Image Processing Reference
In-Depth Information
maximum width of the resulting overlapping region A is  l . According to the figure, the transmission
range r is equal to l
+(
d
/
)
.
d
=
(
r
l
)
(.)
In an ideal environment, both sensor nodes S and S transmit a message. This message can be
received within the radius r around the nodes. In the overlapping region A (dashed region), all n A
enclosed sensor nodes receive both messages. These sensor nodes S i (
n A )areneighborsof
both sending nodes. Due to the uniform distribution of nodes, the number of nodes n in range of
onesensornode( A TR
=
i
=
r ) is constant. Since the node density µ is constant in the whole network,
the following equation is formed:
=
π
n A
A =
n
n
A TR
µ
=
r =
(.)
π
and results in
n A
n
π r
A
=
(.)
The calculation of width l can be approximated by
r
π r
 r
sin
arcsin
(
(
A
)/
)
l
=
r
+
(.)
After calculation of l ,thedistance d can be determined by Equation .. ..The achieved accuracy
of NIDES oscillates between . r and . r .
6.2.9 Received Signal Strength
In vacuum, a radio signal of a circular source propagates circularly. Generally, the transmission of
radio signals is adherent with the transport of energy into the surrounding of the sender. This en-
ergy level is flatten with the distance d to the sender, but it can be detected by a receiver. In several
publications, this method to detect the energy level is called received signal strength (RSS).
Friis presented an equation to compute the distance based on transmission power P TX ,received
power P RX ,antennagains( G TX , G RX ), system losses L ,andthewavelengthλ provided ideal
conditions (no reflection, no diffraction, no obstacles, etc.) are met [Fri].
P RX
P TX =
G RX G TX
L
λ
π d )
(
(.)
If a sensor node S is able to detect the received power P RX of a message, the distance between the
transmitting node S and S canbecalculatedbyrearrangingEquation..
According to Equation ., wave length λ and distance d affect P RX quadratically [Rap]. he
attenuation of a signal is defined as path loss (PL) which is the logarithm of transmitting power to
received power in decibel.
 log P TX
G RX G TX
L
λ
π d )
PL
(
dB
)=
P RX =−
 log
(
(
)
(.)
To detect a signal of a transmitting node at a receiving node correctly, the receiver sensitivity PL max
must be higher than the PL depending on the specific distance d between both nodes. For instance,
 
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