FLIR T420/T440 タイプ2のマニュアルはこちら（約36M）
Contents
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138. 8 5 8 5 1 40 mm 1 57 8 1 T559879 r AG 13004 13006 ja JP 15 Dit A emcee PN 8 5 Ig LASER RADIATION DO NOT STARE INTO BEAM CLASS 2 LASER PRODUCT WAVELENGTH 635 nm MAX OUTPUT POWER 1 mW THIS PRODUCT COMPLIES WITH 21 CFR 1040 10 AND 1040 11 EXCEPT FOR DEVIATIONS PURSUANT TO LASER NOTICE NO 50 DATED JUNE 24 2007 8 5 3 635 nm 1 mW 2007 6 24 No 50 21 CFR 1040 10 1040 11 T559879 r AG 13004 13006 ja JP 9 1 3 24 3 CI Eq
139. 27 3 um 0 28 3 70 SW 0 05 0 08 9 4 70 LW 0 03 0 06 9 4 100 0 09 100 0 09 4 50 500 0 2 0 3 1 20 0 04 2 50 100 0 04 0 06 1 100 0 05 2 100 0 05 4 20 50 0 06 0 07 1 27 10um 0 04 3 27 3 um 0 09 3 70 SW 0 47 9 70 LW 0 46 9 17 SW 0 83 0 94 5 70 SW 0 61 9 70 LW 0 97 9 70 SW 0 67 9 70 LW 0 95 9 PISZA 100 0 55 2 FAMA
140. FLIR Systems PATENT SPECIFICATION DRAWINGS ATTACHED Inventors PER JOHAN LINDBERG and HANS GUNNER MALMBERG 1 057 624 Date of Application and filing Complete Specification Nov 15 1963 1 057 624 No 45167 63 Complete Specification Published Feb 1 1967 Crown Copyright 1967 Index at acceptance H4 F6H Int Cl H 4 n 3 06 Statement COMPLETE SPECIFICATION Scanning Mechanism We AGA AKTIEBOLAG formerly Svenska Aktiebolaget Gasaccumulator of Liding Sweden a Swedish Company do hereby de clare the invention for which we pray that a 5 patent may be granted to us and the method by which it is to be performed to be par ticularly described in and by the following This invention relates to scanning mechan 10 isms and in particular to such mechanisms whereby electro magnetic radiation is picked up and applied thereby to radiation responsive means from which values measured by the radiation responsive means can be studied 15 It is an object of the present invention to provide an improved scanning mechanism of the character indicated It is a further object of the present inven tion to provide improved scanning mechan 20 ism for continuously and automatically scan ning a field of view for ascertaining the energy levels in such field Tt is a still further object of the present invention to provide a scanning mechanism for
141. FUR 45 1723 RX Bicester tees 45 17 4 45 A A UN 45 45 TSE A 45 Lu 46 46 Si 46 18 1 2 ER OD l iecore nct ibo etai bester endet ERE tomes 46 182 TDs orn a A7 18 3 EDEqUTBEu cent edu icta ut 48 18 3 1 48 18 32 WA AW Cases een ied RRR A8 18 3 3 48 i 3220 em NE MMC E NN ELM 49 ON 49 jo Pe Oc ce gt een eT Cee a Ee ee 49 49 1922 FIR ecc wis asciecctutes scant bemus AA 49 19 9 aR EE I d 49 9 49 iX NE I RN i 50 19 4 2s i ae de era veu ee 50 ee 50 19 4 2 50 5 Nl catenin caee 50 fcm a ee ee 50 1952 RR 50 KN 52 ee 52 AO Em 52 ily Ps WEA eS eS Ex B d Sosa Reate pt beaten a kane e RR AIRE RR 53 2 53 n cee 53 2 54 oe 54 SOE ee 54 Lus piti M
142. 1 kW 34 3 4 2 um 3 hm 3 p 3 A
143. External thermography of buildings 4 Proc of the Society of Photo Optical Instrumentation Engineers vol 110 Industrial and Civil Applications of Infrared Technology June 1977 London 6 Paljak Pettersson 3 Thermography of Buildings Swedish Building Research Institute Stockholm 1972 7 Vicek J Determination of emissivity with imaging radiometers and some emissivities at A 5 um Photogrammetric Engineering and Remote Sensing 8 Kern Evaluation of infrared emission of clouds and ground as measured by weather satellites Defence Documentation Center AD 617 417 9 Ohman Claes Emittansm tningar med AGEMA E Boxa Teknisk rapport AGEMA 1999 AGEMA E Box AGEMA 1999 10 Mattei S Tang Kwor E Emissivity measurements for Nextel Velvet coating 811 21 between 36 C AND 82 C 4 11 Lohrengel amp Todtenhaupt 1996 12 ITC Technical publication 32 13 ITC Technical publication 29 SW 36 2 36 1 T SW 2 5 um LW 8 14 um LLW 6 5 20um 1 2 3 C 4 5 6
144. 0 05 4 22 0 05 4 260 0 07 4 175 225 0 05 0 06 1 130 0 60 1 20 0 77 1 5 200 C 200 0 63 1 n 250 0 08 1 20 0 28 1 n 22 0 28 4 100 0 05 4 100 0 93 4 100 0 93 1 100 0 03 2 200 600 0 02 0 03 1 20 0 07 1 20 0 78 2 RV 27 0 07 4 0 88 1 1100 1300 0 13 0 15 1 50 100 0 02 1 100 0 03 2 27 0 03 4 22 0 015 4 22 0 008 4 50 0 6 0 7 1 27 0 78 80 0 018 1 E 34 0 006 4 5 20 50 0 04 0 06 1 5 100 0 07 2 50 150 0 55 1 70 SW 0 08 9 1559879 r AG 13004 13006 ja JP 105 36 36 1 T SW 2 5um LW 8 14 um LLW 6 5 20 um 1 2
145. 000726344 000859020 001106306 0001 001707738 001707746 001707787 001776519 001954074 002021543 002058180 002249953 1144833 1182246 1182620 1285345 1299699 1325808 1336775 1391114 1402918 1404291 1411581 1415075 1421497 1458284 1678485 1732314 2106017 2381417 3006596 3006597 466540 483782 484155 4889913 5177595 60122153 2 602004011681 5 08 6707044 68657 7034300 7110035 7154093 7157705 7237946 7312822 7332716 7336823 7544944 7667198 7809258 B2 7826736 8 018 649 B2 8 153 971 8212210 B2 8289372 8354639 B2 8384783 8520970 8565547 D540838 D549758 D579475 D584755 D599 392 D615 113 D664 580 D664 581 D665 004 D665 440 DI6702302 9 DI690361 7 9 DI7002221 6 DI7002891 5 DI7002892 3 DI7005799 0 DM 057692 DM 061609 EP 2115696 B1 EP2315433 SE 0700240 5 US 8340414 B2 ZL01823221 3 ZL01823226 4 ZL02331553 9 ZL02331554 7 ZL200480034894 0 ZL200530120994 2 ZL200610088759 5 ZL200630130114 4 ZL200730151141 4 ZL200730339504 7 ZL200820105768 8 ZL200830128581 2 ZL200880105236 4 ZL200880105769 2 ZL200930190061 9 ZL201030176127 1 ZL201030176130 3 ZL201030176157 2 ZL201030595931 3 ZL201130442354 9 ZL201230471744 3 ZL201230620731 8 1 8 EULA Terms You have acquired a device INFRARED CAMERA that includes software licensed by FLIR Systems AB from Microsoft Licensing GP or its affiliates MS Those installed software products of MS origin as well as associated
146. 25 rapid scanning of a field A still further object of the present in vention is to provide a scanning mechanism whereby for continuous scanning the retrace time is a relatively small value 30 According to the present invention there is provided a scanning mechanism for receiving electromagnetic radiation within the optical infra red or ultra violet regions of the electro magnetic spectrum which includes a refracting 35 prism adapted to be rotated about its longi tudinal axis the end faces of the prism being polygons each of which polygon has an even number of sides of which opposite sides are parallel a collecting refractive system having 40 an image surface within the prism the axis of which system intersects the longitudinal axis of the prism an aperture situated substanti Pr ally on the axis of the collecting refractive system through which radiation passing through the prism can pass and a radiation responsive element behind said aperture for picking up such radiation Other objects and features of the present invention will be apparent from the following description given by way of example only and with reference to the accompanying dia grammatic drawings in which Fig 1 is a side view of a scanning prism and illustrates the deflection of rays of electro magnetic radiation by the prism and the focus sing of the rays at a fixed scanning aperture Fig 2 graphically illustrates the scanning deflection
147. 9 2 1 2 3 4 5 6 7 8 9 10 11 T559879 r AG 13004 13006 ja JP 10 10 2 2 2 T559879 r AG 13004 13006 ja JP 18 11 Bluetooth
148. EGR 7 20 0 06 1 AR 100 0 03 2 LEES 200 0 03 1 LEES 100 0 61 2 LES 70 SW 0 04 0 09 9 LES 70 LW 0 03 0 07 9 0 3 0 4 1 B 20 0 8 0 9 1 0 60 1 20 0 90 2 19 LLW 0 935 8 19 LLW 0 909 8 20 0 92 1 0 70 0 75 1 70 0 91 1 4 70 SW 0 68 0 74 9 4 70 LW 0 92 0 94 9 El 20 0 7 0 9 1 3 70 SW 0 76 0 78 9 3 70 LW 0 88 0 90 9 20 0 93 2 zd 0 85 1 0 76 1 0 84 1 0 72 1 E 0 90 1 0 94 1 70 SW 0 86 9 70 LW 0 89 9 0 93 1 70 SW 0 77 9 70 LW 0 89 9 70 SW 0 75 9 70 LW 0 88 9 20 SW 0 85 6 20 SW 0 85 6 21 LLW 0 879 8 70 SW 0 95 0 97 9 4 70 LW 0 77 0 87 9 4 T559879 r AG 13004 13006 ja
149. T Wien DRA Wilhelm Wien 1864 1928 Amx Amx 3 000 T um 11 000 kK 0 27 um T559879 r AG 13004 13006 ja JP 87 34 34 5 Wilhelm Wien 1864 1928 49 6 000 K 0 5 hm 300 K 9 7 um EE 77 K 38 um 104 10 10 B 34 6 100 K 1000 K
150. iPhone iPad e WLAN 12 2 1 9 Wi Fi IRCAMxxxx WEP WEPI
151. 1 FLIR Systems 30 2 FLIR Systems Infrared Training Center ITC ITC
152. 13006 ja JP 60 27 27 1 27 1 1 27 1 1 1 49 mm 1 93 96 9 mm 3 81 max minfocus 22 8 mm 0 90 max minfocus ht e d WUJ Optical axis 106 mm 4 17 fo 169 mm 6 65 32 mm 1 26 27 1 0 27 1 2 1 201 mm 7 91 oo e E E LO CD 125 mm 4 92 1559879 r AG 13004 13006 ja JP 61 27 27 1 3 27 1 3 1 Optical axis 35 mm 39 mm 106 mm 4 17 CN o E E LO ei rT 90 4 mm 3 56 27 1 4 30 mm 15 27 1 4 1 121 07 mm 4 77 125 mm 4 92 27 1 5 _ 10 mm 45 27 1 5 1 135 19 mm 5 32 125 mm 4 92 T559879 r AG 13004 13006 ja JP 62 27 27 2 27 2 1 26 2 mm 1 03 91 8 mm 3 61 41 3 mm 1 63 T559879 r AG 13004 13006 ja JP 63 27 27 3 27 3 1 80 2 mm 3 16 46 5 mm 1 83 97 8 mm 3 85 NN n
153. 21 on EE C TRAE ENERO ECCE 21 13 1 2 21 13 1 3 21 13 1 4 P E E E E E TA E E E a 22 13 2 i LINE c Dus 22 19 091 SEMBRA den I CIIM M EMI MM AL 22 19 9 La 23 uu M2 e i ERN 23 194 IX Qa d AZT A erede ed Valete e wen en d er bred 24 135 24 RS NS 24 OO 24 13 6 24 988 NR 24 13 7 BMA ERYN To es ER e oe detras 24 A 25 13 8 3B OD ZRAMRL IL AAW IAG eem 26 TOBA NB ere aae aa a Eate aa oaea iE 26 159 E e D RED OL s tera bi m E AE 28 MR ETE 28 1310 29 29 0 KEN 29 13 11
154. 97 2 17 SW 0 86 5 20 SW 0 90 6 20 0 91 2 25t 0H8IE 20 0 95 2 20 400 0 95 0 97 1 0 96 1 20 0 98 2 0 97 1 37 SW 0 60 7 100 0 05 4 1000 1500 0 14 0 18 1 1094 0 18 4 17 0 016 4 22 0 03 4 260 0 06 4 538 0 10 4 900 1100 0 12 0 17 1 ie He 200 600 0 05 0 10 1 1400 0 18 1 50 200 0 06 0 07 1 500 1000 0 10 0 16 1 32 0 98 2 0 75 0 80 1 1559879 r AG 13004 13006 ja JP 102 36 36 1 T SW 2 5 um LW 8 14 um LLW 6 5 20 um 1 2 3 C 4 5 6 ME 1 2 3 4 5 6 EIS 600 C 200 600 0 59 0 61 1 LEES 80 20 0 20 2 LES 20 350 0 22 1 LES m 20 0 2 1
155. Certain Damages EXCEPT AS PROHIBITED BY LAW MS SHALL HAVE NO LIABILITY FOR ANY INDIRECT SPECIAL CONSEQUENTIAL OR INCIDENTAL DAMAGES ARISING FROM OR IN CONNECTION WITH THE USE OR PERFORMANCE OF THE SOFTWARE THIS LIMITATION SHALL APPLY EVEN IF ANY REMEDY FAILS OF ITS ESSENTIAL PURPOSE IN NO EVENT SHALL MS BE LIABLE FOR ANY AMOUNT IN EXCESS OF U S TWO HUNDRED FIFTY DOLLARS U S 250 00 Limitations on Reverse Engineering Decompilation and Disassembly You may not reverse engineer decompile or disassemble the SOFTWARE except and only to the extent that such activity is expressly permitted by applicable law notwithstanding this limitation e SOFTWARE TRANSFER ALLOWED BUT WITH RESTRICTIONS You may permanently transfer rights under this EULA only as part of a permanent sale or transfer of the Device and only if the recipient agrees to this EULA If the SOFTWARE is an upgrade any transfer must also include all prior versions of the SOFTWARE EXPORT RESTRICTIONS You acknowledge that SOFTWARE is subject to U S export jurisdiction You agree to comply with all applicable international and national laws that apply to the SOFTWARE including the U S Export Administration Regulations as well as end user end use and destination restrictions issued by U S and other governments For additional information see http www microsoft com exporting 1 9 EULATerms Qt4 Core and Qt4 GUI Copyright 2013 Nokia Corporation and FLIR System
156. JP 103 36 36 1 T SW 2 5um LW 8 14 um LLW 6 5 20 um 1 2 3 C 4 5 6 20 LLW 0 849 8 0 46 1 0 16 1 1000 1250 0 75 0 86 1 500 650 0 52 0 59 1 0 70 1 200 600 0 02 0 03 1 100 0 02 2 130 0 018 1 600 C 200 600 0 64 0 78 1 1000 0 95 1 900 1100 0 87 0 95 1 800 1000 0 60 0 70 1 1300 0 28 1 200 0 21 1 38 0 21 4 40 0 21 2 100 0 64 2 260 0 66 4 38 0 63 4 538 0 76 4 50 0 81 1 50 0 95 0 98 1 BR 150 0 16 1
157. T ERN 55 1 55 23 1 1 55 23 150 AAT AA Aa Eo 55 934 9 7 TAD 2 45 BIB AEZIS D S sese dettes suf E ue a E E 55 LC EP DE ari uo ETE 55 OB CNET ded E 55 ON CR RC 56 T559879 r AG 13004 13006 ja JP 24 25 26 27 28 29 30 PN Fe Oe eM EE 57 58 25 1 USB Mini B DRI SREY BRL cece 58 2505 ETA ATZ AOE 8 B ceceneses cento A 58 253 USBA DR740E 2f B cesta eee aed 59 DSA WDR USUE B Cu oio eh ecd 1 59 60 p b lem C ik 61 r MEM i PPP 61 ord SIX ane Ds Ee tet ubt deuten Li ia 61 272 23902 0 SEO Mee Yee cede desiit a a 61 271 3 AFOS A Bot eb iei eb acte Sere ue ER td eie 62 27 1 4 30 mm 15 62 27 1 5 10 mm 45 62 DT INT S a a E 63 DT OA WEN EE RT 63 273 AAISEP OSI Io UO d NE ER ceste eee 64 yc ETUR 64 274 65 DPA E NR RECHERCHE 65 27 5 COMIS rte tastes iste uet ue LORI deu a un ee 65 DT SIAN E E E EA santas sonora E AA EE E 65 27 6 10 mm 45 66 2 66 DISD DPN Lm ME X
158. T559879 r AG 13004 13006 ja JP 82 33 Herschel 75 E Herschel Herschel Herschel Melloni NaCl
159. USB A 5 V USB USB 25 4 RIMIS 1 12V 2 GND 3 GND 1559879 r AG 13004 13006 ja JP 59 26 October 15 2012 AQ125912 CE Declaration of Conformity This is to certify that the System listed below have been designed and manufactured to meet the requirements as applicable of the following EU Directives and corresponding harmonising standards The systems consequently meet the requirements for the CE mark Directives Directive 2004 108 EC Directive 2006 95 EC Directive 1999 5 EC Directive 2002 96 EC Standards Emission Immunity Safety Power Supply System FLIR Systems AB ality Assurance Oud UVN Svensson or Electromagnetic Compatibility Low voltage Directive Power Supply R amp TTE on radio equipment and telecommunications terminal equipment Waste electrical and electronic equipment WEEE As applicable EN 61000 6 3 Electro magnetic Compatibility Generic standards Emission EN 61000 6 2 Electro magnetic Compatibility Generic standards Immunity EN 60950 or other Safety of information technology equipment EN 301489 FLIR T4XX series FLIR Systems AB Antennv gen 6 P O Box 7376 SE 187 15 T by Sweden Telephone 46 8 753 25 00 Telefax 46 8 753 23 64 Registered No 556256 6579 www flir se 1559879 r AG 13004
160. de non responsabilit Fontos megjegyz s Az eszk z haszn lata el tt figyelmesen olvassa el s tartsa be az sszes utas t st figyelmeztet st vint zked st s jogi nyilatkozatot Nota importante Prima di utilizzare il dispositivo importante leggere capire e seguire tutte le istruzioni avvertenze precauzioni ed esclusioni di responsabilit legali Ser su AS FAE t amp 59H7 Ml HOA CSO AES SSMS Sa FIA S HY AAAS Ma 0 ekok BELICE Viktig For du bruker enheten ma du lese forsta og felge instruksjoner advarsler og informasjon om ansvarsfraskrivelse Belangrijke opmerking Zorg ervoor dat u voordat u het apparaat gaat gebruiken alle instructies waarschuwingen en juridische informatie hebt doorgelezen en begrepen en dat u deze opvolgt en in acht neemt Wazna uwaga Przed rozpoczeciem korzystania z urzadzenia nalezy koniecznie zapoznac sie z wszystkimi instrukcjami ostrzezeniami przestrogami i uwagami prawnymi Nale y zawsze post powa zgodnie z zaleceniami tam zawartymi Nota importante Antes de utilizar o dispositivo dever proceder leitura e compreens o de todos os avisos precau es instru es e isen es de responsabilidade legal e assegurar se do seu cumprimento BantHoe npHMMedaHMe 1o Toro Kak NOMb3OBaTbCA VCTDOMCTBOM BAM HEOOXOAMMO NpouuTaTb M nOHRTb BCe npeaynperkAeHWHHR npenocrepexieHMsa n IODMIMH6GCRKMG orpaHuudeHun OTBGTCTBGHHOCTM M Cn
161. view many times per second exceeding the frame frequency of ordinary motion pic tures Referring to the drawings the arrangement according to our invention is characterized by an image surface gen erated inside the circumscribed circle of said prism by a collecting optics 9 in FIGURE 4 Said prism is in our invention of the form of a plane parallel refractive prism which is in one case 1 shown in FIG 1 Said 10 20 30 40 60 70 2 prism has in our invention an even number of sides and is rotated about an axis 2 as indicated by the arrow in FIG 4 that is perpendicular to the paper in FIG 1 The said collecting optics has an optical axis 4 that in tersects said rotating axis 2 and is perpendicular thereto The image surface 5 generated by said collecting optical System is situated inside said prism Just outside the circle 3 generated by said rotating prism and on the Optical axis 4 a scanning aperture 6 is located through Which a radiation passes to the radiation energy respon sive element 12 such as a photocell bolometer or the like depending upon the energy spectrum of interest When said prism rotates the scanning aperture 6 scans a line on said image surface 5 and when a corner of said prism passes the scanning aperture 6 there is a substan tially instantaneous return of the scan In FIGS 1 and 4 there is shown an incoming ray of radiation having a maximum deviation from the di rection of the optical ax
162. 004 13006 ja JP 24 13 13 7 1 1 2 30 E c SH TS ee 3 T559879 r AG 13004 13006 ja JP 25 13 5 6 30 13 8 E 28 2 67 73 8 7 1
163. 13 4 538 0 18 4 20 0 07 2 0 86 1 gt 1500 2200 0 19 0 26 1 600 1000 0 08 0 13 1 700 2500 0 1 0 3 1 17 SW 0 87 5 36 SW 0 94 7 17 SW 0 68 5 95 1230 0 66 1 SiO 1559879 r AG 13004 13006 ja JP 99 36 36 1 T SW 2 5um LW 8 14 um LLW 6 5 20um 1 2 3 C 4 55 6 1 2 3 4 5 6 1500 0 29 1 3396 SiO 64 Al203 1000 0 80 1 1100 0 85 1 1000 0 66 1 17 SW 0 86 0 81 5 35 SW 0 94 7 20 0 94 1 17 SW 0 87 5 500 1000 0 65 0 75 1 1000 0 46 1
164. 2163 2014 03 06 T505470 xml ja JP 12154 2014 03 06 T505012 xml ja JP 12154 2014 03 06 T505007 xml ja JP 12154 2014 03 06 T505004 xml ja JP 12154 2014 03 06 T505000 xml ja JP 12154 2014 03 06 T505005 xml ja JP 12154 2014 03 06 1505001 xml ja JP 12154 2014 03 06 T505006 xml ja JP 12154 2014 03 06 T505002 xml ja JP 12154 2014 03 06 1559879 r AG 13004 13006 ja JP 108 FLIR Corporate Headquarters FLIR Systems Inc 27700 SW Parkway Ave Wilsonville OR 97070 USA Telephone 1 503 498 3547 Website http www flir com Customer support http support flir com Copyright 2014 FLIR Systems Inc All rights reserved worldwide Disclaimer Specifications subject to change without further notice Models and accessories subject to regional market considerations License procedures may apply Products described herein may be subject to US Export Regulations Please refer to exportquestions flir com with any questions Publ No 1559879 Release AG Commit 13004 Head 13006 Language ja JP Modified 2014 04 03 Formatted 2014 04 03
165. 4 1887 T559879 r AG 13004 13006 ja JP 85 34 34 2 Gustav Robert Kirchhoff 1824 1887
166. 98 SCANNING MECHANISM FOR ELECTRO MAGNETIC RADIATION Per Johan Lindberg Stockholm and Hans Gunnar Malm berg Solna Sweden assignors to AGA Aktiebolaget a corporation of Sweden Filed May 14 1962 Ser No 194 622 Claims priority application Belen May 19 1961 299 2 Claims Cl 88 1 This invention relates to an improved optical scanning mechanism for receiving electromagnetic radiation and to radiation responsive means utilizing such optical scan ning It is an object of the invention to provide improved op tical scanning means of the character indicated It is another object of the invention to provide im proved means for continuously and automatically scan ning of a field of view for ascertaining energy levels in such field It is a further object of the invention to provide means for optical scanning of said field of view many times per second A further specific object is to provide means for more accurate and efficient scanning of a field of view the dead or nonutilized scanning time being reduced to a small value Other objects and various further features of novelty and invention will be pointed out or will occur to those skilled in the art from a reading of the following specifica tion in conjunction with the accompanying drawings Said drawings show the principle of the invention FIG 1 is a side view of a scanning prism showing the deflected rays in said prism and the necessary image sur face
167. ATTY LA 700 0 70 1 A27 0 100 0 97 0 93 1 1400 1800 0 69 0 67 1 200 500 0 89 0 78 1 600 1200 0 76 0 70 1 17 SW 0 94 5 1500 2200 0 24 0 31 1 200 0 05 1 600 1000 0 1 0 16 1 3300 0 39 1 0 79 0 84 1 20 0 91 0 93 1 540 C 1000 0 60 1 540 C 200 0 40 1 540 C 500 0 50 1 TO 1000 0 36 1 200 0 15 1 500 0 20 1 700 0 25 1 700 0 70 1 50 0 65 1 500 1000 0 71 0 79 1 50 500 0 95 0 98 1 600 C 200 600 0 37 0 48 1 100 0 045 1 T559879 r AG 13004 13006 ja JP 98 36 1 T SW 2 5um LW 8 14 um LLW 6 5 20 um 1 2 3 C 4 55 6
168. E 20 0 60 1 20 0 9 1 20 0 85 0 95 1 0 89 1 80 0 85 1 50 0 10 1 500 1000 0 28 0 38 1 T559879 r AG 13004 13006 ja JP 97 36 36 1 T SW 2 5um LW 8 14 um LLW 6 5 20 um 1 2 3 C 4 5 6 ME 1 2 3 4 5 6 20 0 92 2 17 SW 0 97 5 36 SW 0 95 7 5 LLW 0 974 8 20 0 95 1 20 0 95 1 10 90 0 91 1 ATLLAS 70 SW 0 30 9 amp ATYLAG 70 LW 0 28 9 ATLLAS 70 SW 0 18 9 70 LW 0 14 18 8 60 0 85 800 C 18 8 20 0 16 2 8 500 0 35 1 JL 18 ATLLAS 700 0 45 1
169. FLIR FLIR T4xx series Important note Before operating the device you must read understand and follow all instructions warnings cautions and legal disclaimers D lezit pozn mka Pred pou it m za zen si p e t te ve ker pokyny upozorn n varov n a vyv z n se ze z ruky ujist te se Ze jim rozum te a i te se jimi Vigtig meddelelse F r du betjener enheden skal du du l se forst og f lge alle anvisninger advarsler sikkerhedsforanstaltninger og ansvarsfraskrivelser Wichtiger Hinweis Bevor Sie das Ger t in Betrieb nehmen lesen verstehen und befolgen Sie unbedingt alle Anweisungen Warnungen Vorsichtshinweise und Haftungsausschl sse 2npavitkr onpeiwon Mp ard rr stroupyia TNS OUOKEUT G TIPETIEL va SLABGOETE va karavorjoere kat va AKOAOUVO OETE OAEC TIC OOT YIEG TIDOELSOTIOINOELC TIPOMUAGEEIC Kat VOUIKEG ATIOTIOINOELC Nota importante Antes de usar el dispositivo debe leer comprender y seguir toda la informacion sobre instrucciones advertencias precauciones y renuncias de responsabilidad Tarkea huomautus Ennen laitteen k ytt mist on luettava ja ymm rrett v kaikki ohjeet vakavat varoitukset varoitukset ja lakitiedotteet sek noudatettava niit Remarque importante Avant d utiliser l appareil vous devez lire comprendre et suivre l ensemble des instructions avertissements mises en garde et clauses l gales
170. R T559879 r AG 13004 13006 ja JP 77 32 AURI XE 3c 007 32 1 32 2
171. as a function of the angle of rota tion for various refractive indices of the prism Fig 3 is a view showing the paraxial image surface for rays in two perpendicular planes for different indices of refraction of the prism The scanning mechanism of the present in vention is particularly applicable to receiving electromagnetic radiation within the optical ultra violet or infra red regions of the electro magnetic spectrum the incoming radiation being focused on a radiation responsive cle ment which may be of a kind well known in the art and as such is not shown in the drawings Hitherto the main difficulty in achieving high scanning speeds has been of a mech anical nature The present invention uses a rotating refractive prism for fast scanning in one direction scanning perpendicular to this direction is slower and can be accomplished by other means for example as by an oscil lating mirror in the collecting optics This slower scanning can also be accomplished by tilting the rotating axis of the prism This BJ 30 1 1960 45 50 55 60 65 70 75 80 United States Patent Office 3 253 498 Patented May 31 1966 1 3 253 4
172. e 35 A FIR TEL 36 14 11 i 36 14 11 1 TUE TITRE 36 AAT eee ene a ae ee ls esed eT ere i Die 36 14 12 PDF LL 36 36 14 19 0 ap 36 5 BL ceci ceteri tr Eee dee ei as eu oc uid DAL 36 imc E 36 15 uj emma iSo rcu 37 TU 37 15 9 BROA eh aarti SN rro a S Nt 37 15 3 BEE 0098 IL as e e eee d e S a e c E reu Deben 38 16 MO 5809Be ocv ceP Pr oePReH ES 39 TO 39 162 Bog Jb05B JB ER uc a i 39 163 39 OA Ei 39 ON EOE 39 164 40 TOAT i NR Nc 40 40 165 AT EOIN oe Oc ht ter a eae hse Bad Serratia 41 EE 41 16 5 2 41 165 ER EN M US 41 BSA FIE MM 41 16 5 5 B ENE uu ee CR ai Me P EE 42 16 6 42 Tox rt bel pue d p E Pa Ec 42 16 6 2 FEB ettet 42 16 7 MEFZG LARED aet tui e E 43 1 43 16 7 2 FV GHD OMB issue icr citra vd pe debat cuu 43 vA NATI 43 ULM MI 43 1559879 r AG 13004 13006 ja JP IX 17 18 19 20 21 22 23 168 44 LS 44 jc feci C PNMCRM HK 44 FLIR Le 45 45 17 2
173. enoBaTb MM Viktig information Innan du anvander enheten m ste du l sa f rst och f lja alla anvisningar varningar forsiktighetsatgarder och ansvarsfriskrivningar Onemli not Cihaz al t rmadan nce tum talimatlar uyar lar ikazlar ve yasal a klamalar okumal anlamal ve bunlara uymalisiniz SEREZ ABANA DEXONMENARSE WH CESOQNDLERK FLIR T4xx series 0 9001 29 PNS AmA A Jj V RTAS TM Ce Intertek 1559879 r AG 13004 13006 ja JP 10 11 1 1 1 hag ERN 1 1 2 1 1 3 Hei 90 DUIIBSR 4 ace ero eroe ee oes t auus 1 1 4 i 1 1 5 See ee Neat Ni C EDT 1 1 6 1 1 7 Ei det uU LE IA M ee EEST 1 1 8 E UEAN e iiam curiae um iu peii IA MARE AIL LE 1 1 9 EUELA TONNS sees sese ent ct 6t cent 6 oe see En delta aia e E tM d crc aes 1 zucc WC T U m 2 EES REA Da D PN TEE TTE T TT 6 3 1 ure UE Vr cR 6 3 2 PUJOLS p EE 6 3 3 D T 6 3 4 aaO END ub 6 3 5 nbl umbo Ni 6 3 6 6 3 7
174. for proper focussing at the fixed scanning aperture FIG 2 is a diagram which shows the scanning deflec tion as a function of the rotating angle of the prism for various indices of refraction of said prism FIG 3 is a view showing said paraxial image surface for rays in two mutually perpendicular planes for different indices of refraction of said prism FIG 4 is a side view showing the essential components of a complete scanning mechanism and FIG 5 is a perspective view of a particular form of a scanning prism Briefly stated our invention is in the following specifica tion characterized as an arrangement for scanning a field of view where the incoming radiation is focused on a radiation energy responsive element The main difficulty of scanning a field of view in a short time is of mechanical nature Our invention uses a rotating refractive prism for scanning in one direction Scanning in a direction essentially perpendicular to said direction is slower than in the first mentioned direction and is accomplished by other means as by a nodding mir ror in the collecting optics Said slower scanning can also be accomplished by tilting the rotating axis of said prism The resulting scanning pattern is like the pattern of common television Said prism can be rotated very rapidly according to our invention and several thousands of scans per second can be accomplished In this way our invention allows com plete scanning of said field of
175. is In FIG 1 w designates the angle of rotation of the prism and x y and z are the axes of a coordinate system x being along the optical axis and z parallel to the axis of rotation 2 A point on the image surface 5 is defined by these coordinates as in dicated in the case of a point x y in FIG 1 the z co ordinate of which is 0 since it is in the x y plane The deflection of rays is shown in FIG 2 in the y di rection as a function of the turning angle o and index of refraction of said prism n The axis y in FIG 3 refers to the same axis as in FIG 2 FIG 3 shows the necessary form 7 and 8 of the image surfaces of said optical system in order that said field of view shall be scanned without aberrations for various values of refractive index of said prism Refer ring to FIG 3 there are for every rotating angle o and every refractive index of said prism n two values of x The larger of said two values of x corresponds to the image surface 7 that is generated by the rays in the plane of the paper i e the x y plane and forming small angles with the x axis The smaller value of x corre sponds to the image surface 8 that is generated by the rays which are parallel with the x z plane and form small angles with the x y plane It is apparent from FIG 3 that the aberrations which are caused by the prism can be neutralized to a sub stantial degree by a suitable choice of image surface In this way it is possible according to ou
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177. r invention to achieve very high resolution in the optical scanning lt is preferable if the refractive index of said prism has a value between 3 and 6 for the wave lengths used Said index of refraction having a value of about 4 is specially advantageous both for yielding a linear scan and for allowing a relatively plane image surface This is pointed out in FIG 2 and FIG 3 As is also shown in FIG 2 a larger index of refraction of said prism gives a greater length of scan The material of said prism must in our invention be transparent for radiation in the energy spectrum of in terest and it is preferable if the sides of said prism are coated with suitable material in order to reduce reflec tions The entry area of the rays coming from said optical System for varying turning angles o does not extend near the corners of the prism in our invention which may therefore be rounded This improves both the air resist ance and the mechanical strength of the prism When said prism rotates and the scanning in the other direction is accomplished in said collecting optics the radiation energy responsive element 12 scans said field of view for various energy levels in such field The out put signals from said element are amplified and filtered and may be used to modulate the intensity of a moving spot on a cathode ray tube The movement of said 258 000
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179. s AB This Qt library is a free software you can redistribute it and or modify it under the terms of the GNU Lesser General Public License as published by the Free Software Foundation either version 2 1 of the License or at your option any later version This library is distributed in the hope that it will be useful but WITHOUT ANY WARRANTY without even the implied warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE See the GNU Lesser General Public License http www gnu org licenses Igpl 2 1 html The source code for the libraries Qt4 Core and Qt4 GUI may be requested from FLIR Systems AB 1559879 r AG 13004 13006 ja JP Dat H B FCC FCC 15 B
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