<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD v1.0 20120330//EN" "JATS-archivearticle1.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>The Mathematical Model for Interference Simulation and Optimization in 802.11n Networks</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Iwona Dolin´ska</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Antoni Masiukiewicz</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Grzegorz Rza¸dkowski</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Vistula University</institution>
          ,
          <addr-line>Warsaw</addr-line>
          ,
          <country country="PL">Poland</country>
        </aff>
      </contrib-group>
      <fpage>99</fpage>
      <lpage>110</lpage>
      <abstract>
        <p>One of the key problems in 802.11 standard networks are interferences. It is not possible to avoid the influence of other wireless systems. One can only minimize the power level of unwanted signals. Typically the designer should find the best localization of access points (AP), but there is no planning and coordination between different private networks. To reduce the level of interferences, the transmitting power reduction is applied. The mathematical model was built to analyze the relationship between the coverage and the level of interferences. The results of these simulations are presented in this article.</p>
      </abstract>
      <kwd-group>
        <kwd>Wi-Fi</kwd>
        <kwd>interferences</kwd>
        <kwd>802</kwd>
        <kwd>11n standard</kwd>
        <kwd>WLAN</kwd>
        <kwd>throughput</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>Introduction</title>
      <p>
        The 802.11 standard networks are the most popular solution of wireless
communication today, besides the mobile telephony networks. One of the key problems
in such networks is the issue of interferences (see [
        <xref ref-type="bibr" rid="ref6">6</xref>
        ]). The main sources of
interferences are various radio systems or devices, which operate on the same or
similar frequency range. These networks produce both, adjacent and inter
channel interferences. The reduction of internal system interferences is crucial for
obtaining the proper QoS of the transmissions (see [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]). Basic methods of the
interference limitation implement proper planning, which means the proper
arrangement of the access point localizations. The next step is a selection of the
transmission frequency dedicated for each channel. Such planning is not possible
in any network. One of the important features of the 802.11 networks is the fact,
that they operate at the public free frequency range (ISM Industrial, Scientific,
Medical), so the high number of different devices can operate at the same time
on a similar area. These devices could be elements of home or office networks.
There is no coordination between such networks.
      </p>
      <p>
        Another method of interference reduction is the diminish of the transmitted
power (see [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ]). In the authors opinion this method is not very efficient especially,
if the coverage is an important issue. The authors built the theoretical model
and carried out several calculations to show both advantages and disadvantages
of such solution.
      </p>
    </sec>
    <sec id="sec-2">
      <title>The Structure of 802.11n Physical Layer</title>
      <p>
        The structure of the Physical Layer has a great influence on the internal system
interference level. For 2.4 GHz transmission frequency range, only three channels
(numbered 1, 6 and 11) are the so called not overlapping channels (see [
        <xref ref-type="bibr" rid="ref9">9</xref>
        ]). The
standard deviation between the central frequencies of these three channels is
25 MHz. The level of signal within a channel is limited by the mask. The mask
is a filter with specially developed characteristic. The characteristics of filters for
1, 6 and 11 channels in the 802.11n standard are presented in Fig. 1.
      </p>
      <p>
        The channel masks overlap partly, even for non overlapping channels. Some
interchannel interferences are always present in the system, when more than one
network is operating on the same area. The final level of the interference signal
power depends strongly on many parameters. The distance plays an important
role, because the level of the received power decreases while increasing the
distance between Wi-Fi stations. Two disadvantages are produced by interferences
(see [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ]). The first is the diminish of signal to noise ratio, because the interference
power is treated as noise within the transmission channel. The thermal noise and
the interference power are produced by uncorrelated sources, so we can calculate
the summarized noise as the sum of power density of the thermal noise and the
interference power (see [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ]):
      </p>
      <p>
        Pnoise = Pint + Pwhite noise :
The noise power diminishes the channel throughput. The throughput is the most
important parameter determining the QoS of the transmission. The channel
throughput could be described by the following formula (see [
        <xref ref-type="bibr" rid="ref3">3</xref>
        ]):
C = B ln (1 + Psignal ) ;
      </p>
      <sec id="sec-2-1">
        <title>Pnoise</title>
        <p>(1)
where B represents the bandwidth of the transmission channel. The second
disadvantage of interferences especially, when their signal power is relatively high,
is the effect of the spurious carrier detection. The high level of interference power
blocks the transmission channel. Some methods of interference level reduction
are discussed in the next section.
3</p>
      </sec>
    </sec>
    <sec id="sec-3">
      <title>The Methods of Interference Level Reduction</title>
      <p>
        A high level of interference power could be reduced by a proper arrangement of
access points (see [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ]). It is possible only in some networks eg. private networks,
company networks. On the other hand, in some networks, the access points are
arranged in a totally chaotic way. There is no coordination of AP localization
and no coordination of utilized channels. An example of a set of private networks
is shown in Fig. 2. Such a situation happens very frequently, especially in the
multi-family or office buildings.
      </p>
      <p>
        Many devices use the same channel (5 devices - channel nr 11), some devices
use channels other then 1, 6, 11, so the choice of a channel is random. Network
planning let us achieve capacity, range and QoS (see [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ], [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ], [
        <xref ref-type="bibr" rid="ref5">5</xref>
        ]). There are several
methods of WiFi network planning described in the literaturte, e.g.
NeldeareMead direct planning (see [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ]). This method enables the optimal determination
of localization of AP stations. The coefficient of channel frequency reuse could be
calculated (co channel interference reduction factor). This factor is the function
of the number of available channels/frequencies especially those not overlapping
and could be expressed by following formula:
      </p>
      <p>Q = p3N;
(3)
where the N is the number of available channels.</p>
      <p>
        The second solution suggests [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ] reduction of transmitted power, but as a
side effect a decrease of coverage occurs. This solution reduces the interference
power level, but on the other hand leads to dead areas with no coverage, what
is shown in Fig. 3.
(4)
(5)
(6)
(7)
      </p>
      <p>The smaller is the coverage of one cell, the more cells we have to produce
to obtain the full coverage. This means more APs and in the end, more
transmissions at the same time, but it does not mean that we reduce the interference
power level. The authors present some proof in Sec. 5 and Sec. 6.
4</p>
    </sec>
    <sec id="sec-4">
      <title>Correlation Between Coverage, Transmitted Power and the Interference Power Level</title>
      <p>
        The basic equation, which describes the radio wave distribution in a free space
is the Friis formula (see[
        <xref ref-type="bibr" rid="ref3">3</xref>
        ]):
      </p>
      <p>Prx (r) =</p>
      <sec id="sec-4-1">
        <title>PtxGrxGtx 2</title>
        <p>(4 r)2
=</p>
      </sec>
      <sec id="sec-4-2">
        <title>PtxGrxGtxc2</title>
        <p>(4 r)2 f 2
:
This formula allows us to calculate the received power (Prx) depending on the
transmitted power (Ptx), the gains of receiving and transmitting antennas (Gtx,
Grx), the channel frequency f and the distance between the transmitter and
receiver (in so called free space, the r power is equal 2):
k
Prx(r) = f 2r2
:
Using the formula (4) we can calculate the attenuation of radio signal in a free
space:</p>
        <p>Podb (r) = PtxGrxGtxLfspl;
Lfspl =</p>
        <p>
          c2
(4 r)2 f 2
and finally we obtain the following formula [
          <xref ref-type="bibr" rid="ref6">6</xref>
          ]:
        </p>
        <p>
          Lfspl[dB] = 32; 44 + 20 log r[km] + 20 log f [M Hz];
(9)
where r is in [km] and f in [MHz]. The more general formula takes the following
form (see [
          <xref ref-type="bibr" rid="ref6">6</xref>
          ]):
This formula for frequencies f in [Hz] or [MHz] can be rewritten respectively as:
The coefficient is rather unstable in time and very sensitive to the environment
e.g. it changes strongly in rooms.
        </p>
        <p>The coverage in the 802.11n standard is determined by the minimal received
power (received signal sensitivity), which is necessary for obtaining required level
of throughput. The set of minimal received power in the case of a single spatial
transmission in 802.11n standard is presented in Table 1.</p>
        <p>The minimal sensitivity is respectively -82 dBm for throughput of 6.5 Mbit/s
and -64 dBm for 65 Mbit/s. It is difficult to correlate these values with a specific
distance, because in practice this distance could vary in a broad range due to a
lot of factors.
5</p>
      </sec>
    </sec>
    <sec id="sec-5">
      <title>The Analysis Assumptions</title>
      <p>
        The authors tried to verify the assumption that the decreasing of transmission
power and reduction of coverage help to diminish the internal interferences in
802.11n networks (see [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ]). The analysis was reduced to a model with one spatial
stream in 802.11n standard. One spatial stream means the use of the SISO
(Single Input Single Output) antenna solution. The isotropic characteristic of
transmission power is also the assumption. The analysis was carried out for
three non overlapping channels 1, 6 and 11. The Tx and Rx configurations are
presented in Fig. 4.
      </p>
      <p>The Table 2 includes the channel allocation, which is used in simulation.</p>
      <p>We assume that all stations are the transmitters. The localization of a station
within the cell (coverage area) could vary from the center of the area to its edge.
We analyze the 802.11n standard with 20 MHz channel bandwidth. The center
frequencies for channels 1, 6, 11 are shown in Table 3.</p>
      <p>The interference power level was calculated as the sum of interferences from
stations S1 and S2 and white noise and the noise figure representing the noise
of electronic circuits (mainly electronic amplifiers).</p>
      <p>Pint =</p>
      <p>
        2
∑ Pintx + (Pwhite noise + PNF ) :
x=1
White noise or thermal noise [
        <xref ref-type="bibr" rid="ref3">3</xref>
        ] within the channel bandwidth could be described
as:
      </p>
      <p>Pwhite noise(f ) = kT [W=Hz] ;
T denotes the environment temperature in K degree, while k is a Boltzman
constant. Threshold of white noise in 1 Hz bandwidth at 0 Kelvin degree is
-228.6 dBW. White noise in B bandwidth can be calculated as:</p>
      <p>Pwhite noise[dBm] = 10 log(kT B) :
The white noise in 20 MHz channel at 17 C degree could reach the following
level:
Pwhite noise(T = 17◦C; B = 20M Hz) = 174 + 10logB = 131dBm .
The following formula was developed by the authors to calculate the received
power:</p>
      <p>Preceived(r) = M (f
2412
5(K</p>
      <sec id="sec-5-1">
        <title>1)) + Ptransmitted</title>
        <p>( 27; 56 + 10 log r[m] + 20 log f [M Hz]) + Gsum:
(16)
We will denote Preceived and Ptransmitted by Prx and Ptx respectively. The M (f )
function represents the mask (filter) of the relevant channel. The signal outside
the mask is eliminated while the one below the mask characteristics passes. The
authors assume that the mask characteristic determines the maximal internal
level of interferences. Gsum is equivalent to the additional gain of the system
including the influence of the antennas of the receiver and the transmitter and
respectively the gain connected with modulation, coding and different types of
signal dispersions. Ptx, and Gsum are the parameters of the simulation and
their values are presented in Table 4.</p>
        <p>The parameters of m(f ) function correspond to the mask of 802.11n standard.
We assume that the function (for f in MHz) is continuous, piecewise linear and</p>
        <p>The stations are placed on Cartesian plane. The S transmitter has the (x; y)
coordinates and S1 respectively (x1; y1). The distance d1 between the above
stations is equal:
d1 = √(x
x1)2 + (y
y1)2 :
The practical formula for interference power level, which influences the S
station (operating on channel 6) in d1 distance from the station S1, producing
interferences while operating on channel 11, will be as follows:
Prx(d1) = M (f 2462) + Ptx ( 27:56 + 10 log d1[m] + 20 log 2462) + Gsum:
(19)
The average interference power within the whole channel is the integral from
Prx over f within the proper channel (6th in our case):</p>
        <p>Prx(d1)average =
∫ 2:447
2:427</p>
        <p>Prxdf :
The authors correlate the distance d1 with the minimal received signal sensitivity
(see Table 3).
6</p>
      </sec>
    </sec>
    <sec id="sec-6">
      <title>The Simulation Results</title>
      <p>In the first simulation the station S, operating on channel 6, was disturbed by
S1 station, operating on channel 11. The transmitting power distribution was
firstly simulated. The figure 5 shows the distribution of points correlated with
(17)
(18)
(20)
and Gsum. Source: own
preparespectively -64 dBm and -82 dBm of received power (upper and lower lines).
This analysis concerns the transmission in channel 6. We assume that the power
transmitted by the S station is equal to receiver sensitivity.</p>
      <p>The points corresponding to the -64dBm received signal are within the range
from single meters to about 25 meters, while these corresponding with -82 dBm
are within the range from a few meters to more than 200 meters. The coverage
diminishes especially for the higher value of . Figure 6 presents the
characteristics of the diminish of transmitted power with distance for different values of
Prx, and Gsum. The critical parameter is the . The highest slope is for = 8.</p>
      <p>The characteristics of the interference power for the fixed distance beetwen
S and S1 are presented in Fig. 7. The Pint characteristics are versus the level
of the disturbances source power. The following assumptions are made: the S is
transmiiting in the channel nr 6, Ptx is 10 dBm, Gsum is 0 [dBm] and = 3;
while the S1 station (disturbing) is transmitting in the channel nr 11, Gsum is 0
[dBm], is 3 and the Ptx change in the range from -10 to 20 dBm. The point of
the interference level calculation coresponds with the maximum coverage of the
S station, where the Prx is -82dBm. This distance is 53,38 m while the distance
between stations is 106.76m. The results are shown in Fig. 7.</p>
      <p>The interference power level diminishes, when the Ptx of S1 diminish, but
at the same time the coverage area is reduced, so the dead zone arises with no
possibility of transmission. The white noise could have higher level than
interference power for low Ptx of disturbing station and for non convenient transmission
conditions (high value of the coefficient- eg. rooms, halls etc.).</p>
      <p>The characteristics of interference level with another assumption is presented
in fig. 8. In this case together with the change of the Ptx we change the point of
S1 localization (x1,y1) to reduce the dead zone. The point of the interference level
calculation (distance from S) is constant and its value is 53.38 m, but the distance
between S and S1 stations (d1) diminishes relatively to Ptx (S1) reduction. The
dead zone is minimized. The level of interference power is constant versus Ptx
and values (Fig. 8). The next simulation concern the situation when the Ptx
power is increased for both S and S1 and the interference power level is calculated
for maximum coverage points corresponds with received power equal -82 dBm
(Fig. 9). The results of the simulation are the same as previously. The inteference
power level is higher than the thermal noise, but if we take into account the the
electronic circuits noise figure, then the total noise could be above interference
power level.
The model for interference power level simulations from one or two disturbing
sources (S1 /S2) was developed. The model includes the efects of the mask
and several other parameters such as antennas gain, modulation coding and
dispersion gain (Gsum coefficient). The following simulations based on this model
were carried out :
1. the characteristic of interference power level, when the Ptx of source of
disturbances is reduced, but the localisation remains the same (see Fig. 7) ,</p>
      <p>Taking into account the mentioned above simulations, we can conclude:
1. for the 1st simulation: the power level of interferences decrease, but the
coverage diminishes at the same time,
2. for the 2nd simulation: the interference level is constatnt,
3. for the 3rd simulation: the interference level is constatnt.</p>
      <p>The achieved results let us make a conclusion, that reduction of Ptx could
reduce the interference power level, but at the same time cause the dead zone
to arise. This solution may be applied, if the station is close to AP, so we can
temporary (for one or more sessions) reduce transmission power, keeping
reasonable throughput. This solution requires communication between different APs
to establish the most efficient transmission power level. Such solutions are not
available nowadays.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          1.
          <string-name>
            <surname>Dolin</surname>
          </string-name>
          <article-title>´ska I., Masiukiewicz A.: Quality of service providing in WLAN networks, possibilities, challenges and perspectives</article-title>
          . In: Information Systems in Management,
          <string-name>
            <surname>Wydawnictwo</surname>
            <given-names>SGGW</given-names>
          </string-name>
          , Warsaw (
          <year>2012</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          2.
          <string-name>
            <surname>Fuxjager</surname>
            <given-names>P.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Valerio</surname>
            <given-names>D.</given-names>
          </string-name>
          , Ricciato F.:
          <source>The Myth of Non-Overlapping Channels: Interference Measurements in IEEE 802.11</source>
          .
          <string-name>
            <surname>IEEE</surname>
          </string-name>
          (
          <year>2007</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          3.
          <string-name>
            <surname>Freeman</surname>
            <given-names>R.L.</given-names>
          </string-name>
          :
          <article-title>Radio system design for telecommunication</article-title>
          ,
          <source>Wiley</source>
          (
          <year>2007</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          4.
          <string-name>
            <surname>Gajewski</surname>
            <given-names>P.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Wszelak</surname>
            <given-names>S.:</given-names>
          </string-name>
          <article-title>Optymalizacja wyboru punktow dostepowych w sieciach WLAN metoda bezposredniego poszukiwania</article-title>
          .
          <source>Przeglad Telekomunikacyjny nr 8-9</source>
          , Warsaw (
          <year>2007</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          5.
          <string-name>
            <surname>Hereman</surname>
            <given-names>F.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Joseph</surname>
            <given-names>W.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Tanghe</surname>
            <given-names>E.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Plets</surname>
            <given-names>D.</given-names>
          </string-name>
          and Martens L.:
          <article-title>Prediction of Range, Power Consumption and Throughput for IEEE 802.11n in Large Conference Rooms</article-title>
          .
          <source>In: Proceedings of the 5th European Conference on Antennas and Propagation (EUCAP)</source>
          (
          <year>2011</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          6.
          <string-name>
            <surname>Hotgkinson</surname>
            <given-names>T.G.</given-names>
          </string-name>
          :
          <article-title>Wireless communication-the fundamentals</article-title>
          .
          <source>In: BT Technology Journal</source>
          , Vol
          <volume>25</volume>
          No 2 (
          <year>2007</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref7">
        <mixed-citation>
          7.
          <string-name>
            <given-names>Juniper</given-names>
            <surname>Networks White Paper</surname>
          </string-name>
          ,
          <article-title>Coverage or Capacity-Making the Best Use of 802</article-title>
          .
          <year>11n</year>
          . (
          <year>2011</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref8">
        <mixed-citation>
          8.
          <string-name>
            <surname>Masiukiewicz</surname>
            <given-names>A.</given-names>
          </string-name>
          ,
          <article-title>Analysis and optimization of quartz crystal oscillators for minimal phase noise</article-title>
          .
          <source>PhD Thesis</source>
          , Warsaw University of Technology (
          <year>1997</year>
          )
        </mixed-citation>
      </ref>
      <ref id="ref9">
        <mixed-citation>
          9.
          <string-name>
            <surname>Roshan</surname>
            <given-names>P.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Leary</surname>
            <given-names>J</given-names>
          </string-name>
          .:
          <source>Bezprzewodowe sieci LAN 802</source>
          .
          <fpage>11</fpage>
          -
          <lpage>Podstawy</lpage>
          . PWN, Warsaw (
          <year>2007</year>
          )
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>