Transmission of high power sensor system and DWDM data system in one optical fiber
Abstract
The main contribution of this paper is simulation of transmission DWDM system and high power sensor system in one optical fiber
Full text
T ansmission o High Powe Senso Sys em and
DWDM Da a Sys em in One Op ical Fibe
Milan Cucka, Pe Muns e , Lukas Koci, Tomas Ho a h, Milosla Filka, and Jose Voj ech
Abs ac —This a icle deals wi h he possibili y o employing
phase sensi i e OTDR (Op ical Time Domain Re lec ome y) in o
ibe s wi h ac i e da a ansmission DWDM (Dense Wa eleng h
Di ision Mul iplex). Due o he low backsca e ed signal o phase
sensi i e OTDR is equi ed o gene a e pulses wi h a high in en-
si y and sho ime du a ion. These high powe pulses can cause
deg ada ion o he da a ansmission. By using VPIpho onics
so wa e we pe o med he simula ions in es iga ing he in luence
o phase sensi i e OTDR o quali y DWDM connec ions and we
a e also in e es ed in he wa eleng h spacing be ween senso ic
sys em and da a sys em. In ou a icle i was e i ied ha phase
sensi i e OTDR and da a ansmission can be ac i e oge he in
one op ical ibe . I bo h sys ems wo k e y close o each o he i
will lead o deg ada ion o da a ansmission. We ha e e i ied
ha da a ansmission may be a ec ed i powe o pulses exceed
13 dBm.
Index Te ms—DWDM, Phi-OTDR, Pulse gene a ion, Backsca -
e ed signal, Simula ions, VPIpho onics.
I. INTRODUCTION
Nowadays op ical senso s a e used hanks o hei abili ies
o sense high empe a u es, ib a ions and mechanical ension.
One big ad an age is accu acy o measu emen and compac
po able ins umen packages. Fo example, ib a ion senso s
a e pu on al eady exis ing ou es and a e used o ack any
mo emen a ound he ou e. Ano he commonly used ype o
op ical senso s a e senso s o empe a u e sensing due o hei
abili y o measu e high empe a u es. These ypes o senso s
can o e noncon ac measu emen .
Op ical senso s can be di ided in o wo g oups. The i s
g oup includes ex insic senso s wi h sensing ou side he ibe
and he second g oup is in insic ha means ha sensing akes
place wi hin he ibe i sel . This a icle ocuces on he in lu-
ence o φ–OTDR (Op ical Time Domain Re lec ome y) senso
and hei lase o he BER (Bi E o Ra e) o he DWDM
(Dense Wa eleng h Di ision Mul iplex) sys em. Using same
op ical ibe s o pa allel ansmission o a da a and a sensing
signals simul aneously is new and inno a i e idea.
The es o his pape is s uc u ed as ollows. Sec ion I
sho ly in oduce ibe op ics senso s and new ends. Sec ion II
Manusc ip ecei ed No embe 30, 2015; e ised No embe 7, 2016 and
No embe 22, 2016.
Resea ch desc ibed in his pape was inanced by he Na ional Sus ainabil-
i y P og am unde g an LO1401, and SIX CZ.1.05/2.1.00/03.0072. Fo he
esea ch, in as uc u e o he SIX Cen e was used.
Au ho s a e wi h he Depa men o Telecommunica ions, B no Uni-
e si y o Technology, B no, Czech Republic and om CESNET,
z.s.p.o., P aha, Czech Republic (E-mails: [email p o ec ed].cz,
[email p o ec ed].cz, [email p o ec ed].cz, ho [email p o ec ed].cz,
[email p o ec ed].cz, [email p o ec ed]).
desc ibes ela ed wo k in φ–OTDR senso s. Sec ion III gi es
an o e iew abou DWDM sys em and in oduces unc ion
o φ–OTDR senso . Sec ion IV and sec ion V desc ibes ou
simula ion se up in VPIpho onics and discusses he esul s
achie ed in he simula ion. Sec ion VI concludes he pape and
desc ibes u u e wo k.
II. RELATED WORKS
Op ical senso s based on φ-OTDR we e i s in oduced in
2003 by Juan Ca los Jua ez. He published his esea ch wo k
abou op ical senso s in [8]. Fu he , φ-OTDR senso s a e
widely used as senso s o mechanical ib a ions o moni o ing
and secu ing na ional bo de s, oil and gaspipelines, mili a y
ins alla ions, s uc u al heal h e c.
Many sys ems use an ex emely na ow lase and EDFAs
(E bium Doped Fib e Ampli ie ). This sys em wo ks on a 4
km long op ical ibe wi h esolu ion o 50 m. A e de ec ion
da a a e p ocessed in Ma lab en i onmen . I is neccessa y
o il e he ecei ed signal. [9] desc ibes he issues bu does
no desc ibe using one op ical ibe o he de ec ion and
o da a ansmission. Nex issue o φ–OTDR is p ocessing
o ecei ed signal due o di icul il e ing and analyzing.
Fea u e ex ac ion o ime domain signals in hese sys ems
is ime-consuming and may lead o inaccu acies due o noise
dis u bances. The ecogni ion and speed o φ–OTDR sys ems
canno be used o online ib a ion moni o ing sys ems.
The wo k which is called Recogni ion o a Phase-Sensi i i y
OTDR Sensing Sys em Based on Mo phologic Fea u e Ex-
ac ion be e desc ibes his p oblem bu does no deal wi h
any simula ion o use φ–OTDR sys ems on elecommunica ion
ou es [10]. Ou a icle ocuses on simula ions in VPIpho onics
so wa e.
The au ho s in [11] desc ibe ampli ica ion o he φ–OTDR
sys ems, epe i ion a e and wid h o he pulses. They use
a simple me hod using he holding beam o ampli ying o
pulses wi h low epe i ion a e by s anda d elecommunica ion
EDFA boos e . The e a e desc ibed h ee me hods o φ–
OTDR signals ampli ica ion and hei e i ica ion by measu e-
men .
These a icles [12], [13], [14], [15], and [16] deal wi h
he same opics, pulse wid h, du a ion, epe i ion equency
and il e ing o he ecei ed signal. In compa ison wi h o he
a icles, ou pape looks a simula ion o φ–OTDR wi h
DWDM sys em on one op ical ibe .
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O iginal scien i ic pape
III. OVERVIEW OF THE SYSTEM
A. Dense wa eleng h di ision mul iplex sys em
T ansmission sys ems based on DWDM a e now o en used
o inc ease he ansmission capaci y o op ical ibe o bi-
di ec ional communica ion. I is a combina ion o se e al
wa eleng hs which ansmi mul iple lase s.
A ansmi e which ansmi s in o ma ion is modula ed
on each ca ie equency. A mul iplexo combines each
op ical channel wi h he op ical ibe . Fo n-channels con-
nec ion one mul iplexo /demul iplexo and also one modula-
o /demodula o a e needed. Each channel needs ligh sou ce
on speci ic wa eleng h.
DWDM echnology uses DFB (Dis ibu ed Feedback) lase
wi h ex emely na ow spec al line and highly selec i e spec-
al il e s. These de ices a e e y sensi i e o equency and
he mal s abili y. This is one eason why he echnology is
expensi e. The s anda d ITU-T G.694.1 speci ies he indi id-
ual ansmission channels a he wa eleng h in he ange om
1490 nm (200.95 THz) o 1620 nm (186.00 THz) called S, C,
and L band.
DWDM g id is based on a no malized pilo equency
193.1 Thz. The minimum spacing o each wa eleng h may
be 0.1 nm, which uses ul a na ow DWDM. To main ain he
s anda d i is necessa y o ha e a spacing o 0.2 nm. To ensu e
p ope unc ioning wa eleng h di ision mul iplexing i is bes
o choose a spacing o 0.8 nm.
B. Φ–OTDR op ical senso
Commonly used op ical ibe ib a ion sensing sys ems use
phase sensi i e op ical ime domain e lec ome e . Φ–OTDR
sys ems can de ec and loca e ib a ion signals by measu ing
he backsca e ligh ac oss op ical spec um. Senso ic sys-
em commonly wo ks wi h Rayleigh and B illouin sca e ing.
Phase sensi i e OTDR uses basic single mode op ical ibe
which is also used o ansmission. This ype o senso has
been used o moni o ing and sa e y condi ion o building
s uc u es, gas o oil pipeline s uc u es. Measu ing can be
eal- ime.
Sou ce o op ical adia ion sends beam o he ibe , i is sho
ime and high powe ed pulse which can p opaga e in op ical
ibe . Then he pa o ligh is con inuously backsca e ed
because o Rayleigh o B illouin sca e ing. This beam is
measu ed by p ocessing he backsca e ed signal. Cap u ing
and p ocessing o he signal is he mos used echnique. This
signal is sensed by he op ical ime domain e lec ome y.
Re lec ome ic sensing is e y use ul o de ec ion ib a ions
and hei localiza ion. Many dis ibu ed senso s use φ–OTDR.
Senso ic sys ems based on φ–OTDR can be used o moni o
mo e han one ib a ion sou ce along he op ical ibe .
This ype o sensing needs special pulses, because he
backsca e ed signal is e y low. The backsca e powe may
be desc ibed as [11]:
PR( ) = Pi·SγR ·W0·υg·exp−γ· g
·
2=PR(0) ·expγ· g
· ,
(1)
whe e γis he a enua ion coe icien and is equal o 1/20 h
o he g adien o a plo o Rayleigh backsca e a enua ion
in dB, Piis he inpu powe , γR is he Rayleigh sca e ing
coe icien .
The ac ion o cap u ed op ical powe is de ined o s ep
index ibe s as [11]:
S=NA2
4n2,(2)
whe e NA is nume ical ape u e and n is he ibe e ac i e
index.
A e his we can simpli ied he i s equa ion as [11]:
PR( )=7.8·Ep·exp−γ· g
· = 7.8·Ep·exp−2γ· g
· ,(3)
whe e we use γ= 4.6·10−5, NA = 0.12, n = 1.46.
¿F om hese equa ions we can see ha backsca e ed powe
is lowe han inpu powe . Fo a e age powe o 150 mW
and pulse du a ion o 200 ns. The le el o he backsca e ed
signal is abou 52 dB lowe compa ed o he inpu . S anda d
elecommunica ion op ical ibe has an a enua ion a ound
0.2 dB/km.
The pulse epe i ion a e is dependen on he maximal leng h
o he op ical ibe , pulse epe ion a e can be exp essed as [9]:
τ=2·L
υ=2·L
c/n (s)(4)
o ou measu e sys em du a ion o he pulse is [9]:
τ=2·L
c/n =2·40 ·103
3·108/1.46 = 3.89 ·10−4(s)(5)
whe e epe i ion a e can be calcula ed as [9]:
=1
τ=1
3.89 ·104= 2.57(kHz).(6)
IV. SYSTEM DESCRIPTION
Ou sys em desc ip ion can be di ided in o wo pa s. The
i s pa ocuses on dense wa eleng h di ision mul iplex, hei
unc ion and se ings. The second pa ocuses on φ–OTDR
sys em. Ou designed sys em is depic ed in Fig.1.
Recei ing pa
T ansmi ing pa
Senso ic sys em
pulses 130 ns,
epe i ion a e 2.57 kHz,
–30 dBm – +20 dBm
DWDM sys em DWDM sys em
Senso ic sys em
M
U
X
D
E
M
U
X
Op ical ibe
40 km, G.652.D
Fig. 1. Block schema ic o sys em
In ou sys em we use ou DFB lase s o DWDM sys em
and one DFB lase o ibe op ics senso . Lase o op ic
senso has wa eleng hs s a ing a 1550.5nm; 1551.0nm;
1551.5nm; 1552.0nm; 1552.5nm; and powe pe o mance is
a iable. These wa eleng hs a e used o in luence he i s
channel o DWDM. Senso ic sys em is shi ed om DWDM
sys em abou 0.5 nm and he ange o wa eleng h o senso ic
M. CUCKA e al.: TRANSMISSION OF HIGH POWER SENSOR SYSTEM AND DWDM DATA SYSTEM
191
sys em is inc eased in compa ison wi h DWDM. Cohe en
leng h o used lase o φ–OTDR is abou 750 Hz. This
leng h is used o 40 km op ical ibe . Lase s o DWDM ha e
wa eleng h o 1550 nm, 1550.8 nm, 1551.6 nm, 1552.4 nm and
powe 3 dBm. Da a sys em ansmi s da a 10 Gbi /s wi h BER
(Bi E o Ra e) abou 1.91E−40.
Fi s o all, we simula e he op ical pa h wi h 40 km op ical
ibe wi hou ampli ie s. We use s anda d elecommunica ion
ibe G.652.D wi h a enua ion 0.2 dB/km. In op ical ib es,
he a enua ion is mainly caused by wo physical ac o s,
abso p ion and sca e ing losses. Abso p ion is caused by ib e
ma e ial and sca e ing due o s uc u al impe ec ions wi hin
he ib e. Mic obending o op ical ib e also con ibu es o he
a enua ion o signal.
Ou simula ion con ains CD (Ch oma ic Dispe sion) and
PMD (Pola iza ion Mode Dispe sion) which a ec ing he
shape and cou se o he ansmi ed signal. I we ake in o
accoun hese e ec s, ou DWDM sys em has clea eye o he
decision.
A ansmi ing pa o DWDM sys em in VPIpho onics is
depic ed in Fig. 2. I is a module which gene a es pseudo
andom da a sequence. A ano he block gene a es a sampled
NRZ (Non Re u n o Ze o) coded signal de ined by a sequence
o bi s a i s inpu . The signal is edi ed by Gaussian il e
ha ans o ms elec ical inpu pulses in o smoo he ou pu
pulses. In ou ansmi e we use Mach-Zehnde modula o
which modula es signal om gene a o o he DFB lase . O he
blocks in Fig. 2 a e o p ope unc ion o he simula ion.
Fig. 2. T ansmi ing pa o he DWDM sys em in VPIpho onics.
A ecei ing pa o he sys em consis s o wo ypes o
il e s, Lo en zian and Bessel (op ical and elec ical). These
ypes o he il e s a e con igu ed by ecei ing wa eleng h. Ou
simula ion ocuses on unc ion o DWDM sys em, we do no
conside o wa ch he BER o senso sys em. In ou simula ion
we use DMUX 4 which has ex ension a io abou 20 dB. We
wan o simula e eal pa ame e s o he bo h sys ems (DWDM
and φ–OTDR ). A ecei ing pa o he DWDM sys em can
be seen in Fig. 3
Fig. 3. Recei ing pa o he DWDM sys em in VPI pho onics.
V. SIMULATION
We s a a –30 dBm powe o senso ic sys em and wa ch
he BER o each channel o DWDM sys em which un a
10 Gbi /s. In ou simula ion we ha e ou channels DWDM.
DWDM sys em is shi ed om senso ic sys em abou 1 nm. In
his case he BER o all channels a e abou 1E−40 and eyes
o he decision a e clea . When we g adually inc ease powe o
he senso ic lase , we can see in all g aphs ha he BER slowly
dec eases and eye o he decisions is no clea . I inc eases i
he senso ic lase has he powe a ound 0 dBm. Wi h high
powe o he senso ic lase (abou 13 dBm) DWDM is no
able o ans e da a (1E−7). Tha means da a ansmission is
unsuccess ul. In schema ic Fig. 4 we can see he simula ion
se up in VPI pho onics which is desc ibed ea lie .
Fig. 4. Lase and DWDM sys em con igu a ion in VPIpho onics.
The i s esul s o ou simula ions a e shown in Fig. 5.
I shows he in luence o he senso ic sys em o DWDM
sys em shi ed o 1 nm. Wa eleng h o he DWDM sys em is
1551.6 nm which is he hi d channel o DWDM sys em. We
s a wi h BER 1E−40 and inc ease he powe o senso ic
sys em. Dependence shows ha he BER o he hi d channel
DWDM sys em g adually dec eases wi h inc easing powe . All
g aphs also include he cu e ha shows BER limi o DWDM
sys em.
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10−210−1
10−7
102
1011
1020
1029
1038
BER limi
(W)
–BER(—)
1553.4 nm
1552.4 nm
Fig. 5. In luence o he φ–OTDR o he DWDM sys em (1551.6 nm).
Fig. 6 depic s he dependency o high powe senso sys em
(abou 27 dBm) o DWDM sys em. Dis ance be ween da a
sys em and senso ic sys em is 0.5 nm.
10−210−1
10−3
104
1011
1018
1025
1032
BER limi
(W)
BER (-)
1550.5 nm
1551 nm
Fig. 6. In luence o he high powe φ–OTDR o he DWDM sys em.
Ano he impo an pa o he measu emen s is a di e ence
be ween wa eleng h spacing DWDM and φ–OTDR ha can be
seen in Fig. 7. I we ha e small spacing, in luence o φ–OTDR
sys em on he i s channel o DWDM sys em is highe han
a dis ance o mo e han 2.5 nm, when sys em is no a ec ed.
Ou designed model also includes he non-linea and linea
e ec s. Dis ance be ween da a sys em and senso ic sys em is
a iable. We ocus on dis ance by 0.5 nm, 1 nm, 1.5 nm, 2 nm,
2.5 nm.
10−210−1
10−12
108
1028
1048
1068
1088
BER limi
(W)
–BER (—)
1550.5 nm
1551 nm
1551.5 nm
1552 nm
1552.5 nm
Fig. 7. In luence o he φ–OTDR o he DWDM sys em wi h a iable dis ance.
VI. CONCLUSION
Ou simula ion sys em designed in he VPI pho onics so -
wa e showed ha i is possible o use an op ical ibe o
DWDM ansmission and i can be also used as an op ical
senso . This da a ansmission sys em is limi ed by maximum
op ical powe o he used lase o he senso sys em. Ou sim-
ula ion shows ha DWDM can ansmi da a i he powe o
φ–OTDR is unde 13 dBm. I was also e i ied ha a dis ance
o 2.5 nm i is no possible o a ec DWDM sys em wi h φ–
OTDR. Fu u e wo k aims o use ano he pulse gene a o wi h
di e en ange o pulse. These gene a o can make pulses om
10 ns o 1000 ns wi h di e en epe i ion a e o he pulses. The
mos impo an u u e wo k is measu emen in he unc ion o
DWDM sys em. This measu emen con i ms o disapp o es
ou simula ions.
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Milan Cucka (MSc.) was bo n in Vysko , Czech
Republic on Janua y 20, 1989. He ecei ed his
M.Sc. deg ees in Telecommunica ions om he B no
Uni e si y o Technology, B no, in 2014. His e-
sea ch in e es s include dis ibu ed op ical senso s,
op oelec onics, and ibe b agg g a ings. Cu en ly,
he has been pos g adua e s uden a B no Uni e si y
o Technology, Depa men o Telecommunica ions
and his opic o disse a ion hesis is dis ibu ed ibe
op ics sys ems.
Pe Muns e (MSc., Ph.D) was bo n in Zlin,
Czech Republic. In 2010 he g adua ed om he B no
Uni e si y o Technology and ecei ed his academic
i le o elec ical enginee (Ing.). His esea ch wo k
ocuses on op ical communica ions, especially FTTx
access ne wo ks and OTDM sys ems, and be op ic
senso s. He is an au ho o co-au ho o mo e han
wen y publica ions in scien ic jou nals and a in e -
na ional con e ences. He is a membe o p og am
commi ees o se e al con e ences.
Lukas Koci (MSc.) was bo n on 29 Sep embe 1990
in B no, Czech Republic. He g adua ed om he
B no Uni e si y o Technology and ecei ed aca-
demic i le Ing a he Depa men o Telecommuni-
ca ions. Cu en ly, he is s udying Doc o al p og am
a he B no Uni e si y o Technology, Depa men o
Telecommunica ions. His esea ch ocuses on op ical
communica ion ne wo ks, op ical ime di ision mul-
iplexing, wa eleng h di ision mul iplexing, passi e
op ical ne wo ks, and especially so wa e de ined
op ical ne wo ks.
Tomas Ho a h (MSc.) was bo n in Ha i o , Czech
Republic on Ma ch 7, 1989. He ecei ed his M.Sc.
deg ees in Telecommunica ions om he B no Uni-
e si y o Technology, B no, in 2013. His esea ch
in e es s include passi e op ical ne wo ks (xPON),
op oelec onics, and Bi To en p o ocol. Cu en ly,
he has been pos g adua e s uden a he B no
Uni e si y o Technology, Depa men o Telecom-
munica ions and his opic o disse a ion hesis is
Op imiza ion se ices in FTTx op ical access ne -
wo ks.
Milosla Filka p o . was bo n in 1946 in B no,
Czech Republic. Since 2010 he has been a p o-
esso a he Depa men o Telecommunica ions a
he B no Uni e si y o Technology. He is a leade
o he op ical g oup Op oLab and also a head o
he Labo a o y o ansmission media and op ical
ne wo ks. He is a membe o a se e al ins i u es (e.g.
Ins i u e o Elec ical Elec onics Enginee es) and is
also a commi ee o many con e ences (In e na ional
Con e ency Telecommunica ions and Signal P o-
cessing, In e na ional Con e ency New In o ma ion
and Mul imedia Technologies). His cu en esea ch hemes ocus on ibe -
op ic elecommunica ions, especially FTTx echnologies.
Jose Voj ech (MSc., B.Sc., Ph.D) ecei ed wi h
hono s M.SC. deg ee in Compu e Science, B.Sc.
deg ee in Pedagogy and Ph.D. in ield o op ical
ne wo king om he Czech Technical Uni e si y,
P ague, in 2001, 2003 and 2009 espec i ely. Since
2003, he has been wi h esea ch Depa men o
Op ical Ne wo ks, CESNET, a.l.e., which he leads
now. He pa icipa ed in in e na ional p ojec s: COM-
PLETE, FI-PPP XIFI, GN4, GN3+, GN3, GN2,
Po a Op ica S udy, SEEFIRE. He has been also
esponsible o de elopmen o open amily o pho-
onic de ices. He holds 15 pa en s (including 3 US and 1EU) and u ili y
models. His eco d shows Hi sch index 5 wi h mo e han 64 ci a ions. He is
a membe o IEEE, OSA and SPIE. In 2007 he ecei ed he Resea ch p ize
o he Czech minis e o educa ion.
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JOURNAL OF COMMUNICATIONS SOFTWARE AND SYSTEMS, VOL. 12, NO. 4, DECEMBER 2016