDE 17 W f
Limiting Network
dN → ∞, N → ∞, dN/N → α
SLIDE 18 W f
Limiting Network
dN → ∞, N → ∞, dN/N → α
SLIDE 19 W f
Limiting Network
dN → ∞, N → ∞, dN/N → α
SLIDE 20 W f
Limiting Network
dN → ∞, N → ∞, dN/N → α
SLIDE 21 W f
Limiting Network
dN → ∞, N → ∞, dN/N → α
SLIDE 22 Objective
For the limiting network as dN → ∞, N → ∞,
dN/N → α, we derive
Transport capacity (bit-meters/symbol
period/node)
Spectral efficiency (bit-meters/Hz/second/m2)
SLIDE 23 Received Signal in a node
Chip matched filter output in a receiving node
r is link distance b, P(r), and s are for desired sending node bx, P(||x||), and sx are for interference nodes n ~ N(0,σ2I)
n s x s y
x x x
+ + =
∑
∈ ) (
||) (|| ) (
t BN
P b r P b
r
SLIDE 24 MF Output
MF outputs an estimate of b Unit-power SIR
y sT y = ) ( 1
2
I E
N ≡
η I b r P + = ) ( n s s s x
x x x T T t BN
P b b r P + + =
∑
∈ ) (
||) (|| ) (
SLIDE 25 Asymptotics
Theorem: Interference I is asymptotically independent
Gaussian, and unit-power SIR ηN converges a.s. to
where total interference power to a node is finite
(watts/Hz/second)
Include all interference of the network Limit network is capable of information transportation
) ( 1
2
∞ + = P σ η ) 1 )( 2 ( 2 ) (
2
− − = ∞ β β αρ π P r P
SLIDE 26 Limit Link Channel
From sending b to MF output, there is a link
channel, which is memoryless Gaussian
z ~ N(0,1), i.i.d.
SIR = ηP(r) depends only on link distance Same result can be obtained if a decorrelator
- r MMES receiver is employed
z b r P y + = ) ( η
r b y
SLIDE 27 Link Channel Capacity
For a link of distance r, the link capacity is
(bits/symbol period)
)) ( 1 ( log 2 1 ) (
2
r P r C η + =
SLIDE 28 Packet delivery
A packet is delivered from source node to
destination node via a multihop route ϕ(x) = {xi, i = 1, …, h(x), x1 + x2 + … + xh(x) = x}
A packet is coded
with achievable rate
The code rate of a packet
to be delivered via route ϕ(x) must be not greater than the minimum link capacity on the route
x1 S D x2 x3 x4 x
SLIDE 29 Route Transport Capacity
Via route ϕ(x), bits per symbol
period are transported by a distance of ||x|| meters
h(x) nodes participate in transportation Route transport capacity is
(bit-meters/symbol period/node)
) ( ||) (|| min || ||
) ( 1 ) (
x x x
x x
h C
i h i≤ ≤
= Γ
ϕ
x1 S D x2 x3 x4 x
||) (|| min
) ( 1 i h i
C x
x ≤ ≤
SLIDE 30
Routing Protocol
A global routing protocol schedules routes of
all packets
Consider achievable routing protocols that
schedule routes without traffic conflict
Let distribution of S-D vector x be F(x) For the same S-D vector x, different routes
ϕ(x) may be scheduled
Under routing protocol u, let route ϕ(x) for S-
D vector x have distribution Vu[ϕ(x)]
SLIDE 31 Transport Throughput
Transport throughput achieved under routing
protocol u
(bit-meters/symbol period/node)
F(x) – distribution of S-D vector x Vu[ϕ(x)] – route distribution
( )
) (
) (
r ϕ
ρΓ = Γ
u
E u
∫ ∫
ℜ Ω ∈ ≤ ≤
=
2
) ( )) ( ( ) ( ) ( min || ||
) ( ) ( ) ( 1
x x x x x
x x x
dF dV h C
u
u h i ϕ
ϕ ρ
SLIDE 32 Transport Capacity
Each achievable routing protocol attains a
transport throughput
Transport capacity is defined as
- – collection of all achievable routing
protocols
) ( sup u
u
Γ = Γ
Ψ ∈
Ψ
SLIDE 33
Spectral Efficiency
Given transport capacity Γ, spectral efficiency
is
(bit-meters/Hz/second/m2)
Γ = Π α
SLIDE 34 Main Result
Theorem: Transport capacity equals
r – S-D distance; F(r) – distribution of r
Spectral efficiency equals
∫
∞ ≥
= Γ
1 ) ( *
) ( ) ( )) ( / ( max r dF r h r h r C r
r h
ρ
∫
∞ ≥
= Π
1 ) ( *
) ( ) ( )) ( / ( max r dF r h r h r C r
r h
αρ
SLIDE 35 Outline of Proof
Step 1: Show that Γ* is an upper bound Step 2: Show that Γ* is the lowest upper
bound
Need to find an achievable routing protocol to
attain Γ* − ε for any ε > 0
SLIDE 36 Scaling Law
If α → ∞ (or N fixed but dN → ∞), then
Transport capacity goes to zero at rate 1/α -
“scaling law” behavior
Spectral efficiency converges to a constant
This scaling law is due to that radio
bandwidth does not increases as fast as node density increases
– different from that of Gupta-Kumar model
) / 1 ( α O = Γ ) 1 ( O = Π
SLIDE 37
Scaling Law
The “scaling law” can be overcome, provided
spreading gain N (or bandwidth) increases at the same rate as node density dN increases
A large wireless CDMA ad hoc network is
capable of information transportation!
constant > = Γ constant > = Π
SLIDE 38 Transport capacity monotonically decreases with α
10
10
10
10
10 0.5 1 1.5 2 2.5 3 3.5 4 5x100 Transport capacity vs. alpha α (nodes/Hz/second/m2) - node density / processing gain Γ (bit-meters/symbol period/node) GIGC BIGC BSC MMSE Dec MF
Transport Capacity vs. Traffic Intensity
SLIDE 39 Π monotonically increases with α
Spectral Efficiency vs. Traffic Intensity
10
10
10
10
10 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 x 10
5x100 α (nodes/Hz/second/m2) Π (bit-meters/Hz/second/m2/watt) GIGC BIGC BSC MMSE Dec MF
SLIDE 40 Transport capacity monotonically increases with P0
10 20 30 40 0.05 0.1 0.15 0.2 0.25 P0 (dB) Γ (bit-meters/Hz/second/m2/watt) GIGC BIGC BSC MMSE Dec MF
Transport Capacity vs. Transmission Power
SLIDE 41 Π monotonically decreases with P0
Spectral Power Efficiency vs. Transmission Power
10 20 30 40 0.5 1 1.5 2 2.5 3 3.5 x 10
P0 (dB) Π (bit-meters/Hz/second/m2/watt) GIGC BIGC BSC MMSE Dec MF
SLIDE 42 Sensor Networks:
Sensor Density vs. Transmission Power
Sensor network is low powered, P0 → 0 Question: with given total power per square meter
αρP0 = ω,
should we increase node density and decrease node
transmission power?
Answer:
we should increase node density and decrease node
transmission power in terms of increase of spectral power efficiency
∫
∞ ∈ = →
+ = Π
+
) ( ,
) ( ] 1 )) ( ( )[ ( min lim r dR r h r r r h r c
Z r h P P β ω ω αρ
αρη
SLIDE 43 Conclusions
If radio bandwidth increases slower than
node density increases, transport capacity decreases to zero – “scaling law”
The scaling law is essentially different from
that of Gupta-Kumar model
The scaling law can be overcome, provided
radio bandwidth increases as fast as node density increases
A large wireless CDMA ad hoc network is
capable of information transportation