MIME-Version: 1.0 Content-Type: multipart/related; boundary="----=_NextPart_01CE0857.EAF86F50" Αυτό το έγγραφο είναι ιστοσελίδα ενός μόνο αρχείου, γνωστό και ως αρχείο αρχειοθέτησης Web. Αν βλέπετε αυτό το μήνυμα, το πρόγραμμα περιήγησης ή επεξεργασίας δεν υποστηρίζει αρχεία αρχειοθέτησης Web. Κάντε λήψη ενός προγράμματος περιήγησης που υποστηρίζει αρχεία αρχειοθέτησης Web, π.χ. Microsoft Internet Explorer. ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" PowerPoint Presentation

Αυτή η παρουσίαση περιέχει στοιχεία τα οποία ίσως να μην προβληθού&#= 957; σωστά από το πρόγραμμα περιήγησης. Η παρουσίαση αυτή έχει βελτιστοποιη = 52;εί για τις νεότερες εκδόσεις του Microso= ft Internet Explorer.

Εάν θέλετε να συνεχίσετε, κάντε κλικ εδώ.

 ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/master45.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii"
‹ημ = 49;ρομηνία/ώρα›
‹υποσέλιδο›= ;
‹#›
Κάντε κλικ για να επεξεργαστεί = 64;ε τα στυλ κειμένου του υποδείγματος= 3;
Δεύτερου επιπέδου
Τρίτου επιπέδου
Τέταρτου επιπέδου
Πέμπτου επιπέδου
Κάντε κλικ για επεξεργασία του τίτλου
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file:///C:/0EC8A292/OptikesInes2.files/master46.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii"
Κάντε κλικ για επεξε&= #961;γασία του τίτλου
Κάντε κλικ για να επε= ξεργαστείτε τον υπότιτλο τ&= #959;υ υποδείγματος
‹ημερο&#= 956;ηνία/ώρα› =
‹&#= 965;ποσέλιδο› =
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------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/master46.xml Content-Transfer-Encoding: quoted-printable Content-Type: text/xml; charset="utf-8" ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/pres.xml Content-Transfer-Encoding: quoted-printable Content-Type: text/xml; charset="utf-8" ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/slide0001.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" PowerPoint Presentation

ΘΕΜΑ: ΟΠΤΙΚΕΣ  ΙΝΕΣ
ΕΡΓΑ = 31;ΙΑ ΣΤΗΝ ΤΕΧΝΟΛΟΓΙΑ ΕΠΙΚΟΙΝΩΝΙΩΝ
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Ι= ;στορικά Στοιχεία
§= Η ιδέα της χρήσης του φωτός για την επικοινωνία σ&= #949; μεγάλες αποστάσεις έχει τις ρίζες= της στην αρχαιότητα = §Ο = 53; αρχαίοι Έλληνες άναβαν φωτιές σε ψηλά σημεία= , όπως κορυφές βουνών, για να = ανταλλάξ&#= 959;υν πληροφορίες =
<= span style=3D'font-size:44%'>§Α = 61;γότερα χρησιμοποιήθ&#= 951;κε το άναμμα των πυρσών
§Σ = 64;α τέλη του 19ου αιώνα και στις αρχές του 20ου ο = 53; καπετάνιοι των πλοίων χρησιμοπ&#= 959;ιούσαν ειδικούς ισχυρούς φακούς τους οπ= οίους αναβόσβηναν<= span lang=3DEN-US style=3D'font-size:44%'> σύμφωνα με τ&= #959;ν Κώδικα Moρs (ανακαλύφθηκε το 1854 από τον Samuel Morse), = §Τ = 59; 1790 ο Γάλλος μηχανικός Claude παρουσίασε τον οπτικό τηλ= έγραφο με τον οποίο = μπορούσε να στείλει μήνυμα χωρίς προσυννενόησ&#= 951; §γ = 73;ρω στα 1880, ο Alexander Graham Bell παρουσίασε το οπτικό τηλεφωνικό σύ&= #963;τημα το οποίο ονόμασε φωνόφωνο
<= span style=3D'font-size:44%'>§Τ = 59; όνειρο του μεγάλου εφευρέτη ήταν η μετάδοση των φωτεινών σημάτων
<= span style=3D'font-size:44%'>§Π = 59;λύ αργότερα, εμφανίστηκε μια νέα τεχνολογία
uΠρόκειται για τις οπτικές ίνες δηλ. τις πολύ λεπτές κυλινδρικές ίνες γυαλιού, με τη βοήθεια των οποίων μπορούμε να «αναγκάσουμε&= raquo; μια φωτεινή δέσμη να ακολουθήσει = όποια διαδρομή επιθυμούμε §To γυαλί, η πρώτη ύλη της οπτικής ίνας εμφανίστηκε γ&= #953;α πρώτη φορά γύρω στα 2500 π.χ.
<= span style=3D'font-size:88%'>§ Επομένως η τεχνική υποδομή για τις οπτικές ίνες υπήρχε από νωρίς.
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ΙΣΤΟΡΙ&= #922;Α ΣΤΟΙΧΕΙΑ
§= Τη δεκαετία του 1920 ένας Βρετανός και ένας Αμερικανός συνέλαβαν την ιδέα χρήσης = των οπτικών ινών για τη μετάδοση εικόνας = §=  ]= 2;ο θέμα έμεινε στάσιμο μέχρι που το 1930 ο Heinrich Lamm μετέδωσε για πρώτη φορά εικόνα χρησιμοποιών&#= 964;ας δέσμη οπτικών ινών, με στόχο να αποκτήσει ορατότητα σε σημεία του σώματος μη προσβάσιμα οπτικώς. §=  [= 9; μετάδοση δεδομένων στηρίζεται στη χρήση χάλκινων καλωδίων για την μεταφορά = διαμορφω&#= 956;ένων ηλεκτρικών σημάτων. §=  ]= 2;ο 1966 διαπιστώθηκ = 49; ότι οι διάφανες γυάλινες ίνες μπορούν να γίνουν κατάλληλοι = κυματοδη&#= 947;οί φωτεινής ακτινοβολίας § Τέσσερα χρόνια αργότερα, παράγονται οι πρώτες οπτικέ&= #962; ίνες για πρακτικές εφαρμογέ&#= 962;
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ΔΙΑΚΡΙΣΕΙΣ ΣΤΟΝ ΤΟΜΕΑ ΤΩΝ ΟΠΤΙΚΩΝ ΙΝΩΝ=
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§= Το βραβεί&= #959; Νόμπελ Φυσικής για το 2009 απονεμήθηκε στον καθηγητή Charles K. Kao γ&= #953;α τα επιτεύγματα του, σε σχέση μ^= 9; την διάδοση το= υ φωτός σε ίνες για τις οπτικές επικοινω&#= 957;ίες §Ο Kao γεννήθηκε στη Σαγκάη το 1933, σπούδασε Ηλεκτρολόγος Μηχανικός και έλαβε το διδακτορικό στην Ηλεκτρολογικ&#= 942; Μηχανική από τ= ο Πανεπιστήμιο του Λονδίνου το 1965 &#= 13;§Τ = 59; 1966 δημοσίευσε ένα άρθρο στα IEE Proceedings, μαζί με τον συνάδελφ&#= 959; του George Hockham, Το κύρι&#= 959; αποτέλεσμα της έρευνας ήταν πως οι απώλειες οφείλονταν στην απορρόφηση και τη διασκόρπιση του φ&= #969;τός μέσα στην οπτική ίνα, εξ’αιτίας των ατελειών στο γυαλί και συγκεκρι&#= 956;ένα των ιόντων σιδήρου. §ο Kao προέβη σε μια τολμηρή δήλωση Η ίνα από γυάλινο υλ= ικό, κατασ= κευασμένη με επικάλυψη συνιστά ένα πιθανό πρακτι&= #954;ό οπτικό κυματοδηγό, με σημαντικές προοπτικές ως μια καινούρια μορφή μέσου επικοινω&#= 957;ίας §Ο Ka= o 3 χρόνια αργότερα, πρότεινε την χρήση του οξειδίου του πυριτίου για τις οπτικές ίνες
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------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/slide0005.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" PowerPoint Presentation
ΒΑΣΙΚΑ ΧΑΡΑΚΤΗΡΙΣΤΙ&#= 922;Α ΟΠΤΙΚΩΝ ΙΝΩΝ
§= Χρησιμοπ&#= 959;ιείται, κυρίως, όπου οι αποστάσεις είναι μεγάλες και δεν μπορεί να χ= ρησιμοποιηθε = 43; το καλώδιο συνεστραμένω&#= 957; ζευγών και όπου οι απαιτήσεις σε ρυθμούς μετάδοση&#= 962; είναι αρκετά αυξημένες = = §μ = 60;ορούμε να χρησιμοποιήσ&#= 959;υμε οπτική ίνα για να καλύψουμε απόσταση 5Km κ^= 5;ι οι ρ&= #965;θμοί μετάδοσης δεδομένων φθάνουν τα 10 Gbps. §Μ = 49; την βοήθεια των οπτικών ινών μπορούμε να “αναγκάσου= με” μια φωτεινή δέσμη να = ακολουθή&#= 963;ει όποια διαδρομή επιθυμούμε. Γι’αυτό λέμε ότι μια οπτική ίνα είναι ένας= = φωτοαγωγ= ;ός ή φωτοοδήγος.
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ΒΑΣΙΚΗ ΧΗΜΙΚΗ ΑΝΤΙΔΡΑΣΗ
u
SiCl4 (gas) + O2 ( SiO2 (solid)) + 2Cl2 (Υψηλή θερμοκρασία)

GeCl<= /span>4 (gas) + O2 ( GeO2 (solid)) + 2Cl2 (Υψηλή θερμοκρασία)
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file:///C:/0EC8A292/OptikesInes2.files/slide0007.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" PowerPoint Presentation
Τ&#= 929;ΟΠΟΙ ΜΕΤΑΔΟΣΗΣ ΣΤΙΣ ΟΠΤΙΚΕΣ ΙΝΕΣ
<= span style=3D'font-size:44%'>§Η εκπομπή του οπτικού σήματος σε οπτική ίνα γίνεται από πηγή LED
uμήκη κύματος του φωτός, που η οπτική ίνα είναι σχεδιασ&= #956;ένη να μεταφέρει, ποικίλουν από 800nm μέχρι 1500nm.
<= span style=3D'font-size:44%'>§Ο = 53; οπτικές ίνες διαφοροποιού&#= 957;ται από τον τρόπο μ= ;ετάδοσης του σήματος =
§Η πρώτη βασική διάκριση είναι μεταξύ των πολύτροπω&= #957; και μονότροπων οπτικών ινών.
<= span style=3D'font-size:44%;visibility:hidden'>§
u
125μm= 3;
125μm= 3;
125μm= 3;
125μm= 3;
125μm= 3;
125μm= 3;
125μm= 3;
Διάμε= τρος περιβλήματ&= #959;ς
62.5μm= 3;
50μm= 3;
50μm= 3;
9μm= 3;
9μm= 3;
9μm= 3;
9μm= 3;
Διάμε= τρος πυρήνα
IEC <= /span>60793-= 2= 3;
ISO/IEC 11801= 3;
ITU-T G.651= 3;
ITU-T G.657= 3;
ITU-T G.655C= 3;
ITU-<= /span>T G.652D= 3;
ITU-<= /span>T G.652B= 3;
Πρότυ= πο
Graded = index <= span style=3D'mso-bidi-font-family:Arial'>62.5/12= 5= 3;
Graded = index = 50/125 = OM3= 3;
Graded = index <= span style=3D'mso-bidi-font-family:Arial'>50/125 = OM2= 3;
Bending = loss = insensitiv= e= 3;
Non-zero = Dispersi<= span style=3D'position:absolute;top:62.0%;left:43.07%;width:6.55%;height:2.5%'>= on = Shifted= 3;
Low <= /span>water peak= 3;
Standard
step index= 3;
Τύπος= ίν= ας
Πολύ = 64;ροπες οπτικές ίνες (Multi-mode)
Μονό = 64;ροπες οπτικές ίνες (Single-mode)
Χαρα = 54;τηριστικό
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Π= ;ολύτροπες οπτικές ίνες (<= /span>Multimode fiber optics<= span style=3D'font-size:45%'>)
§= Οι πολύτροπες οπτικές ίνες έχουν τυπικά μεγέθη 50μm/ 125μm, 62,5/125, 85/1= 25 ή 100/140
§ = Ο συνηθέστερος τύπος, ο οποίος κυκλοφορεί, είναι ο 62,5/125
§<= /span>ο τρόπος μετάδοσης ονομάζεται πολύτροπος (multimode), επειδή έχουμε πολλούς = δρόμους μετάδοσης, που αντιστοιχούν στις διαφορετ&= #953;κές γωνίες ανάκλασης <= /div>
§ \= 7;ι πολύτροπες οπτικές ίνες διακρίνονται σε δυο κατηγορ= ίες: τις διακριτού βήματος = (step index) και τις βαθμιαίου βήματος (graded index)= .
§= Στις διακριτού βήματος συμβαίνει απότομη μεταβ&= #959;λή του δείκτη διάθλασης μεταξύ της = κεντρική&#= 962; ίνας και του υλικού επίστρωσης <= /span>
§= Οι ίνες αυτές χαρακτηρίζον&#= 964;αι από βαθμιαία μεταβολή του δείκτη διάθλασης του υλικού της κεντρικής ίνας. Συμβαίνε= ι βαθμιαία μείωση όσο απομακρυ&#= 957;όμαστε από το κέντρο προς την εξωτερική επιφάνεια του = = γυαλιού.=
§
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ΜΟΝΟΤΡΟΠΕΣ ΟΠΤΙΚΕΣ ΙΝΕΣ=
=
§= Στις μονότροπες οπτικές ίνες η διάμετρος της κεντρικής ίνας είναι πολύ μικρή και= = πλησιάζε&#= 953; περίπου το επίπεδο του μήκους κύματος του εκπεμπόμενου σήματος
§=  Z= 4;χουμε έναν μόνο δυνατό τρόπο μετάδοσης του οπτικού σήματος, τον αξονικό.
§Η κεντρική ίνα στις μονότροπες οπτικές ίνες έχει διάμετρο από 5μm έως 10μm με = συνηθέστ&#= 949;ρη τιμή τα 8,3 μm.
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ΕΠΙΔΟΣΕΙΣ ΟΠΤΙΚΩΝ ΙΝΩΝ=
=
<= span style=3D'font-size:44%'>§Ο = 53; επιδόσεις μιας οπτικής ίνας συνδέονται με τον τρόπο μετάδοσης του σήματος
§Σ = 64;ις μονότροπες οπτικές ίνες χρησιμοποιού&#= 957;ται μήκη κύματος μεταξύ των 1310 nm και των 1550 = nm
<= span style=3D'font-size:44%'>§Σ = 64;ις πολύτροπες οπτικές ίνες έχουμε μήκη κύματος από 850 <= span lang=3DEN-US style=3D'font-size:44%'>nm έως 1300 = nm
§ Οι πολύτροπες οπτικές ίνες μπορούν να χρη= σιμοποιηθούν σε αποστάσεις, που υ&= #960;ερβαίνουν τα 3Km<= span style=3D'font-size:44%'>, ενώ οι μονότροπες οπτικές ίνες μπορούν να υπερβούν τα 10 = Km. §Σ = 64;ις πολύτροπες οπτικές ίνες μπορούν να χρησιμοποιηθ&#= 959;ύν χαμηλ= ού κόστους πηγές = LED, ενώ οι μονότροπες οδηγούνται συνήθως από πηγή LASER. Τυπική τιμή εξασθένισης σήματος για μια 62,5/125 πολύτροπη οπτική ίνα είναι 3,5 dB/Km γ_= 3;α σήμα με μήκος κύματος 850 nm κ^= 5;ι 1.0 dB/Km για μήκος κύματος 1300nm. Τυπικό μέγεθος εξασθένισης σήματος για μονότροπη οπτική ίν&= #945; είναι 0,5 dB/Km σ`= 4;α 1310 nm και 0,4 dB/Km στα 1550nm.
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ΤΥΠΟΙ ΟΠΤΙΚΩΝ ΙΝΩΝ
<= span style=3D'font-size:44%'>§Θ = 45; ξεχωρίσουμε δυο τύπους οπτικών ινών ως προς την κατασκευή τους.
u. Στην πρώτ&= #951; περίπτωση, έχουμε σε κάθε οπτική ίνα και εξωτερικά από την ε&= #960;ίστρωση συνθετικές ίνες και εξωτερικό μονωτικό περίβλημα. Μέσα στο καλώδιο υπάρχουν πολλές τέτοιες ίνες, όπου η κάθε ίνα αποτελεί και ένα ξ= εχωριστό καλώδιο. Μέσα στο καλώδιο περιέχονται ε&= #954;τός από καλώδια οπτικών ινών και καλώδια, τα οποία χρησιμεύουν για ενίσχυση και σ= ;τρογγυλοποίη&#= 963;η του όλου σχήματος. Αυτή η κατασκευή είναι γνωστή σαν Tight Buffer §Σ = 64;ην δεύτερη περίπτωση, έχουμε τις οπτικές ίνες μ= ε την επίστρωση = τους να είναι τοποθετημένε&#= 962; ελεύθερα μέσα στο καλώδιο και π= ερικλείονται από εξωτερικό περίβλημα, αφού πρώτα τοποθετηθεί = μέσα στο καλώδιο επίστρωση από συνθετικές ίνες για την ανθεκτικ&#= 972;τητα του καλωδίου. Αυτή η κατασκευή είν&= #945;ι γνωστή σαν Loose Buffer
u
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ΠΑΡΑΔΕΙΓΜΑΤΑ ΧΡΗΣΕΙΣ ΟΠΤΙΚΩΝ ΙΝΩΝ
§= Τα καλώδι&= #945; οπτικών ινών χρησιμοποιού&#= 957;ται, κυρίως, από τους τηλεπικοινων&#= 953;ακούς οργαν&= #953;σμούς για επίγειες και υποθαλάσσιες συνδέσεις μεγάλων αποστάσεων, αντικαθι&#= 963;τώντας τόσο τις γραμμές ομοαξονικών κ&= #945;λωδίων, όσο και τις επίγειες και δορυφορι&#= 954;ές μικροκυματικ&#= 941;ς ζεύξεις. Τα τελευταία χρόνια έχουν ποντισθεί πολλά καλώδια οπτικών ινών, με χωρητικότητα, η οποία ξεπερν= ά τα 30.000 κυκλώματα= = φωνής, για τη διασύνδεση ηπείρων. Τέτοια παραδείγματα αποτελούν το καλώδιο = BSFOCS, που εκτείνεται στην περιοχή της Μαύρης θάλασσας και συνδέει τη Βουλγαρί&#= 945;, Ουκρανία και Ρωσία, το καλωδιακό σύστημα SEA - Μ&= #917; - WE 3 (South East Asia - Middle East - West Europe), που ξεκινά από τη Δυτική Ευρώπη (Γερμανία, Μεγ. Βρετανία), περνά από τα στενά του Γιβραλτάρ στη Μεσόγειο (Ιταλία, Ελλάδα= ;, Κύπρο) συνεχίζει από τα στενά του Σουέζ προς την Ασία
§= Οι οπτικέ&= #962; ίνες χρησιμοποιού&#= 957;ται, επίσης, από ιδι= ;ωτικές εταιρίες σε τοπικά δίκτυα, σε π&= #945;νεπιστημιακ^= 0; δίκτυα κορμού, σε δίκτυα ευρείας περιο&= #967;ής, σε δίκτυα καλωδιακής τηλεόρασ&#= 951;ς, σε εφαρμογές με υψηλές απαιτήσεις σε = ασφάλεια μετάδοσης, όπως οι στρατιωτ&#= 953;κές και, τέλος, σε βιομηχανικές εφαρμογές, όπου υπάρχει υψηλός βιομηχανικός θόρυβος, στον οποίο οι οπτικές ίνες π= αρουσιάζουν ανοσία.
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Π&#= 923;ΕΟΝΕΚΤΗΜΑΤΑ ΟΠΤΙΚΩΝ ΙΝΩΝ=
§ &nbs= p; 1) μπορούν να μεταφέρουν παράλληλα πολύ μεγαλύτερο όγκο δεδομένων σε σχέση με το χάλκινο καλώδιο
2) η μεταφορ= ά των δεδομένων γίνεται γρηγορότερα
3) είναι λιγότερο ευάλωτα τα δεδομένα που ταξιδεύουν μέσα τους, σε παρεμβολές
4) είναι πολ= ύ πιο λεπτές και ελαφρύτερες από το χάλκινο καλώδιο.
5) τα δεδομένα μεταδίδονται ψηφιακά: άρα πιο γρήγορη κωδικοποίηση -= = αποκωδικ&#= 959;ποίηση δεδομένων, σχεδόν καθόλου απώλε&= #953;ες δεδομένων.


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Μ&#= 917;ΙΟΝΕΚΤΗΜΑΤΑ ΟΠΤΙΚΩΝ ΙΝΩΝ=
§     1) είναι πιο ακριβές,
2) είναι πιο δύσκολη η εγκατάστασή τους,
3) είναι πιο εύθραυστες,
4) δεν μπορούμε να τις λυγίζουμε πολύ, θα πρέπει να τις εγκαθιστούμε με ελαφριά κλίση, γιατί αλλιώς θα έχουμε απώλειες.
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ΜΕΡΗ ΟΠΤΙΚΗΣ ΙΝΑΣ
uκάθε οπτική ίνα αποτελείται από τρία μέρη: =
1)Τη&= #957; κεντρική γυάλινη κυλινδρική ίνα, που ονομάζεται πυρήνας = και είναι το τμήμα στο οποίο διαδίδεται το φως.
2)Τη&= #957; επικάλυψη (απλή ή πολλαπλή), που είναι ένας ομό= κεντρος με τον πυρήνα κύλινδρο&#= 962;. Έχει μικρότερο δείκτη διάθλασης από τον πυρήνα, για να παθαίνει το φως σ= υνεχείς ολικές ανακλάσεις. Η επικάλυψη αυτή ονομάζετ&= #945;ι μανδύας
<= span style=3D'font-size:44%'>3) Το περίβλημ= ;α, που είναι ένα αδιαφανές πλαστικό.
<= span style=3D'font-size:44%;visibility:hidden'>§
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ΕΞΑΣΘΕΝΗΣΗ ΤΟΥ ΦΩΤΟΣ
uΤο φως κατά το “ταξίδι” του σε μια οπτική ίνα εξασθενεί. Αυτό συμβαίνει συνήθως για = τους παρακάτω λόγους:
§= Λόγω απορρόφησης= , που οφείλεται στις ξένες προσμείξεις που υπάρχουν στο γυαλί
§= Λόγω σκέδασης το φως διεισδύει στο μανδύα και διασκορπίζετ&#= 945;ι. Το φαινόμενο αυτό παρατηρείται εντονότερα, αν στην οπτική ίνα υπάρχουν συνδέσεις.
§= Λόγω κακής κατασκευής υπάρχουν στην διάμετρο του πυρήνα, για παράδειγμα, = μικροδια&#= 954;υμάνσεις.
§= Λόγω μεγάλης καμπής της οπτικής ίνας.
§= ;
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Τ= ΡΟΠΟΣ ΛΕΙΤΟΥΡΓΙΑΣ ΟΠΤΙΚΩΝ ΙΝΩΝ=
§= Στο ένα άκρο της οπτικής ίνας, υπάρχει ο πομπός και στο άλλο, ο δέκτης.

§= Ο πομπός, μετατρέπει τα ψηφιακά δεδομένα ενός υπολογιστή, σε ψηφιακά κύματα φωτός. =
§= Ο δέκτης, αποκωδικοποι&#= 949;ί τα ψηφιακά κύματα φωτός, σε ψηφιακά δεδομένα.
Τα ψηφιακά κύματα φωτός, ταξιδεύουν με την ταχύτητα του φωτός μέσα από την οπτική ίνα, με διαδοχικές ανακλάσεις στα τοιχώματα της οπτικής ίνας.

Οι ανακλάσεις αυτές, γίνονται στα τοιχώματα, σε γ= ;ωνία μικρότερη των = 42 μοιρών, με αποτέλεσμα να = = λειτουργ&#= 959;ύν τα τοιχώματα σαν καθρέφτες.

Το φαινόμενο αυτό ονομάζεται ολική ανάκλαση και είναι η αιτία που τα κύματα φωτός μένουνε = μέσα στην οπτική ίνα, συνεχίζοντας το ταξίδι τους μέχρι το άλλο άκρο, χωρίς να βγαίνουν-χάνο&= #957;ται έξω απ= ό την ίνα.

Σε αυτ= ό συνεισφέρει και η δομή της. Το εσωτερικό μ= έρος της οπ = 64;ικής ίνας, ονομάζεται πυρήνας και = μέσω αυτο&= #973;, ταξιδεύουν τα κύματα φωτός. Ο πυρήνας, είναι περιτυλιγμέν&#= 959;ς από μία άλλη στρώση πλαστικου - γυαλιου που ονομάζεται περίβλημα. Το π= ;ερίβλημα από τις οπτικές ίνες, είναι έτσι κατασκευ&#= 945;σμένο, ώστε να κρατάει τα κύματα φωτός, μ= ;ε ολικές ανακλάσεις, μέσα στον πυρήνα και <= span style=3D'font-size:38%'>να συνεχίζουν το ταξίδι τους μέσω αυτού (του πυρήνα).

Το περίβλημα το πετυχαίνει αυτό, λόγω της διαφορετικότ&#= 951;τας του υλικού από το οποίο είναι= <= span style=3D'font-size:38%'>κατασκευ&#= 945;σμένο, σε σχέση με το υλικό του πυρήνα.
3D"οπτικέ=
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ΔΗΜΙΟΥΡΓΙΑ ΚΑΛΩΔΙΟΥ ΟΠΤΙΚΩΝ ΙΝΩΝ
§= Η δημιουργία μιας οπτικής ίνας πραγματοποιε&#= 943;ται σε τρία βήματα, που είναι ο σχηματισμός ενός αρχικού υάλινου κυλίνδρου, η τομή των ινών από τον κύλινδρο αυτό, καθώς και η δοκιμή για την= αντοχή τους, αλλά και για την σωστή λειτουργία το&= #965;ς.
§= Στο πρώτο στάδιο, γίνονται όλες οι απαραίτητες χημικές διαδικασίες για τον σχηματισ&#= 956;ό του καθαρού γυαλιού, ενώ ειδικός εξοπλ&= #953;σμός αναλαμβάνει να α&#= 960;ομακρύνει από τον υάλινο κύλινδρο όλα τα ξένα σώματα, που θα είχαν ως= ; = αποτέλεσ&#= 956;α τη μείωση της απόδοσης της οπτικής ίνας.
§= Αφού δημιουργηθεί ο αρχικός κύλινδρος, στη συνέχεια τοποθετείται σε μια συσκευή η οπο= ;ία έχει το σχήμα πύργου και αναλαμβάνει τη δημιουργία των μικροσκοπικώ&#= 957; ινών. Ο πύργος αυτός λιώνει το γυαλί σε θερμοκρασία περίπου 2.300 βαθμών Κελσίου και = στη συνέχεια αυτό ρέει κατακόρυφα από μικρές οπέ= ς, οπότε και ψύχεται σταδιακά, = ώστε να πάρει την τελική μορφή οπτικής ίνας.
§= Στο τελικ&= #972; στάδιο, η οπτική ίνα περνά από ένα σύνολο ελέγχων που εξασφαλίζουν ότι ε= ίναι σε θέση να διατεθεί προς χρήση, χωρίς να προξενηθούν τυχόν προβλήματα κατά τη χρήση της. Στα τεστ αυτά περιλαμβάνετ&#= 945;ι ο έλεγχος αντοχής κατά ενδεχόμενης = = θραύσης, τ= ο σωστό της σχήμα αλλά και η μέτρηση της δ= ;ιαφάνειας
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file:///C:/0EC8A292/OptikesInes2.files/slide0020.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" PowerPoint Presentation
Τ&#= 933;ΠΟΙ ΠΗΓΩΝ ΦΩΤΟΣ
§= Led. Τα LED έχουν ένα μη γραμμικό χαρακτήρα. Επιπλέον, δε σχ= ;ετίζονται άμεσα με τη θερμοκρασία = αφού δεν απαιτούν έλεγχο της ενέργειας και της θερμοκρασ&= #943;ας. Ακόμη, είναι πιο αργά και με= ; λιγότερη εκπομπή ενέργειας από τους πομπούς LASER. Το φως που εκπέμπουν είναι ασυνεχές και έχει φάσμ&= #945; πλάτους της τάξης των 60nm. 
§=  Laser Τα LASER είναι δίοδοι ημιαγωγών που εκπέμπουν μια συνεχή δέσμη φωτός με φάσμα= = πλάτους μικρότερο από 10nm. Απαιτούν εξειδικευμέν&#= 959; έλεγχο της θερμοκρασίας και της ενέργειας και χρησιμοποιού&#= 957;ται για ροή σήματος αρκετών Μbit αφο = 73; έχουν μεγάλη ταχύτητα εναλλαγής πολικότη&#= 964;ας. Επιπλέον πάνω από ένα όριο ρεύματος, τα LASER έχουν γραμμικό χαρακτήρα και είναι κατάλληλα για αναλογική μετάδοση.
§=
Δέ = 54;τες
Οι δέκτες λαμβάνουν το σήμα από την οπτική ίνα και το μετατρέπουν σε ηλεκτρικό ρεύμα. Σήμερα = χρησιμοπ&#= 959;ιούνται δυο τύποι φωτοδιόδων ως ανιχνευτές για τη μετατροπή του οπτικού σήματος σε ηλεκτρικ&#= 959;ύ. Οι δίοδοι ΡΙΝ, οι οποίοι είναι λιγότερ&= #959;ι ευαίσθητοι στο φως αποτελούνται από θετικά, αρνητικά και ουδέτερα υλικά τα οποία βρίσκονται σε στερεά κατάσταση. Οι δίοδοι χιονοστιβάδα&#= 962;, ή αλλ= ιώς APD (Avalance Photo Diode) είναι ακριβότεροι από τους ΡΙΝ επειδή παρέχουν μεγαλύτερη ευαισθησ&#= 943;α. Τέλος οι δέκτες ΑPD χρειάζονται εξωτερική τροφοδοσία.
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§=
Έν = 69;ση με τη μέθοδο της σύντηξης
Στη= ν ένωση με σύντηξη, τα δύο άκρα ευθυγραμμίζο&#= 957;ται είτε με τα χέρια χρησιμοποιών&#= 964;ας micro-manipulators και ένα μικροσκόπιο για να βλέπουμε την ίνα, είτε αυτόματα με τη βοήθεια κάμερας ή μετρώντα&#= 962; το φως που φτάνει στο τέλος τις ίνας και προσαρμόζοντ&#= 945;ς τη στοίχιση της ίνας έως ότου πετύχουμε τη μέγιστη απόδοση. Στη συνέχεια τα δύο άκρα ‘λιώνονται’ χρησιμοποιών&#= 964;ας είτε μια φλόγα γκαζιού είτε πιο συνήθες ένα ηλεκτρικό τόξο. Με τη μέθοδο αυτή επιτυγχάνοντ&#= 945;ι σχεδόν τέλειες ενώσεις με απώλειες που κυμαίνονται στα 0.02dB.

3D"Δέκτης
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Σ&= #933;ΓΚΡΙΣΗ ΣΕ LASER ΚΑΙ LED
uLaser
uμεγάλ&= #951; ισχύ εκπομπής.
uΥψηλό ρυθμό μετάδοσης (bit rate).
= uστενή δέσμη φωτός. =
= uταιριάζε&#= 953; σε multimode και σε single mode τύπο οπτικής ίνας.
= uδεν υπόκεινται σε χρωματική διάχυση καθώς είναι σχεδόν μονοχρωματικ&#= 942;
uLED
u χαμηλ= ό κόστος.
u μεγάλ= η διάρκεια ζωής.
u μικρή ευαισθησία σε μεταβολές της θερμοκρασίας
3DFO-KHPOS-PISINA-2.jpg
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Content-Location: file:///C:/0EC8A292/OptikesInes2.files/slide0022.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" PowerPoint Presentation
ΟΦΕΛΗ ΓΙΑ ΤΗΝ ΟΙΚΟΝΟΜΙΑ
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§= ΤΑ ΔΙΚΤΥΑ νέας γενιάς αναπτύσσοντα&#= 953; από πολλές ευρ= ωπαϊκές κυβερ= νήσεις ως απαραίτητη προϋπόθεση για την κάλυψη της μελλοντικής = ζήτησης σ&= #949; χωρητικότητα και προηγμένες τηλεπικοινων&#= 953;ακές υπηρεσίες. Όμως ακολουθούντα&#= 953; διαφορετικά μοντέλα και υπάρχουν πολλές αμφιβολίες για την απόδοση των επενδύσεων <= /span>§Ο = 53; επενδύσεις αυτές έχουν σημαντικό ρόλο να παίξου= ν στο σχέδιο τόνωσης της οικονομίας, δεδομένου ότι θα θέσουν τη βάση για συνεχή αύξηση της π= αραγωγικότητ = 45;ς και της καινοτομίας, ενώ θα έχουν και θετικότατη επίδραση στη μείωση της ανεργίας (εκτιμάται ότι μια επένδυση ύψους 2 δισ. ευρώ θα δημιουργήσει/&= #948;ιατηρήσει άνω των 120.000 θέσε`= 9;ν εργασίας)
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Κ&#= 921;ΝΗΤΟΠΟΙΗΣΗ ΓΙΑ ΤΙΣ ΟΠΤΙΚΕΣ ΙΝΕΣ=
§= Σχεδόν όλες οι ευρωπαϊκές κυβερνήσεις έχουν εξαγγεί&= #955;ει αντίστοιχα σχέδια καθώς τα δίκτυα νέας= γενιάς, πο= υ προσφέρουν ταχύτατη πρόσβαση στο Διαδίκτυο, θεωρούνται κρίσιμα για την α&= #957;ταγωνιστικό`= 4;ητα των οικονομιών και την αύξηση της απασχόλησης.

Όμως, κανένα από τα σχέδια δεν έχει προχωρήσει αρ&= #954;ετά, ώστε να αποτελέσει μπούσουλα για την ε&= #955;ληνική πλευρά. Στη δύσκολη εξίσωση για το έργο των δύο δισ. εμπλέκονται ο ΟΤΕ (από τις αποφάσει&#= 962; του θα εξαρτηθεί η βιωσιμότητα της επένδυσης), οι δήμοι (με τη στάση τους συνδέεται η = ταχεία εγκατάσταση των δικτύων), η κυβέρνηση (απα= ιτούνται θεσμικό πλαίσιο και κίνητρα για την ε= γκατάσταση οπτικών ινών μέσα στα σπίτια έτσι ώσ= τε να απολαμβάνουμ&#= 949; τις υψηλές ταχύτητες) και= οι εγχώριοι ή ξένοι επενδυτές (απαιτείται πλαίσιο διαγωνισμού που θα τους προσελκύει σε μια δ&= #973;σκολη συγκυρία για την ελληνική οικονομία).
§= Οι ειδικο&= #943; που παρακολουθού&#= 957; τις αντίστοιχες ευρωπαϊκές πρωτοβουλίες καταλήγουν σε τρία βασικά = συμπεράσ&#= 956;ατα:
1. Πρέπει να συμμετάσχει στο έργο ο ΟΤΕ.
2. Το έργο πρέπει να υλοποιηθεί με κρατική ενίσχυση και με τη μέθοδο της Σύμπραξης Δημοσίου και = Ιδιωτικο&#= 973; Τομέα (ΣΔΙΤ).
3. Απαιτούνται προσεκτικές νομοθετικές ρυθμίσεις ώστε να επιλυθεί σωρεία προβλημάτων όπως η διέλευση των δικτύων από τους δρόμους, η εγκατάσταση οπτικών ινών στις κατοικίες και η ενίσχυση = του ανταγωνισμού στην αγορά τηλεπικοινων&#= 953;ών.

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ΥΠΟΔΟΜΕΣ ΓΙΑ ΟΠΤΙΚΕΣ ΙΝΕΣ
uο ΟΤΕ ως ιδιωτικών συμφερόντων εταιρεία προφανώς έχει ως στόχο την αύξηση της <= span style=3D'font-size:44%'>κερδοφορ&#= 943;ας του αλλά και τον περιορισμό της ισχύος των ανταγωνιστών του.

Σε περίπτωση λοιπόν που θα προχωρήσει σε ανάπτυξη δικτύου VDSL, αποκτά προφανές πλεονέκτημα έναντι του ανταγωνισμού γιατί: (α) μπορε = 43; να εξυπηρετήσει <= /span>= καλύτερα τους πελάτες του έναντι των ανταγωνιστών του και (β) οδηγεί τους = ανταγωνι&#= 963;τές του ουσιαστικά εκτός της αγοράς, γιατί για να μπορούν αυτοί να τον <= span style=3D'font-size:44%'>ανταγωνι&#= 963;τούν πρέπει να εγκατασταθού&#= 957; με σημεία παρουσίας δίπλα στις καμπίνες <= span style=3D'font-size:44%'>του ΟΤΕ, οπότε πρέπει να πραγματοποιή&#= 963;ουν επιπλέον επενδύσεις, με αμφίβολη = επιτυχία&#= 13;
uΒέβαια, μι= α τέτοια περίπτωση αποτελεί ουσιαστικά πισωγύρισμα για τη χώρα γιατί: (α) αυτή η τεχνολογία (VDSL) δεν μπορεί να καλύψει τις ανάγκες των τελικών πελατών = (λόγω του διπλασιασμού της ζήτησης κάθε δύο χρόνι= α) για πολλά χρόνια, και (β) τ&#= 959; μοντέ&= #955;ο του ανταγωνισμού που έχει ακολουθηθεί ω&= #962; τώρα (αποδεσμοποίη&= #963;η τοπικών βρόχων) οφείλει να εγκαταλειφθε&#= 943; και να χρησιμοποιηθ&#= 949;ί από τους εναλλακτικού&#= 962; αποκλ&= #949;ιστικά και μόνο η υποδομή του ΟΤΕ μέσω χονδρ= ικής ευρυζωνικής πρόσβασης. <= span style=3D'font-size:44%'>Η επένδυσ&= #951; σε VDSL για τον ΟΤΕ ίσως φαίνεται καλή για το εγγύς μέλλον, αλλά  έχει τέτοια μειονεκτήματ&#= 945; που την καθιστούν επένδυση με πολύ κοντινή ημερομηνία <= span style=3D'font-size:44%'>λήξεως=
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Υπερηχητικό&= raquo; Ιντερνετ µε οπτικές ίνες
uΣΕΡΦΑΡΙΣ= ;ΜΑ στο Ιντερνετ µε ταχύτητες τέσσερις έως πέντε φορές υψηλότερ&#= 949;ς σε σχέση µε αυτές που προσφέρουν αυτή τη στιγµή οι πιο γρήγορες ευρυζωνικές συνδέσεις (ADSL)... Μετάδοση τηλε&= #959;πτικών προ= γραµµάτων υψηλής ευκρίνειας (high definit= ion) µέσω ∆ιαδικτύ= ;ου, µε ποιότητα εφάμιλλη του κινηµατογράφ&= #959;υ! Τηλεδιασκέψε&#= 953;ς όπου οι συνοµιλη&= #964;ές θα αισθάνονται ότι βρίσκονται ο ένας δίπλα στον άλλον! 

Αυτ= ό είναι µόνο ένα µικρό δείγµα από τις εφαρµογές που θα π&= #961;οσφέρουν τα νέα... υπερηχητικά τηλεπικοινων&#= 953;ακά δίκτυα, τα οποία αναµένεται σταδιακά να έρθουν και στη χώρα µας και ν^= 5; αποτελέσουν = το επόµεν= ο σηµαντικό βήµα στον χώρο των τηλεπικοι&= #957;ωνιών. Η Ελλ= άδα φιλοδοξεί να γίνει µία από τις πρώτες χώρ= ες της Ευρωπαϊκής Ενωσης µε δίκτυα νέας γενιάς, τα οποία θα εξαπλωθούν σε νοικοκυριά και επιχειρήσεις.&= nbsp;

 =
uΟι οπτικέ&= #962; ίνες προσφέρουν... υπερηχητικές ταχύτητες διακίνησ&#= 951;ς δεδοµένων που φθάνουν µέχρι τα 100 Mbps, έναντι 24 Mbps που θεωρητικά προσφέρει αυτή τη στιγµή= ; – µόνο γι^= 5; τη λήψη δεδοµένων – η υπάρχουσα τεχνολογία ADSL. Αυτό θα έχει ως αποτέλεσµα την παροχή προηγµέν&= #969;ν τηλεπικοινων&#= 953;ακών υπηρεσιών, όπως είναι το πολύ γρήγορο σερφάρισµα στο Ιντερνετ, η τηλε-εργασία, η τηλεϊατρική κ.λπ. Επίσης, συναρπαστική θα είναι η πρόσβαση σε τηλεοπτικά κανάλια υψηλής ευκρίνειας ή ακόµη και σε τηλεοπτικό περιεχόµενο... τριών διαστάσ&= #949;ων (3D).
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document.all("NSPlay").autoStart =3D false; if( sld.filters && sld.filters.revealtrans ) setTimeout( "document.body.start()", sld.filters.revealtrans.duration * = 1000 ); else document.body.start(); } } function MakeSldVis()=20 { var fTrans=3Dg_showAnimation && SldHasTrans() if( fTrans )=09 { if( g_bgSound ) { idx=3Dg_bgSound.indexOf(","); pptSound.src=3Dg_bgSound.substr( 0, idx ); pptSound.loop=3D -(parseInt(g_bgSound.substr(idx+1))); } SlideObj.filters.revealtrans.Apply()=09 } SlideObj.style.visibility=3D"visible" if( fTrans ) SlideObj.filters.revealtrans.Play() } function MakeNotesVis()=20 { if( !IsNts() ) return false=20 SlideObj.style.display=3D"none" nObj =3D document.all.item("NotesObj") parent.SetHasNts(0) if( nObj ) {=20 nObj.style.display=3D"" parent.SetHasNts(1) } return 1 } function ChkAutoAdv() { if(SldHasTrans()) SlideObj.onfilterchange=3DAutoAdv else AutoAdv() } function AutoAdv() { if(!IsWin("PPTSld") || !gUseSldTimings )return var sld=3DGetCurSld() if( (sld.mAdvDelay>0) && !parent.IsFramesMode() ) setTimeout("parent.GoToNextSld()",sld.mAdvDelay) } function GetObj(id) { if(g_supportsPPTHTML) return document.all(id); else return document.getElementById(id); } function SldHasTrans() { return SlideObj.style.filter !=3D ""; } function GetSldId()=20 { var regExp =3D /file:\/\/\//i var pos =3D location.href.search(regExp) if (MHTMLPrefix !=3D "" && pos !=3D -1) sId =3D location.href.substring(pos) else { sId =3D RemoveFilePrefixFromHref(location.href); var regExp =3D /\// var fixedHref =3D sId var pos =3D -1 =09 pos =3D fixedHref.search(regExp) while (pos !=3D -1) { fixedHref =3D fixedHref.replace(regExp, "\\") pos =3D fixedHref.search(regExp) } =09 if (g_fBaseHyperlink =3D=3D true) sId =3D "file:///" + fixedHref; else sId =3D fixedHref.substring(fixedHref.lastIndexOf('\\') + 1) } =09 return sId } function HideMenu() { if( frames["PPTSld"] && PPTSld.document.all.item("ctx= tmenu") && PPTSld.ctxtmenu.style.display!=3D"none" ) { PPTSld.ctxtmenu.styl= e.display=3D'none'; return true } return false } function IsWin( name ) { return window.name =3D=3D name } function IsNts() { return IsWin("PPTNts") } function IsSldOrNts() { return( IsWin("PPTSld")||IsWin("PPTNts") ) } function SupportsPPTAnimation() { return( navigator.platform =3D=3D "Win32"= && navigator.appVersion.indexOf("Windows")>0 ) } function SupportsPPTHTML() { var appVer=3Dnavigator.appVersion, msie=3DappVer.indexOf("MSIE "), ver=3D0 if( msie >=3D 0 ) ver=3DparseFloat( appVer.substring( msie+5, appVer.indexOf(";",msie) ) ) else ver=3DparseInt(appVer) return( ver >=3D 4 && msie >=3D 0 ) } function _RSW() { if( !g_supportsPPTHTML || IsNts() || ( !g_scaleInFrame && (!IsWin("PPTSld") || !parent.IsFullScrMode()) ) ) return var padding=3D0; if( IsWin("PPTSld") && parent.IsFramesMode() ) padding=3D6 cltWidth=3Ddocument.body.clientWidth-padding cltHeight=3Ddocument.body.clientHeight-padding factor=3D(1.0*cltWidth)/g_origW if( cltHeight < g_origH*factor ) factor=3D(1.0*cltHeight)/g_origH newSize =3D g_origSz * factor if( newSize < 1 ) newSize=3D1 s=3DSlideObj.style s.fontSize=3DnewSize+"px" s.posWidth=3Dg_origW*factor s.posHeight=3Dg_origH*factor s.posLeft=3D(cltWidth-s.posWidth+padding)/2 s.posTop=3D(cltHeight-s.posHeight+padding)/2 if( g_scaleHyperlinks ) ScaleHyperlinks( factor ) } function _InitAnimations() { animRuntimeInstalled =3D ''+document.body.localTime !=3D 'undefined'; isFullScreen =3D (window.name =3D=3D "PPTSld") && !parent.IsFramesMode(); g_animUseRuntime =3D g_showAnimation && animRuntimeInstalled && !(isFullSc= reen && parent.IsSldVisited()); if( g_animUseRuntime ) { collSeq =3D document.all.tags("seq"); if( collSeq !=3D null ) { for(ii=3D0;ii numSlds ) gSldJumpIdx =3D numSlds; if ( gSldJumpIdx >=3D 0 ) { if ( gSldJumpIdx =3D=3D 0 ) gSldJumpIdx =3D 1; var jumpTo =3D parseInt(gSldJumpIdx); gSldJump =3D 0; gSldJumpIdx =3D ""; win.GoToSld( parent.GetSldList().mList[jumpTo-1].mSldHref ) } } } function _KDH() { if( event.keyCode =3D=3D 8 ) { event.returnValue =3D 0; parent.GoToPrevSld(); } } function DocumentOnClick() { if( IsNts() || parent.HideMenu() ) return; if( ( g_allowAdvOnClick && !parent.IsFramesMode() ) || (event && (event.keyCode=3D=3D32) ) ) parent.GoToNextSld(); } var g_supportsPPTHTML =3D SupportsPPTHTML(), g_scaleInFrame =3D 1, gId=3D""= , g_bgSound=3D"", g_scaleHyperlinks =3D false, g_allowAdvOnClick =3D 1, g_showInBrowser = =3D 0, gLoopCont =3D 0, gUseSldTimings =3D 1; var g_showAnimation =3D g_supportsPPTHTML && SupportsPPTAnimation() && ( (w= indow.name=3D=3D"PPTSld" && !parent.IsFramesMode()) || g_showInBrowser );va= r g_animManager =3D null; var g_animUseRuntime =3D false; var g_animItemsToHide, g_animInteractiveItems, g_animSlideTime; var g_animMainSequence =3D null; var ENDSHOW_MESG=3D"Τέλος της π= ;ροβολής παρου&= #963;ίασης, κάντε κ&= #955;ικ για έξοδο.", SCRE= EN_MODE=3D"Frames", gIsEndShow=3D0, NUM_VIS_SLDS=3D25, SCRIPT_HREF=3D"scrip= t.js", FULLSCR_HREF=3D"fullscreen.htm"; var gCurSld =3D gPrevSld =3D 1, g_offset =3D 0, gNtsOpen =3D gHasNts =3D gO= tlTxtExp =3D 0, gHasNarration =3D 0, gOtlOpen =3D true window.gPPTHTML=3DSupportsPPTHTML() var g_fBaseHyperlink =3D false; var gMainDoc=3Dnew Array(new hrefList("slide0001.htm",1,-1,1),new hrefList(= "slide0002.htm",1,-1,1),new hrefList("slide0003.htm",1,-1,1),new hrefList("= slide0004.htm",1,-1,1),new hrefList("slide0005.htm",1,-1,1),new hrefList("s= lide0006.htm",1,-1,1),new hrefList("slide0007.htm",1,-1,1),new hrefList("sl= ide0008.htm",1,-1,1),new hrefList("slide0009.htm",1,-1,1),new hrefList("sli= de0010.htm",1,-1,1),new hrefList("slide0011.htm",1,-1,1),new hrefList("slid= e0012.htm",1,-1,1),new hrefList("slide0013.htm",1,-1,1),new hrefList("slide= 0014.htm",1,-1,1),new hrefList("slide0015.htm",1,-1,1),new hrefList("slide0= 016.htm",1,-1,1),new hrefList("slide0017.htm",1,-1,1),new hrefList("slide00= 18.htm",1,-1,1),new hrefList("slide0019.htm",1,-1,1),new hrefList("slide002= 0.htm",1,-1,1),new hrefList("slide0021.htm",1,-1,1),new hrefList("slide0022= .htm",1,-1,1),new hrefList("slide0023.htm",1,-1,1),new hrefList("slide0024.= htm",1,-1,1),new hrefList("slide0025.htm",1,-1,1)); /********************************************* Frameset functions These functions control slide navigation and state of the frameset. **********************************************/ function RemoveFilePrefixFromHref(href) { var regExp =3D /^file:\/\/\//i; return href.replace(regExp, "") } function FullScrInit() { g_allowAdvOnClick =3D GetCurSld().mAdvOnClk document.body.style.backgroundColor=3D"black" document.oncontextmenu=3Dparent._CM; document.onkeydown =3D _KDH; document.ondragstart=3DCancel document.onselectstart=3DCancel self.focus() } function Redirect( frmId ) {=09 var str=3Ddocument.location.hash,idx=3Dstr.indexOf('#'), sId=3DGetSldId() if(idx>=3D0) str=3Dstr.substr(1); if( window.name !=3D frmId && ( sId !=3D str) ) { obj =3D GetObj("Main-File") window.location.href=3Dobj.href+"#"+sId return 1 } return 0 } var MHTMLPrefix =3D CalculateMHTMLPrefix();=20 function CalculateMHTMLPrefix() { if ( document.location.protocol =3D=3D 'mhtml:') {=20 href=3Dnew String(document.location.href)=20 Start=3Dhref.indexOf('!')+1=20 End=3Dhref.lastIndexOf('/')+1=20 if (End < Start)=20 return href.substring(0, Start)=20 else=20 return href.substring(0, End)=20 } return ''; } function GetTags(base,tag) { if(g_supportsPPTHTML) return base.all.tags(tag); else return base.getElementsByTagName(tag); } function UpdNtsPane(){ if(frames["PPTNts"]) PPTNts.location.replace( MHTMLP= refix+GetHrefObj( gCurSld ).mNtsHref ) } function UpdNavPane( sldIndex ){ if(gNavLoaded) PPTNav.UpdNav() } function UpdOtNavPane(){ if(gOtlNavLoaded) PPTOtlNav.UpdOtlNav() } function UpdOtlPane(){ if(gOtlLoaded) PPTOtl.UpdOtl() } function SetHasNts( fVal ) { if( gHasNts !=3D fVal ) { gHasNts=3DfVal UpdNavPane() } } function ToggleOtlText() { gOtlTxtExp=3D!gOtlTxtExp UpdOtlPane() } function ClearMedia() { // Clear any sounds playing before launching another browser window. Other= wise, // in fullscreen mode, you'll continue to hear the sound in the frames mod= e. if (PPTSld.pptSound) PPTSld.pptSound.loop =3D 0; } function FullScreen() {=20 if ( PPTSld.g_animUseRuntime ) PPTSld.document.body.pause(); ClearMedia(); var href =3D ( document.location.protocol =3D=3D 'mhtml:') ? FULLSCR_HREF = : FULLSCR_HREF+"#"+GetHrefObj(gCurSld).mSldHref; if (MHTMLPrefix !=3D "") href =3D RemoveFilePrefixFromHref(href) if(PPTNav.event.ctrlKey) { var w =3D (window.screen.availWidth * 1.0) / 2.0 var h =3D w * (PPTSld.g_origH * 1.0) / PPTSld.g_origW win =3D window.open( MHTMLPrefix+href,null,"toolbar=3D0,resizable=3D1,top= =3D0,left=3D0," + "width=3D"+ w + ",height=3D" + h ); if( win.document.body && PPTSld.g_animUseRuntime ) win.document.body.PPTSldFrameset=3Dwindow; } else { win =3D window.open( MHTMLPrefix+href,null,"fullscreen=3Dyes" ); if( win.document.body && PPTSld.g_animUseRuntime ) win.document.body.PPTSldFrameset=3Dwindow; } } function ToggleVNarration() { rObj=3DPPTSld.document.all("NSPlay") if( rObj && !PPTSld.g_animUseRuntime ) { if( (rObj.playState =3D=3D 1)||(rObj.playState =3D=3D 0) ) rObj.Play() else if( rObj.playState =3D=3D 2 ) rObj.Pause() else return; } else if( PPTSld.g_animUseRuntime ) { narObj =3D PPTSld.document.all("narrationID") if( narObj ) narObj.togglePause() } } function GetCurSldNum() { =20 obj=3DGetHrefObj(gCurSld) if( obj.mOrigVis =3D=3D 1 ) return obj.mSldIdx else =20 return gCurSld } function GetNumSlds() { =20 if( GetHrefObj(gCurSld).mOrigVis =3D=3D 1 ) return GetSldList().mNumVisSlds; else return GetSldList().mList.length } function GetSldNum( href ) { for(ii=3D0; ii 1 ) PopSldList(); else if( !IsFramesMode() ) { if( gLoopCont ) GoToFirst() else EndShow() } } function GoToPrevSld() { ii=3DgCurSld-1 if( ii > 0 ) { obj=3DGetHrefObj(ii) while ( obj && ( obj.mVis =3D=3D 0 ) && ( ii>0 ) ) obj=3DGetHrefObj(--ii) if( ii =3D=3D 0 ) ii=3D1 GoToSldNum(ii) } } function GoToFirst(){ GoToSld( GetHrefObj(1).mSldHref ) } function GoToLast() { ii=3DGetSldList().mList.length if( ii !=3D gCurSld ) GoToSld( GetHrefObj(ii).mSldHref ) } function GoToSldNum( num ) { if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue obj =3D GetHrefObj( num ) obj.mVis=3D1 gPrevSld=3DgCurSld gCurSld =3D num; =09 if (MHTMLPrefix !=3D "") PPTSld.location.replace(MHTMLPrefix+RemoveFilePrefixFromHref(obj.mSldHref= )) else PPTSld.location.replace(obj.mSldHref) =09 if( IsFramesMode() ) { UpdNavPane(); UpdOtlPane(); UpdNtsPane() } } function GoToSld( href ) { if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue GetHrefObj( GetSldNum(href) ).mVis=3D1 if (MHTMLPrefix !=3D "") PPTSld.location.replace(MHTMLPrefix+RemoveFilePrefixFromHref(href)) else PPTSld.location.replace(href) } function SldUpdated( id ) { if( id =3D=3D GetHrefObj(gCurSld).mSldHref ) return gPrevSld=3DgCurSld gCurSld=3DGetSldNum(id) if( IsFramesMode() ) { UpdNavPane(); UpdOtlPane(); UpdNtsPane() } } function PrevSldViewed(){ GoToSld( GetHrefObj(gPrevSld).mSldHref ) } function HasPrevSld() { return ( gIsEndShow || ( gCurSld !=3D 1 && GetHrefO= bj( gCurSld-1 ).mVis =3D=3D 1 )||( GetCurSldNum() > 1 ) ) } function HasNextSld() { return (GetCurSldNum() !=3D GetNumSlds()) } function CloseWindow() { if( HideMenu() ) return; =09 var event =3D PPTSld.event; if( !IsFramesMode() && event && (event.keyCode=3D=3D27 || event.keyCode=3D= =3D32 || event.type=3D=3D"click" ) ) window.close( self ); CatchNumKeys( self, event ); } function Unload() { gIsEndShow=3D0; } function SetupEndShow() { gIsEndShow=3D1; PPTSld.document.body.scroll=3D"no"; PPTSld.document.onkeypress=3DCloseWindow; PPTSld.document.onclick=3DCloseWindow; PPTSld.document.oncontextmenu=3D_CM; } function EndShow() { if( IsFramesMode() ) return if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue doc=3DPPTSld.document var dir =3D doc.body.dir if( dir !=3D "rtl" ) dir =3D "ltr"; doc.open() doc.writeln('


' + ENDSHOW_MESG + '

') doc.close() } function SetSldVisited(){ GetSldList().mList[gCurSld-1].mVisited=3Dtrue } function IsSldVisited(){ return GetSldList().mList[gCurSld-1].mVisited } function hrefList( sldHref, visible, advDelay, advClk ) { this.mSldHref=3D this.mNtsHref =3D sldHref this.mOrigVis=3D this.mVis =3D visible this.mVisited=3D false this.mAdvDelay=3D advDelay this.mAdvOnClk=3D advClk } function SldList(arr,curSld,fEnd) { this.mCurSld =3D curSld; this.mList =3D new Array(); var idx =3D 1; for(ii=3D0;ii 0) { PushSldList(sldList,fEnd); gCurSld =3D 1; } else if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue } function PushSldList(arr,fEnd) { var ii =3D gSldStack.length; gSldStack[ii] =3D new SldList(arr,gCurSld,fEnd); GoToSld( gSldStack[ii].mList[0].mSldHref ); } function PopSldList() { if (gSldStack[gSldStack.length-1].fEndShow) EndShow() else { gCurSld =3D gSldStack[gSldStack.length-1].mCurSld; gSldStack[gSldStack.length-1] =3D null; gSldStack.length--; var sldList =3D gSldStack[gSldStack.length-1]; GoToSld( sldList.mList[gCurSld - 1].mSldHref ); } } var custShowList=3Dnew Array(); /********************************************* Navigation button implementation There are 2 types of buttons: ImgBtn, TxtBtn implemented as function objects. They share a similiar interface so the event handlers can call SetActive, for example, on a button=20 object without needing to know exactly=20 what type of button it is. **********************************************/ //---------------------------------- function ImgBtn( oId,bId,w,action ) //---------------------------------- { var t=3Dthis t.Perform =3D _IBP t.SetActive =3D _IBSetA t.SetInactive=3D _IBSetI t.SetPressed =3D _IBSetP t.SetDisabled=3D _IBSetD t.Enabled =3D _IBSetE t.ChangeIcon =3D null t.UserAction =3D action t.ChgState =3D _IBUI t.mObjId =3D oId t.mBorderId=3D bId t.mWidth =3D w t.mIsOn =3D t.mCurState =3D 0 } function _IBSetA() { if( this.mIsOn ) { obj=3Dthis.ChgState( gHiliteClr,gShadowClr,2 ) obj.style.posTop=3D0 } } function _IBSetI() { if( this.mIsOn ) { obj=3Dthis.ChgState( gFaceClr,gFaceClr,1 ) obj.style.posTop=3D0=20 } } function _IBSetP() { if( this.mIsOn ) { obj=3Dthis.ChgState( gShadowClr,gHiliteClr,2 ) obj.style.posLeft+=3D1; obj.style.posTop+=3D1 } } function _IBSetD() { =20 obj=3Dthis.ChgState( gFaceClr,gFaceClr,0 ) obj.style.posTop=3D0=20 } function _IBSetE( state ) { var t=3Dthis GetObj( t.mBorderId ).style.visibility=3D"visible" if( state !=3D t.mIsOn ) { t.mIsOn=3Dstate if( state ) t.SetInactive() else t.SetDisabled() } } function _IBP() { var t=3Dthis if( t.mIsOn ) { if( t.UserAction !=3D null ) t.UserAction() if( t.ChangeIcon ) { obj=3DGetObj(t.mObjId) if( t.ChangeIcon() ) obj.style.posLeft=3Dobj.style.posLeft+(t.mCurState-4)*t.mWidth else obj.style.posLeft=3Dobj.style.posLeft+(t.mCurState-0)*t.mWidth } t.SetActive() } =20 } function _IBUI( clr1,clr2,nextState ) { var t=3Dthis SetBorder( GetObj( t.mBorderId ),clr1,clr2 ) obj=3DGetObj( t.mObjId ) obj.style.posLeft=3Dobj.style.posLeft+(t.mCurState-nextState)*t.mWidth-obj= .style.posTop t.mCurState=3DnextState return obj } //----------------------------------------- function TxtBtn( oId,oeId,action,chkState ) //----------------------------------------- { var t=3Dthis t.Perform =3D _TBP t.SetActive =3D _TBSetA t.SetInactive=3D _TBSetI t.SetPressed =3D _TBSetP t.SetDisabled=3D _TBSetD t.SetEnabled =3D _TBSetE t.GetState =3D chkState t.UserAction =3D action t.ChgState =3D _TBUI t.mObjId =3D oId t.m_elementsId=3D oeId t.mIsOn =3D 1 } function _TBSetA() { var t=3Dthis if( t.mIsOn && !t.GetState() ) t.ChgState( gHiliteClr,gShadowClr,0,0 ) } function _TBSetI() { var t=3Dthis if( t.mIsOn && !t.GetState() ) t.ChgState( gFaceClr,gFaceClr,0,0 ) } function _TBSetP() { if( this.mIsOn ) this.ChgState( gShadowClr,gHiliteClr,1,1 ) } function _TBSetD() { =20 this.ChgState( gFaceClr,gFaceClr,0,0 ) this.mIsOn =3D 0 } function _TBSetE() { var t=3Dthis if( !t.GetState() ) t.ChgState( gFaceClr,gFaceClr,0,0 ) else t.ChgState( gShadowClr,gHiliteClr,1,1 ) t.mIsOn =3D 1 } function _TBP() { var t=3Dthis if( t.mIsOn ) {=20 if( t.UserAction !=3D null ) t.UserAction() if( !t.GetState ) return if( t.GetState() ) t.SetPressed() else t.SetActive() } =20 } function _TBUI( clr1,clr2,lOffset,tOffset ) { SetBorder( GetObj( this.mObjId ),clr1,clr2 ) Offset( GetObj( this.m_elementsId ),lOffset,tOffset ) } function Offset( obj, top, left ){ obj.style.top=3Dtop; obj.style.left=3Dle= ft } function SetBorder( obj, upperLeft, lowerRight ) { s=3Dobj.style; s.borderStyle =3D "solid" s.borderWidth =3D 1=20 s.borderLeftColor =3D s.borderTopColor =3D upperLeft s.borderBottomColor=3D s.borderRightColor =3D lowerRight } function GetBtnObj(){ return gBtnArr[window.event.srcElement.id] } function BtnOnOver(){ b=3DGetBtnObj(); if( b !=3D null ) b.SetActive() } function BtnOnDown(){ b=3DGetBtnObj(); if( b !=3D null ) b.SetPressed() } function BtnOnOut(){ b=3DGetBtnObj(); if( b !=3D null ) b.SetInactive() } function BtnOnUp() { b=3DGetBtnObj() if( b !=3D null ) b.Perform() else Upd() } function GetNtsState(){ return parent.gNtsOpen } function GetOtlState(){ return parent.gOtlOpen } function GetOtlTxtState(){ return parent.gOtlTxtExp } function NtsBtnSetFlag( fVal ) { s=3Ddocument.all.item( this.m_flagId ).style s.display=3D"none" if( fVal ) s.display=3D"" else s.display=3D"none" } function _BSetA_Border(){ b =3D gBtnArr[this.mObjId]; if( b !=3D null ) b.S= etActive() } function _BSetI_Border(){ b =3D gBtnArr[this.mObjId]; if( b !=3D null ) b.S= etInactive() } function _BSetP_Border(){ b =3D gBtnArr[this.mObjId]; if( b !=3D null ) b.S= etPressed() } function _BSetA_BorderImg() {=20 b =3D gBtnArr[this.mBorderId]=20 if( b !=3D null && this.mIsOn && !b.GetState() ) { obj=3Dthis.ChgState( gHiliteClr,gShadowClr,2 ) obj.style.posTop=3D0 } } function _BSetI_BorderImg() {=20 b =3D gBtnArr[this.mBorderId] if( b !=3D null && this.mIsOn && !b.GetState() ) { obj=3Dthis.ChgState( gFaceClr,gFaceClr,1 ) obj.style.posTop=3D0 } } var gHiliteClr=3D"THREEDHIGHLIGHT",gShadowClr=3D"THREEDSHADOW",gFaceClr=3D"= THREEDFACE" var gBtnArr =3D new Array() gBtnArr["nb_otl"] =3D new TxtBtn( "nb_otl","nb_otlElem",parent.ToggleOtlPan= e,GetOtlState ) gBtnArr["nb_otlElem"] =3D new TxtBtn( "nb_otl","nb_otlElem",parent.ToggleOt= lPane,GetOtlState ) gBtnArr["nb_nts"] =3D new ImgBtn( "nb_nts","nb_ntsBorder",10,parent.ToggleN= tsPane ) gBtnArr["nb_nts"].SetActive =3D _BSetA_BorderImg; gBtnArr["nb_nts"].SetInactive =3D _BSetI_BorderImg; gBtnArr["nb_ntsBorder"] =3D new TxtBtn( "nb_ntsBorder","nb_ntsElem",parent.= ToggleNtsPane,GetNtsState ) gBtnArr["nb_ntsElem"] =3D new TxtBtn( "nb_ntsBorder","nb_ntsElem",parent.To= ggleNtsPane,GetNtsState ) gBtnArr["nb_prevBorder"] =3D gBtnArr["nb_prev"]=3D new ImgBtn( "nb_prev","n= b_prevBorder",30,parent.GoToPrevSld ) gBtnArr["nb_nextBorder"] =3D gBtnArr["nb_next"]=3D new ImgBtn( "nb_next","n= b_nextBorder",30,parent.GoToNextSld ) gBtnArr["nb_sldshw"]=3D new ImgBtn( "nb_sldshw","nb_sldshwBorder",18,parent= .FullScreen ) gBtnArr["nb_sldshwBorder"] =3D new TxtBtn( "nb_sldshw","nb_sldshwBorder",pa= rent.FullScreen,null ) gBtnArr["nb_sldshwBorder"].SetActive =3D _BSetA_Border; gBtnArr["nb_sldshwBorder"].SetInactive =3D _BSetI_Border; gBtnArr["nb_sldshwText"] =3D new TxtBtn( "nb_sldshw","nb_sldshwText",parent= .FullScreen,null ) gBtnArr["nb_sldshwText"].SetActive =3D _BSetA_Border; gBtnArr["nb_sldshwText"].SetInactive =3D _BSetI_Border; gBtnArr["nb_voice"] =3D gBtnArr["nb_voiceBorder"] =3D new ImgBtn( "nb_voice= ","nb_voiceBorder",18,parent.ToggleVNarration ) gBtnArr["nb_otlTxtBorder"] =3D gBtnArr["nb_otlTxt"]=3D new ImgBtn( "nb_otlT= xt","nb_otlTxtBorder",23,parent.ToggleOtlText ) gBtnArr["nb_ntsBorder"].m_flagId=3D "nb_nts" gBtnArr["nb_ntsBorder"].SetFlag =3D NtsBtnSetFlag gBtnArr["nb_otlTxt"].ChangeIcon=3D GetOtlTxtState /********************************************* Context menu implementation _CM() is the function that's hooked up to the oncontextmenu event. Once we're asked to show the menu, we first build it by creating DIVs on-the-fly. Then we position it=20 within the screen area so it doesn't get clipped. Creating the DIVs using createElement() means we don't have to write out any extra HTML into the slide HTML files. **********************************************/ var sNext=3D"Επόμενο",sPrev=3D"Π = 61;οηγούμενο",sEnd=3D"Τ&#= 941;λος προβολής",sF= ont=3D"Arial",sArrow=3D"Βέλος",sFreeform=3D"Ε= λεύθερη σχεδί&#= 945;ση",sRect=3D"Ορθογώνι= ο",sOval=3D"Έλλειψη" function ShowMenu() { BuildMenu(); var doc=3DPPTSld.document.body,x=3DPPTSld.event.clientX+doc.scrollLeft,y= =3DPPTSld.event.clientY+doc.scrollTop m =3D PPTSld.document.all.item("ctxtmenu") m.style.pixelLeft=3Dx if( (x+m.scrollWidth > doc.clientWidth)&&(x-m.scrollWidth > 0) ) m.style.pixelLeft=3Dx-m.scrollWidth m.style.pixelTop=3Dy if( (y+m.scrollHeight > doc.clientHeight)&&(y-m.scrollHeight > 0) ) m.style.pixelTop=3Dy-m.scrollHeight m.style.display=3D"" } function _CM() { if( !parent.IsFullScrMode() ) return; if(!PPTSld.event.ctrlKey) { ShowMenu() return false } else HideMenu() } function BuildMenu() { if( PPTSld.document.all.item("ctxtmenu") ) return var mObj=3DCreateItem( PPTSld.document.body ) mObj.id=3D"ctxtmenu" mObj.style.visibility=3D"hidden" var s=3DmObj.style s.position=3D"absolute" s.cursor=3D"default" s.width=3D"120px" SetCMBorder(mObj,"menu","black") var iObj=3DCreateItem( mObj ) SetCMBorder( iObj, "threedhighlight","threedshadow" ) iObj.style.padding=3D2 CreateMenuItem( iObj,sNext,M_GoNextSld,M_True ) CreateMenuItem( iObj,sPrev,M_GoPrevSld,M_HasPrevSld ) =09 CreateSeparator( iObj ) CreateMenuItem( iObj,sEnd,M_End,M_True ) mObj.style.visibility=3D"visible" } function Cancel() { window.event.cancelBubble=3Dtrue; window.event.returnVa= lue=3Dfalse } function Highlight() { ChangeClr("activecaption","threedhighlight") } function Deselect() { ChangeClr("threedface","menutext") } function Perform() { e=3DPPTSld.event.srcElement if( e.type=3D=3D"menuitem" && e.IsActive() ) e.Action() else PPTSld.event.cancelBubble=3Dtrue } function ChangeClr( bg,clr ) { e=3DPPTSld.event.srcElement if( e.type=3D=3D"menuitem" && e.IsActive() ) { e.style.backgroundColor=3Dbg e.style.color=3Dclr } } function M_HasPrevSld() { return( parent.HasPrevSld() ) } function M_GoNextSld() { if( gIsEndShow ) M_End(); else GoToNextSld() } function M_GoPrevSld() { if( gIsEndShow ) { gIsEndShow=3D0; history.back();= PPTSld.event.cancelBubble=3Dtrue; } else GoToPrevSld() } function M_True() { return true } function M_End() { window.close( self ) } function CreateMenuItem( node,text,action,eval ) { var e=3DCreateItem( node ) e.type=3D"menuitem" e.Action=3Daction e.IsActive=3Deval e.innerHTML=3Dtext if( !e.IsActive() ) e.style.color=3D"threedshadow" e.onclick=3DPerform e.onmouseover=3DHighlight e.onmouseout=3DDeselect s=3De.style; s.fontFamily=3DsFont s.fontSize=3D"9pt" s.paddingLeft=3D2 } function CreateSeparator( node ) { var sObj=3DCreateItem( node ) SetCMBorder(sObj,"menu","menu") var s=3DsObj.style s.borderTopColor=3D"threedshadow" s.borderBottomColor=3D"threedhighlight" s.height=3D1 s.fontSize=3D"0px" } function CreateItem( node ) { var elem=3DPPTSld.document.createElement("DIV") node.insertBefore( elem ) return elem } function SetCMBorder( o,ltClr,rbClr ) { var s=3Do.style s.backgroundColor=3D"menu" s.borderStyle=3D"solid" s.borderWidth=3D1 s.borderColor=3DltClr+" "+rbClr+" "+rbClr+" "+ltClr } ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/fullscreen.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/buttons.gif Content-Transfer-Encoding: base64 Content-Type: image/gif R0lGODlhWAESAPf4AAAAAIAAAACAAICAAAAAgIAAgACAgICAgAQEBISEBASEBISEhAQEhMTExAQE /KTM9Pz8/ERERPz8BAT8/KSkpGRkhMTcxCRkxAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAMDAwP8AAAD/AP//AAAA//8A/wD//////yH5BAEAAPgALAAAAABYARIA QAj/APEJHEiwoMGDCBMqXMiwocOHECNKnEixosWLGCEiQKCRo8YDIEHig2DxAD4LKD1avDDhgUuV GUOGbHBR5QGYFBG4fHAB58EKECJEwCfUYAWPFGAygLCRKQIIUKM6WAohKUGgCikcFWh1INWoYKVS 7SrQ41GbIhGYLAuVQVOoC+IyXUuUAkG1HE3KFDhAwkgJc5/qDZmxsOHDiBMrXsy4sePDGyP7lChT 5MULmDPnlDw5YmW6FTNrfgi0aNGEZPEtbfo2bNTUpYeeRph69dPWrqvCNFuBIGG1A59CYPAVQtwF cw0OxWdTIOiBCQAjaAB17fOFII8voGmRc+eOkilm/z9OvTtnjN4hYk1YoT3H2rnBOphPAB9skgq3 2lcaX/5YnJVt9BloAar12UEIRGCZdQghMABI1Tn32IQUVthYexhmqGGGMBHAgIfEhSiiiATAtOGJ GnYI4ogsEldicAYOGNJGZaml3Y0L3NTZUBz1xlB0PUoUI0jlVWRSVN89xBKSGB1YU1TMoRfVBEle hR9HQs1GEHxQ3RZZbveZthxt/LEmXHyp5XWABSCpaRJwbM13gAACPHVccgJFgF+NEhqUAEkQSCfc ddhVhh5dVTaEAEsTUNlkZUWKN9BNGDE6QU8OrSdbllzpxyVTTrU21Uj3scfhp7nNpyoDaTIEJ3P9 If8J2kbLNYegg9JRBwGhFvbq66+ZUiDssMQWK2yHxiZLrInKNotss8l+B5yBrr5p2UIJvortANoC 6+234IbLla/elRtZjeamh5CC3Sb0YLvixivvYkDFGlZqBNh7r4n6goVvv6/ZlCicN+kL71ALTnpQ dCIZp7CihkLA3UQmoWRBogyxtBPGCTnZncVR1rSTo5nuydC/Eo8kUH+lOoTyyvjoCuZu+PjYIKLD rZybtrM1d10C0QXKEVz48GrQkEeWdFJKlbb0UmEeV0SzyC6RvNB646LWIVjUNeC1zAFb+RDKXksM 9r531bwmpQW9+hQDDsx5pqwDRWBXcFES2hc+gEn/wJGdEEWdE6LoWcoxQweaTNmkhydkKaYMYY2Q p1unbLl/pPKbn3v7EZRvrKvqlja2ONvrtoIw9tn2g32/tQBlhtYkU+MNikZ7QYlPDPuMldpOmuJX nVo5VF3HjI+q89mteX5IDd/fVFClma5kiE4f2XUJhlz09gj2NbTDRifkmu7zXjR++RVJ/lPznuvr QH2iD6S+UewP9Dnon6d2NLwN8n90BB6hC68cFMCHoe+ACASP9c4DowUyEF0OPFcDI0ij/VXPaAKC UfhS95AKGoQ7IBRICI1HwhGaUIQoLGEKT6jCFrLwhSuMoQtlCMMZ2rCGOKShDm+4wxzy8Ic+DGIP B4cIRCKGMCAAOy== ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/frame.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" PowerPoint Presentation ------=_NextPart_01CE0857.EAF86F50 Content-Location: file:///C:/0EC8A292/OptikesInes2.files/outline.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii"
 &#= 931;ημειώσεις
Π = 61;οβολή παρουσίασης
Περίγρα= μμα
= = = = = = = =
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