【US20190346749A1】STOPMODULEANDCAMERAMODULEINCLUDIN
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Faraday Discuss .,1997,108,469È471Concluding RemarksR.M.Hochstrasser a and J.P.Simons ba Department of Chemistry ,University of Pennsylvania ,Philadelphia ,PA 19104,USAb Physical and T heoretical Chemistry L aboratory ,University of Oxford ,Oxford ,UK OX13QZThere are several Golden Rules associated with the presentation of Concluding Remarks at Faraday Discussions.The Ðrst of these,“ask someone else to give themÏhas,sadly,been obeyed because of Prof.HochstrasserÏs enforced immobility,occasioned by a prol-apsed disc.We wish him a speedy recovery.The second Rule,“if you have nothing to say,say nothingÏhas been compensated,fortunately,by Prof.HochstrasserÏs provision of the outline notes of some of the remarks he would have made,had it been possible.They are presented below.The third Rule,“say some nice thingsÏis the easiest of all to obey since Prof.Whitehead has organised so imaginative and timely a Discussion,which has been introduced with all of Prof.JortnerÏs customary dynamism.It has addressed many issues.How do we monitor and interpret the dynamics of photon-induced processes in clusters and condensed media?What is the nature of the chromophore when it is no longer isolated in the gas phase?How does it “communicateÏwith its environment?How does the environment inÑuence electronic motions,e .g .in atomic or molecular Rydberg states;or nuclear motions,e .g .through caging or chap-eroning of atomic or molecular fragments;or their coupling,through non-adiabatic dynamics?How does photon absorption lead to nuclear motion in the neighbouring environment?How do the interactions of the chromophore with the environment depend upon the nature of the environment,and the way it is coupled to it,e .g .through space or through bonds?What are the characteristic timescales of the interactions;are they separable?Can we trace the pathway from the initial energy localisation,through its delocalisation to its eventual dissipation?What is the nature of the “molecular and intermolecular circuitryÏthat governs this evolution?Most pertinently,as Prof.Hochstrasser asks:How do the structural and dynamical results obtained from simple systems help us to understand the behaviour of more complex materials?What do clusters,for example,teach us about liquid structure?What do we learn about the dynamic behaviour in liquids and solids,from the study of Ðnite-sized assemblies?What conditions require statistical as opposed to discrete (level by level)models of dynamics?What is reasonable (or unreasonable)about seeking a microscopic quantum mechanical description of liquids?Investigations of small molecules teach us about chemical bonding and the charac-teristics of accurate potential energy surfaces.Weaker interactions are often evaluated from studies of van der Waals complexes and Ðnite clusters.The dynamics in such systems are determined by forces obtained from these potentials.While the properties of molecules in large clusters,liquids or extended aggregates might,in some cases,be framed in terms of isolated molecule potentials there will be cases where this is not possible.The most appropriate description of the dynamics of complex systems depends upon how the energy is partitioned.Typically,for a solution phase problem,the Hamiltonian involves the molecular part,and the solvent part which are separately solved either exactly or approx-H M H S ,imately,and a coupling part,that slightly mixes them.This partitioning yields a V MS ,useful representation when the molecular or solvent states are only slightly modiÐed by469470Concluding Remarkstheir interactions.The molecular potential is especially valuable in this case and may dominate the motion of the molecular nuclei even though the dynamics may be in a statistical limit.The intermolecular perturbations cause irreversible relaxation corre-sponding to transitions between the molecular states,accompanied by energy transfer to and from the solvent bath.In order that energy can be transferred to it,the solvent must have unoccupied states.Energy transfer to the molecule requires occupied states of the bath.A fully worked out example where this approach is nearly exact is the coupling of an atom or molecule to a very weak radiation Ðeld.Another example would be molecu-lar dynamics in very weakly interacting solvents.Quantum dynamics in this limit can be handled along the lines of RedÐeld theory,in which the reduced molecular density matrix is expanded to second order in This approach gives rise to spectral shifts V MS .and to coherence transfer along with relaxation of both the population and the phase of the molecular levels.The nuclear motions are largely governed by a slightly modiÐed version of the molecular potential.In stochastic dynamics,the solvent e†ect is estimated from correlation functions of where the Ñuctuations in the interaction potential V MS (t ),due to the motion of very large numbers of solvent nuclei and electrons are modelled by statistical forms or calculated from molecular dynamics simulations.There are situations where the molecular potential is so severely modiÐed by the solvent Èsolute interaction that an alternative representation is more realistic.In such cases it may be that the system of interest is a supermolecule or cluster,consisting of the solute and strongly interacting solvent molecules.The Hamiltonian could then be parti-tioned to yield a term for the energy states of the cluster,and the surrounding bath,comprising those solvent molecules that do not interact strongly with the solute.The dynamics can be determined from one of the perturbation approaches mentioned earlier.In examples of this type the relevant nuclear dynamics are controlled by the potential surface of the cluster but the irreversible relaxation is caused by the weak coupling between the supermolecule and the solvent.Measurements and calculations of potential energy surfaces of solute Èsolvent clusters are sorely needed for this approach.Such a picture assumes that the long-range forces are weak and that the interactions between the solvent molecules are not much inÑuenced by the presence of the solute.These assumptions would surely be inappropriate in accounting for the dynamics and struc-ture of polar molecules or ions in water,to give just one example.When Coulombic forces are important in determining structure,and their Ñuctuations determine the dynamics,we can imagine that long-range interactions will have to be included.As chemical reactions take place and charges redistribute,there may be large changes in the energy from interactions with moving solvent molecules.The solvent nuclear dynamics have been measured by time-resolved Kerr e†ects in transparent media,by dynamic Stokes shifts and by three pulse photon echoes in dye systems and in proteins (see the paper by Fleming and co-workers in this Discussion 1).In the cases that were examined theoretically,the major part of the solvent reorganisation energy around charges appears to originate from the Ðrst solvation shell.While the experiments charac-terise correlation functions of the solvent,they usually do not provide a microscopic picture of the motions that cause the energy changes other than to classify them broadly,as vibrational,librational or di†usive.On the other hand we would like to know when there are changes in the solute potential surfaces as a result of solvation and when solvation can inÑuence reactive motions.Equally important is the experimental charac-terisation of the solvent structures as the solvation dynamics evolve.Simulations are able to predict the answers to all these questions so some experimental results will allow the theory to be tested.In experiments on the photodissociation of changes HgBr 2,2in the potential energy function of the released HgBr occur on the timescale of the solvation.They can be followed through the changes in the vibrational frequency.The fast process involves the breaking up of the solvent structure associated with the tri-atomic molecule and a slower process involves the construction of the equilibriumR .M .Hochstrasser and J .P .Simons 471solvent structure around the HgBr fragment.Similar results for solvent structure changes were seen for ClO ~.3These structures should be accessible to spectroscopic experiments.As shown in the paper by Neumark and co-workers,4the cage reaction of I and I ~in a cluster of induces slow solvent evaporation and fast vibrational relax-CO 2ation.These experiments show details of the solvent involvement in the reactive motions that have proved difficult to obtain in solution phase experiments.Of course,it is known from experiment that the energy of a solution phase reaction is used to heat up the surrounding solvent molecules,and that the rate of reaction can be altered if the heat di†usion is very slow compared with the reaction rate.However,at conventional liquid densities (10M )the number of solvent molecules over which the released energy is dis-tributed grows to approximately 25in 10ps,by classical heat di†usion.The task of Ðnding a microscopic level description of solvent e†ects on relaxation and chemical processes is daunting.Nuclear motions can be extremely complex even for relatively small molecules in the absence of intermolecular interactions.When the solvent Èsolute interactions are strong the solvent forces can introduce additional anhar-monicity into the “soluteÏmotions thereby causing nuclear trajectories that are e†ec-tively absent in the isolated solvent molecule.For example,in the gas phase IR spectrum of the asymmetric stretch region shows no sign of any perturbations.In aqueous N 3~,solution,however,the mode relaxes in ca .1ps due to very strong coupling between solute modes;the motion is a combined solvent Èsolute displacement.5Such motions could be characterised through IR and Raman studies of clusters.There are many things (of course)that we have not heard about at this Discussion.One of the most important is single molecule spectroscopy,which can reveal the dis-tribution of molecular properties associated with Ñuctuations in their environment.When the observation time is shorter than the Ñuctuation timescale,the ensemble average is no longer equal to the time average.Not much has been heard about mol-ecules at interfaces,which is where much chemistry and biochemistry actually takes place.Not much has been heard about optical control of reaction rates in condensed phases;can we tune the solvent response to the lifetime of the transition state?We have not heard much about self-assembled supramolecular systems where the dynamics of photon-induced processes may be controlled by synthetic designÈmuch as it is in a photosynthetic centre.Perhaps these will feature in a future Faraday Discussion.References1Y.Nagasawa,J-Y.Yu,M.Cho and G.R.Fleming,Faraday Discuss .,1997,108,23.2M.Lim,M.Wo†ord,P.Hamm and R.M.Hochstrasser,Chem .Phys .L ett .,1998,in press.3M.Lim,S.Gnanakaran and R.M.Hochstrasser,J .Chem .Phys .,1997,106,3485.4B.J.Greenblatt,M.T.Zanni and M.Neumark,Faraday Discuss .,1997,108,101.5J.C.Owrutsky,D.Raftery and R.M.Hochstrasser,Ann .Rev .Phys .Chem .,1994,45,519.。
HH11CDIGITAL THERMOMETERServicing North America:U.S.A. Omega Engineering, Inc.Headquarters: Toll-Free: 1-800-826-6342 (USA & Canada only) Customer Service: 1-800-622-2378 (USA & Canada only) Engineering Service: 1-800-872-9436 (USA & Canada only) Tel: (203) 359-1660 Fax: (203) 359-7700 e-mail:**************For Other Locations Visit /worldwideIt is the policy of OMEGA Engineering, Inc. to comply with all worldwide safety and EMC/EMI regulations that apply. OMEGA is constantly pursuing certification of its products to theEuropean New Approach Directives. OMEGA will add the CE mark to every appropriate device upon certification.The information contained in this document is believed to be correct, but OMEGA accepts no liability for any errors itcontains, and reserves the right to alter specifications without notice.WARNING: These products are not designed for use in, and should not be used for, human applications.INTRODUCTIONThis instrument is a portable 4½ digit, compact-sized digital thermometer designed to use external K-type thermocouples as temperature sensor. Temperature indication follows National Bureau of Standards and IEC 584 tem-perature/voltage tables for K-type thermocouples. One K-type thermocouple is supplied with the thermometer.SAFETY INFORMATIONIt is recommended that you read the safety and operation instructions before using this t hermometer.WARNINGTo avoid electrical shock, do not use this instrument when working voltages at the measurement surface over 24V AC or 60V DC.WARNINGTo avoid damage or burns, do not make temperaturemeasurement in microwave ovens.CAUTIONRepeated sharp flexing can break the thermocouple leads. To prolong lead life, avoid sharp bends in theleads, especially near the connector.Thesymbol on the instrument indicates that the operator must refer to an explanation in this manual.SPECIFICATIONSELECTRICALTemperature Scale: Celsius or Fahrenheit user-selectable Measurement Range:-200°C to 1372°C, -328°F to 2501°F Auto range: 0.1°C/1°C, 0.1°F/1°FAccuracy:Accuracy is specified for operating tempera-tures over the range of 18°C to 28°C (64°F to 82°F), for 1 year, not including thermocouple error. ±(0.1%rdg+0.5°C) on -60°C to 1372°C ±(0.1%rdg+2°C) on -60°C to -200°C ±(0.1%rdg+1°F) on -76°F to 2501°F ±(0.1%rdg+4°F) on -76°F to -328°F Temperature Coefficient:0.1 times the applicable accuracy specification per °C from 0°C to 18°C and 28°C to 50°C (32°F to 64°F and 82°F to122°F). Input Protection:60V dc or 24V ac rms maximum input voltage on any combination of input pins. Input Connector:Accepts standard miniature thermocouple connectors (flat blades spaced 7.9mm, center to center). ENVIRONMENTALAmbient Operating Ranges: 0°C to 50°C (32°F to 122°F) Storage Temperature:-20°C to 60°C (-4°F to 140°F)GENERALDisplay: 4½ digit liquid crystal display (LCD) with max-imum reading of 19999.Low battery indication: The “ ” is displayed when the battery voltage drops below the operating level. Measurement rate: 1 time/second.Operating environment: 0°C to 50°C at<70% R.H.Storage temperature: -20°C to 60°C, 0 to 80% R.H. with battery removed from meter.Accuracy: Stated accuracy at 23°C±5°C, <75% R.H. Battery: Standard 9V battery (NEDA 1604, IEC 6F22). Battery Life: 100 hours typical with carbon zinc battery. Dimensions: 210mm(H) x 65mm(W) x 35mm(D). Weight: approx. 282g including battery.Supplied Wire: 4 feet type “K” thermocouple bead wire (PTFE tape insulated). Maximum insulation tempera-ture 260°C (500°F). Wire accuracy ±2.2°C or ±0.75% of reading (whichever is greater) from 0°C to 800°C.OPERATING INSTRUCTIONS1.“°C/°F” Button: Selecting the Temperature ScaleReadings are displayed in either degrees Celsius(°C) or degrees Fahrenheit(°F). When the thermometer is turned on, it is set to the temperature scale that was in use when the thermometer was last turned off. To change the temperature scale, hold down for 2 seconds “APO >2S°C/°F” key.2.“HOLD” ButtonPress the “HOLD” key to enter the Data Hold mode, the “HOLD” annunciator is displayed. When HOLD mode is selected, the thermometer held the present readings and stops all further measurements. Press the “HOLD” key again cancels HOLD mode, causing the thermometer to resume taking measurements.3.“REL” ButtonPress “REL” key to enter Relative mode, zero the display, and store the displayed reading as a reference value and annunciator REL is displayed. Pressing “REL” key over 2 seconds to exit the relative mode.4.“APO” ButtonPressing “APO >2S °C/°F” key to trigger on or off APO mode, and then APO annunciator will appear or disappear on the display. Power is automatically turn off, if no operation for a period of time, and “APO”annunciator is displayed at upper-left corner when APO function is enabled.5.“MIN/MAX” ButtonPress “MIN/MAX” once to begin recording MIN and MAX. Press “MIN/MAX” to select MIN or MAX or MAX-MIN or A VG. Hold down for 2 seconds to exit MIN/MAX function.In the MIN/MAX record mode can not power off, must leave MIN/MAX record mode then power off.OFFSET ADJUSTMENTThe OFFSET control is set at the factory to allow for the variations found in standard thermocouples. By adjusting the OFFSET control, you can optimize measurement ac-curacy for a particular thermocouple at a particular tem-perature.Adjusting for Accurate Measurements1. Connect the thermocouple to the input connector and turn the thermometer on.2. Place the thermocouple in a known, stable temperature environment at or near the temperature you wish to measure, and allow the readings to stabilize.3. Slowly adjust the OFFSET control so that the thermom-eter reading matches the temperature of the known en-vironment. Leave sufficient time between adjustments to allow for measurement lag.Resetting the OFFSET ControlTo return the OFFSET control to the factory setting without having to recalibrate the thermometer, perform the following procedure:1. Connect a thermocouple that is in good working order to the input that is to be adjusted.2. Place the thermocouple in an ice-water bath and allow the readings to stabilize.3. Slowly adjust the OFFSET control until the thermome-ter reads 0°C (32°F).Probe DetectorThe red LED will be ON when no K-type thermocouple probe is inserted into the TEMP input of the meter, and will be OFF after K-type thermocouple probe is inserted. If the red LED stays ON when thermocouple probe is at-tached, check the thermocouple probe which might be damaged.OPERATOR MAINTENANCEWARNINGTo avoid possible electrical shock, disconnect the thermocouple connectors from the thermometer beforeremoving the cover.Battery Replacement1. Power is supplied by 9V (NEDA 1604, IEC 6F22).2. The “” appears on the LCD display when replace-ment is needed.3. Remove the battery from battery contacts.4. When not use for long time remove battery.5. Don’t keep in place with high Temp, or high humidity. CleaningPeriodically wipe the case with a damp cloth and deter-gent, do not use abrasives or solvents.Where Do I Find Everything I Need forProcess Measurementand Control?OMEGA…Of Course!Shop online at TEMPERATUREThermocouple, RTD & Thermistor Probes,Connectors, Panels & AssembliesWire: Thermocouple, RTD & ThermistorCalibrators & Ice Point ReferencesRecorders, Controllers & Process MonitorsInfrared PyrometersPRESSURE, STRAIN AND FORCETransducers & Strain GagesLoad Cells & Pressure GagesDisplacement TransducersInstrumentation & AccessoriesFLOW/LEVELRotameters, Gas Mass Flowmeters & Flow Com-putersAir Velocity IndicatorsTurbine/Paddlewheel SystemsTotalizers & Batch ControllerspH/CONDUCTIVITYpH Electrodes, Testers & AccessoriesBenchtop/Laboratory MetersControllers, Calibrators, Simulators & PumpsIndustrial pH & Conductivity EquipmentDATA ACQUISITIONData Acquisition & Engineering SoftwareCommunications-Based Acquisition SystemsPlug-in Cards for Apple, IBM & CompatiblesDatalogging SystemsRecorders, Printers & Plo tte rsHEATERSHeating CableCartridge & Strip HeatersImmersion & Band HeatersFlexible HeatersLaboratory HeatersENVIRONMENTALMONITORING AND CONTROLMetering & Control InstrumentationRefractometersPumps & TubingAir, Soil & Water MonitorsIndustrial Water & Wastewater TreatmentpH, Conductivity & Dissolved OxygenInstrumentsMade in Taiwan WARRANTY/DISCLAIMEROMEGA ENGINEERING, INC. warrants this unit to be free of defectsin materials and workmanship for a period of 13 months from dateof purchase. OMEGA’s WARRANTY adds an additional one (1) monthgrace period to the normal one (1) year product warranty to coverhandling and shipping time. This ensures that OMEGA’s customersreceive maximum coverage on each product.If the unit malfunctions, it must be returned to the factory for evalua-tion. OMEGA’s Customer Service Department will issue an AuthorizedReturn (AR) number immediately upon phone or written request.Upon examination by OMEGA, if the unit is found to be defective, itwill be repaired or replaced at no charge. OMEGA’s WARRANTY doesnot apply to defects resulting from any action of the purchaser, includ-ing but not limited to mishandling, improper interfacing, operationoutside of design limits, improper repair, or unauthorized modifica-tion. 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u1080p resolution for sharp imagesu Easy to install with auto zoom/focus lens, wizardand pre-configured modesu Fully configurable quad streamingu IR version with 15 m (50 ft) viewing distanceu Regions of interest and E-PTZThe HD indoor dome cameras from Bosch areprofessional surveillance cameras that provide highquality HD images for demanding security andsurveillance network requirements. These domes aretrue day/night cameras offering excellent performanceday or night.There is a version with a built-in active infraredilluminator that provides high performance in extremelow-light environments.System overviewEasy to install stylish indoor domeIdeal for indoor use, the stylish design is suitable forinstallations where appearance and flexible coverageare important. The varifocal lens allows you to choosethe coverage area to best suit your application. Usingthe proprietary pan/tilt/rotation mechanism, installerscan select the exact field of view. Mounting optionsare numerous, including surface, wall, and suspended-ceiling mounting.The automatic zoom/focus lens wizard makes it easyfor an installer to accurately zoom and focus thecamera for both day and night operation. The wizard isactivated from the PC or from the on-board camerapush button making it easy to choose the workflowthat suits best.The AVF (Automatic Varifocal) feature means that thezoom can be changed without opening the camera.The automatic motorized zoom/focus adjustment with1:1 pixel mapping ensures the camera is alwaysaccurately focused.FunctionsIntelligent Dynamic Noise Reduction reducesbandwidth and storage requirementsThe camera uses Intelligent Dynamic Noise Reductionwhich actively analyzes the contents of a scene andreduces noise artifacts accordingly.The low-noise image and the efficient H.264compression technology provide clear images whilereducing bandwidth and storage by up to 50%compared to other H.264 cameras. This results inreduced-bandwidth streams that still retain a highimage quality and smooth motion. The cameraprovides the most usable image possible by cleverlyoptimizing the detail-to-bandwidth ratio.Area-based encodingArea-based encoding is another feature which reduces bandwidth. Compression parameters for up to eight user-definable regions can be set. This allows uninteresting regions to be highly compressed, leaving more bandwidth for important parts of the scene. Bitrate optimized profileThe average typical optimized bandwidth in kbits/s for various image rates is shown in the table:Multiple streamsThe innovative multi-streaming feature delivers various H.264 streams together with an M‑JPEG stream. These streams facilitate bandwidth-efficient viewing and recording as well as integration with third-party video management systems.Depending on the resolution and frame rate selected for the first stream, the second stream provides a copy of the first stream or a lower resolution stream.The third stream uses the I-frames of the first stream for recording; the fourth stream shows a JPEG image at a maximum of 10 Mbit/s.Regions of interest and E-PTZRegions of Interest (ROI) can be user defined. The remote E-PTZ (Electronic Pan, Tilt and Zoom) controls allow you to select specific areas of the parent image. These regions produce separate streams for remote viewing and recording. These streams, together with the main stream, allow the operator to separately monitor the most interesting part of a scene while still retaining situational awareness.Built-in microphone, two-way audio and audio alarm The camera has a built-in microphone to allow operators to listen in on the monitored area. Two-way audio allows the operator to communicate with visitors or intruders via an external audio line input and output. Audio detection can be used to generate an alarm if needed.If required by local laws, the microphone can be permanently blocked via a secure license key. Tamper and motion detectionA wide range of configuration options is available for alarms signaling camera tampering. A built-in algorithm for detecting movement in the video can also be used for alarm signaling.Storage managementRecording management can be controlled by the Bosch Video Recording Manager (VRM) or the camera can use iSCSI targets directly without any recording software.Edge recordingThe MicroSD card slot supports up to 2 TB of storage capacity. A microSD card can be used for local alarm recording. Pre-alarm recording in RAM reduces recording bandwidth on the network, or — if microSD card recording is used — extends the effective life of the storage medium.Cloud-based servicesThe camera supports time-based or alarm-based JPEG posting to four different accounts. These accounts can address FTP servers or cloud-based storage facilities (for example, Dropbox). Video clips or JPEG images can also be exported to these accounts.Alarms can be set up to trigger an e-mail or SMS notification so you are always aware of abnormal events.Easy installationPower for the camera can be supplied via a Power-over-Ethernet compliant network cable connection. With this configuration, only a single cable connection is required to view, power, and control the camera. Using PoE makes installation easier and more cost-effective, as cameras do not require a local power source.The camera can also be supplied with power from+12 VDC power supplies.For trouble-free network cabling, the camera supports Auto-MDIX which allows the use of straight or cross-over cables.True day/night switchingThe camera incorporates mechanical filter technology for vivid daytime color and exceptional night-time imaging while maintaining sharp focus under all lighting conditions.Hybrid modeAn analog video output enables the camera to operate in hybrid mode. This mode provides simultaneous high resolution HD video streaming and an analog video output via an SMB connector. The hybrid functionality offers an easy migration path from legacy CCTV to a modern IP-based system.Access securityPassword protection with three levels and 802.1x authentication is supported. To secure Web browser access, use HTTPS with a SSL certificate stored in the camera.Complete viewing softwareThere are many ways to access the camera’s features: using a web browser, with the Bosch Video Management System, with the free-of-chargeBosch Video Client or Video Security Client, with the video security mobile app, or via third-party software. Video security appThe Bosch video security mobile app has been developed to enable Anywhere access to HD surveillance images allowing you to view live images from any location. The app is designed to give you complete control of all your cameras, from panning and tilting to zoom and focus functions. It’s like taking your control room with you.This app, together with the separately available Bosch transcoder, will allow you to fully utilize our dynamic transcoding features so you can play back images even over low-bandwidth connections.System integrationThe camera conforms to the ONVIF Profile S, ONVIF Profile Q and ONVIF Profile G specifications. Compliance with these standards guarantees interoperability between network video products regardless of manufacturer.Third-party integrators can easily access the internal feature set of the camera for integration into large projects. Visit the Bosch Integration Partner Program (IPP) website () for more information.HD standardsComplies with the SMPTE 274M-2008 Standard in:–Resolution: 1920x1080–Scan: Progressive–Color representation: complies with ITU-R BT.709–Aspect ratio: 16:9–Frame rate: 25 and 30 frames/sComplies with the SMPTE 296M-2001 Standard in:–Resolution: 1280x720–Scan: Progressive–Color representation: complies with ITU-R BT.709–Aspect ratio: 16:9–Frame rate: 25 and 30 frames/sInstallation/configuration notesDimensions mm (inch)Parts included•Camera•Screw kit•Installation documentation Technical specificationsSensitivity – (3200K, reflectivity 89%, F1.3, 30IRE)Ordering informationFLEXIDOME IP indoor 5000 HDProfessional IP dome camera for indoor HD surveillance. Varifocal 3 to 10 mm f1.3 lens; IDNR; day/ night; H.264 quad-streaming; cloud services; motion/ tamper/audio detection; microphone; 1080pOrder number NIN-51022-V3FLEXIDOME IP indoor 5000 IRProfessional IP dome camera for indoor HD surveillance. Varifocal 3 to 10 mm f1.3 lens; IDNR; day/ night; H.264 quad-streaming; cloud services; motion/ tamper/audio detection; microphone; 1080p; infrared Order number NII-51022-V3FLEXIDOME IP indoor 5000 HDProfessional IP dome camera for indoor HD surveillance. Automatic Varifocal 3 to 10 mm f1.3 lens; DC iris; IDNR; day/night; H.264 quad-streaming; cloud services; motion/tamper/audio detection; microphone; 1080pOrder number NIN-50022-A3FLEXIDOME IP indoor 5000 IRProfessional IP dome camera for indoor HD surveillance. Automatic Varifocal 3 to 10 mm f1.3 lens; DC iris; IDNR; day/night; H.264 quad-streaming; cloud services; motion/tamper/audio detection; microphone; 1080p; infraredOrder number NII-50022-A3AccessoriesNDA-LWMT-DOME Dome Wall MountSturdy wall L-shaped bracket for dome cameras Order number NDA-LWMT-DOMENDA-ADTVEZ-DOME Dome Adapter BracketAdapter bracket (used together with appropriate wall or pipe mount, or surface mount box)Order number NDA-ADTVEZ-DOMEVEZ-A2-WW Wall MountWall mount (Ø145/149 mm) for dome cameras (use together with appropriate dome adapter bracket); whiteOrder number VEZ-A2-WWVEZ-A2-PW Pipe MountPendant pipe mount (Ø145/149 mm) for dome cameras (use together with appropriate dome adapter bracket); whiteOrder number VEZ-A2-PWLTC 9213/01 Pole Mount AdapterFlexible pole mount adapter for camera mounts (use together with the appropriate wall mount bracket). Max. 9 kg (20 lb); 3 to 15 inch diameter pole; stainless steel strapsOrder number LTC 9213/01NDA-FMT-DOME In-ceiling mountIn-ceiling flush mounting kit for dome cameras(Ø157 mm)Order number NDA-FMT-DOMENDA-ADT4S-MINDOME 4S Surface Mount BoxSurface mount box (Ø145 mm / Ø5.71 in) for dome cameras (use together with the appropriate dome adapter bracket).Order number NDA-ADT4S-MINDOMEMonitor/DVR Cable SMB 0.3M0.3 m (1 ft) analog cable, SMB (female) to BNC (female) to connect camera to coaxial cableOrder number NBN-MCSMB-03MMonitor/DVR Cable SMB 3.0M3 m (9 ft) analog cable, SMB (female) to BNC (male) to connect camera to monitor or DVROrder number NBN-MCSMB-30MNPD-5001-POE Midspan PoE InjectorPower-over-Ethernet midspan injector for use with PoE enabled cameras; 15.4 W, 1-portOrder number NPD-5001-POENPD-5004-POE Midspan PoE InjectorPower-over-Ethernet midspan injectors for use with PoE enabled cameras; 15.4 W, 4-portsOrder number NPD-5004-POERepresented by:North America:Europe, Middle East, Africa:Asia-Pacific:China:Latin America and Caribbean:Bosch Security Systems, Inc. 130 Perinton Parkway Fairport, New York, 14450, USA Phone: +1 800 289 0096 Fax: +1 585 223 9180***********************.com Bosch Security Systems B.V.P.O. Box 800025617 BA Eindhoven, The NetherlandsPhone: + 31 40 2577 284Fax: +31 40 2577 330******************************Robert Bosch (SEA) Pte Ltd, SecuritySystems11 Bishan Street 21Singapore 573943Phone: +65 6571 2808Fax: +65 6571 2699*****************************Bosch (Shanghai) Security Systems Ltd.203 Building, No. 333 Fuquan RoadNorth IBPChangning District, Shanghai200335 ChinaPhone +86 21 22181111Fax: +86 21 22182398Robert Bosch Ltda Security Systems DivisionVia Anhanguera, Km 98CEP 13065-900Campinas, Sao Paulo, BrazilPhone: +55 19 2103 2860Fax: +55 19 2103 2862*****************************© Bosch Security Systems 2016 | Data subject to change without notice 188****8507|en,V9,01.Jun2016。