Electric and magnetic fields inside neurons and their impact upon the cytoskeletal microtub
电磁场英文作文
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电磁场英文作文English: Electromagnetic fields are a fundamental aspect of physics that encompass the combined electric and magnetic fields that permeate through space. These fields are generated by the movement of electrically charged particles, such as electrons, creating a force that can affect objects within the field. Electromagnetic fields play a crucial role in numerous phenomena, including light propagation, radio wave transmission, and the operation of electrical devices. Understanding electromagnetic fields is essential in various fields of science and technology, from designing electrical circuits to explaining the behavior of celestial bodies. Moreover, the study of electromagnetic fields has significant implications in our daily lives, such as in the development of new technologies and advancements in communication systems. Overall, the intricate interplay of electric and magnetic fields in electromagnetic phenomena highlights the fundamental nature of these fields in shaping the physical world around us.中文翻译: 电磁场是物理学中的一个基本方面,涵盖了贯穿空间的电场和磁场的结合。
关于电磁场的英文作文
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关于电磁场的英文作文英文回答:Electromagnetic fields are a fundamental aspect of our modern world. They are all around us, from the electricity that powers our homes to the signals that allow us to communicate wirelessly. Understanding electromagneticfields is essential for many aspects of our daily lives.One of the key concepts in electromagnetism is the idea of electric and magnetic fields. These fields are invisible, but they have a significant impact on the world around us. Electric fields are created by electric charges, such asthe positive and negative charges in a battery. Magnetic fields, on the other hand, are created by moving electric charges, such as the current flowing through a wire.These fields interact with each other and with charged particles, creating a wide range of phenomena. For example, when an electric field and a magnetic field areperpendicular to each other, they can produce a force that causes a charged particle to move in a circular path. Thisis the principle behind the operation of a particle accelerator.Electromagnetic fields also play a crucial role in the transmission of information. Radio waves, for instance, are a type of electromagnetic wave that carries signals fromone place to another. We use radio waves to listen to music, talk on our cell phones, and watch television. Without electromagnetic fields, these technologies would not be possible.In addition to their practical applications, electromagnetic fields also have some interesting properties. For example, they can be described by mathematical equations known as Maxwell's equations. These equations provide a comprehensive description of howelectric and magnetic fields behave and interact with each other. They have been instrumental in the development of modern physics and engineering.中文回答:电磁场是我们现代世界的一个基本方面。
电子信息工程专业英语翻译清华出版社EnglishforITandEE03
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will experience a force (in a similar way that planets
experience a force in the gravitational field of the Sun). If
电子信息工程专业英语 翻译清华出版社
EnglishforITandEE03
2020/11/27
电子信息工程专业英语翻译清华出版 社EnglishforITandEE03
Unit 3
EM Fields, Antenna and Microwaves
电子信息工程专业英语翻译清华出版 社EnglishforITandEE03
two locations. For instance, the metal atoms in a radio
transmitter appear to transfer energy continuously. This view
is useful to a certain extent (radiation of low frequency), but
Part I
Electromagnetic Field
电子信息工程专业英语翻译清华出版 社EnglishforITandEE03
New Words
vicinity 邻近,附近 charge 电荷 photon 光子 atom 原子 catastrophe 大灾难,大祸 emission 发射,散发 incident 入射的 electrodynamics 电动力学 gravitational 重力的
•随着时间的推移,人们认识到 电场和磁场是电磁场这一整体 的两个部分。
电子信息工程专业英语翻译清华出版 社EnglishforITandEE03
纳达场域人手:全功能电磁场仪说明书
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DatasheetNarda FieldManNarda FieldMan ®All-in-one electromagnetic field meter ranging from 0 Hz to 90 GHzThe Narda FieldMan performs highly accurate measure-ments of non-ionizing high-frequency radiation and low-frequency fields. Equipped with digital probes for measuring electric or magnetic field strengths, it covers the range from static and low-frequency fields in medical and industrial applications to mobile radio frequencies and millimeter waves. Flat frequency response probes (“flat probes”), as well as so-called shaped probes that evaluate the field strength on the basis of a human safety standard are available. Probes with built-in FFT analysis enable spectral measurements along with time domain analyses up to frequencies of 400 kHz. All probes have a digital interface that transmits the measurement data to the basic device in a fail-safe manner. This eliminates the need to calibrate the basic unit.›Non-directional measurement using isotropic probes for applications in the frequency range 0 Hz (DC) to 90 GHz›Large sunlight readable color display 5” diagonal with 1280x720 HD resolution›Digital probe interface for broadband and selective probes – no more meter calibration›Powerful time and frequency domain analysis for low frequency fields up to 400 kHz including Weighted Peak measurements›WiFi/Bluetooth interface for remote operation via smartphone app (Option)›Built-in GPS receiver and rangefinder for easy location determination (Option)›Fast data transmission ›optical interface ›Ethernet ›USB-CApplicationsThe Narda FieldMan is used to make precision measurements to establish human safety, particularly in workplace environments where high electric or magnetic field strengths are likely to occur. An essential task is to demonstrate compliance with generalsafety regulations, such as FCC, IEEE, ICNIRP or EMF Directive 2013/35/EU. Examples of measurement environments are:›Radiocommunication base stations (e.g. IEC / EN 62232)›Broadcasting systems (e.g. IEC 62577)›Radar and satellite communications systems ›Induction heating and melting (e.g. EN 50519)›Household appliances (e.g. IEC / EN 62233)›Electric welding equipment (e.g. IEC / EN 62822)›Railroad operations (e.g. EN 50500)›Automotive operations (e.g. IEC 62764)›Energy supply systems (e.g. IEC / EN 62110)›Electrical medical devices (e.g. IEC / EN 60601)›TEM cells and absorber chambers to demonstrate electromagnetic compatibility (EMC)Digital ProbesA large number of isotropic field probes are available for theFieldMan. All of them transmit their information and measurement data as a digital signal to the FieldMan, either via an electrical USB interface or via an optical COM interface. In this way,interference is significantly reduced compared to high-resistance analog interfaces. The specially developed screw connectors and electrical contacts are extremely robust and resilient.The probes are automatically recognized after connection to the FieldMan. Sensors inside the probe record the temperature of the measuring location and transmit it to the FieldMan display. In addition to the automatic offset correction, the temperature measurement is also used to compensate for the typicaltemperature dependency of the sensor diodes. The advantages are uninterrupted measurements without zero adjustment and higher measurement accuracy over wide temperature ranges. An automatic self-test function can even detect possible errors in the sensor system, which means that additional checking with a test generator is superfluous. Only the digital probes arecalibrated. You can continue to use your FieldMan during this time.There are probes for many different applications with theappropriate frequency and level ranges. The following table gives an overview of common areas of application.Frequency rangeDC up to1 kHzUp to400 kHzUp to400 kHz Up to 30 MHz Up to 1 GHz Up to 6 GHz Up to 40 GHz Up to 90 GHz Up to 50 GHz Field type, magnetic (H) or electric (E)H E+HHHHEEEE ShapedProbe modelsHP-01EHP-50F/G BFD-400-1 (100 cm 2) BFD-400-3 (3 cm 2) HFD-3061 HFD-0191 EFD-0391 EFD-0392 EFD-0691 EFD-0692 EFD-1891 EFD-4091 EFD-5091 EFD-6091EFD-9091EAD-5091EBD-5091ECD-5091EDD-50915G mobile radio / telecommunications Broadcast radio / TVSatellite communications RadarIndustry: Heating and temperingIndustry: Plastics weldingIndustry: Semiconductor productionMedicine: Diathermy, hyperthermyLeak locationHousehold appliances Electric welding equipmentRailroad operationsAutomotive operationsEnergy supply systems Electric medical devicesAccredited calibration includedProbe interfaceOptical connectionDigital probe interfaceFig. 1. Areas of application and suitable probe modelsUse and benefitDuring the development of the FieldMan, special attention was paid to achieving simple, well-structured and fluid operation. The arrangement of many display elements known from smartphones, the self-explanatory symbols and the FieldMan processes, which are perfectly tailored to the measurement tasks, offer maximum ease of use. The large, anti-glare HD color display shows the measured values numerically and graphically with all important additional information in a clear form and is easy to read even in bright sunlight. From simple broadband measurements to sophisticated time signal recording in real time or spectral frequency analysis of low-frequency fields, you have the right operating modes at your disposal.Measurement results can be commented on by text or voice and can be saved as a screen copy at the push of a button. Built-in sensors record the current environmental conditions as well as the position data and automatically add them to the measurement result. The built-in distance meter (option) shows you the measuring height above the ground, which makes the exact positioning of the measuring device much easier. For a better overview, the measurement results can be assigned to freely definable projects, which is particularly helpful when the measurement locations change frequently. If you want todocument your measurement results with photos and videos, the FieldMan smartphone app will help you. For example, the app wirelessly transfers media files created with the smartphone to the project directory on the FieldMan SD memory card. A newly developed, extremely powerful PC software "Narda-TSX" is available for documenting the measurement results, media and other information. It is Narda's new software platform for device configuration, measurement data evaluation and documentation, which in addition to the FieldMan will also support other Narda products in the future.Fig. 2. FieldMan display and controlsFig. 3. The FieldMan is supplied with a robust transport caseProbe connectionBrightness sensor LoudspeakerMicrophone, humidity sensor Status bar Probe information Measurement informationMeasurement isotropic Measurement single axes Statistical values Interface panelMeasurement graphic: Time curve, spectrum or bar graph Softkey symbolsSoftkeys Save key Back key Navigation keyStatus LEDDefinitions and ConditionsConditionsUnless otherwise noted, specifications apply after 30 minutes warm-up time within the specified environmental conditions. The product is within the recommended calibration cycle.Specifications with limitsThese describe product performance for the given parameter covered by warranty. Specifications with limits (shown as <, ≤, >, ≥, ±, max., min.) apply under the given conditions for the product and are tested during production, considering measurement uncertainty.Specifications without limitsThese describe product performance for the given parameter covered by warranty. Specifications without limits represent values with negligible deviations, which are ensured by design (e.g. dimensions or resolution of a setting parameter). Typical values (typ.)These characterize product performance for the given parameter that is not covered by warranty. When stated as a range or as a limit (shown as <, ≤, >, ≥, ±, max., min.), they represent the performance met by approximately 80% of the instruments. Otherwise, they represent the mean value. The measurement uncertainty is not taken into account. Nominal values (nom.)These characterize expected product performance for the given parameter that is not covered by warranty. Nominal values are verified during product development but are not tested during production. UncertaintiesThese characterize the dispersion of the values attributed to the measurands with an estimated confidence level of approximately 95%. Uncertainty is stated as the standard uncertainty multiplied by the coverage factor k=2 based on the normal distribution. The evaluation has been carried out in accordance with the rules of the “Guide to the Expression of Uncertainty in Measurement” (GUM).Specifications MetricsElectric and magnetic fieldsMeasurement control and result display for the following probes and analyzers.Frequency range and level range depending on the probe/ analyzer. Broadband probes 100 kHz to 90 GHz (see list of digital broadband probes)Selective probes 1 Hz to 400 kHz, B-field (see list of digital selective probes)Probe model EHP-50F/G 1 Hz to 400 kHz, E-field and B-field (FFT-Analyzer, see separate datasheet)Probe model HP-01 0 Hz to 1 kHz, B-field (Magnetometer/ FFT-Analyzer, see separate datasheet)Electric field units V/m, mW/cm2, W/m2, % of standard (depending on the connected probe)Magnetic field units A/m, Tesla, Gauss, mW/cm2, W/m2, % of standard (depending on the connected probe)Temperature 1Logging of the ambient temperature at the time of measurement (-40 °C to +85 °C) in °C or °F Humidity 1Logging of the ambient relative humidity at the time of measurement (0% to 100% RH)Air pressure Logging of the ambient air pressure at the time of measurement (300 to 1100 hPa)Distance (Option) An ultrasonic rangefinder on the bottom side measures the distance to ground or to an object (0.25 m to 4 m) in m, ft, in or yd. Coverage ratio ≈ Distance / 4.Geolocation (Option) Built-in GNSS receiver for determining latitude, longitude and altitude (MSL).72 channels with the support of GNSS systems (GPS / QZSS, Galileo, GLONASS, BeiDou) and the SBAS extension system (WAAS, EGNOS, MSAS, GAGAN).Position accuracy: Autonomous 2.5 m CEP.DisplayDisplay type Sunlight readable 5” color TFT-LCD anti-glare display (HD 1280 x 720 pixels) Brightness Manual control or automatic control via brightness sensorOperating languages Largely language-independent measurement control via symbols.Menu languages: English, German, more are planned.1 The permissible operating range of the device and probe must not be exceeded. The temperature sensor is located in the probe.Operating ModesMode description Field Strength Broadband field measurements. Numerical results with time curve or bar graph display.Spatial Average Procedure for spatial averaging of broadband measurements over several measurement positions. Timer Logging Time-controlled broadband measurement of the field strength in a definable period.Spectrum FFT analysis with spectrum display, marker evaluation and display of the broadband level. Shaped Time Domain Time domain assessment (WPM, WRM) with digital filtering related to a selected safety limit. Scope Triggered measurement of the field curve over time with pretrigger feature.Available modes Broadband ProbesDigital Interface100 kHz to 90 GHzSelective ProbesDigital Interface1 Hz to 400 kHzModel EHP-50F/GOptical Interface1 Hz to 400 kHzModel HP-01Optical InterfaceDC to 1 kHzField Strength ☑☑☑☑Spatial Average ☑☑☑☑Timer Logging ☑☑☑☑Spectrum ☑☑☑Shaped Time Domain ☑☑Scope ☑FeaturesProbe features Recognition Probes are automatically recognized after being plugged in.Operating principle Measurement signals are sampled and processed inside the probe and provided as digital values. Offset compensation Automatic offset compensation enables gapless RF measurements without zero adjustment.Self-test Functional test including the sensor function of each measuring axis for digital interface probes.Signal detection RMS detection, Peak detection for WPM measurementsand selectable detection RMS/Peak with BDF-400 probes.Numerical display Total field (isotropic) and field components X, Y, Z (for probes up to 18 GHz).Result types Field Strength Actual, Max, Min, Avg (average) and Max Avg Spectrum Actual or Max or AvgShaped Time Domain Actual, Max and MinScope Actual, Max and marker for dB/dtAverage mode Moving average over time of the square values of the field strength.Averaging time Field Strength,Timer Logging 1 s, 3 s, 10 s, 30 s, 1 min, 3 min, 6 min, 10 min, 30 min, 1 h, 6 h, or 24 h Spectrum 4, 8, 16, 32 or 64 number of averagesGraphical display with marker function Field Strength Actual and Avg trace vs. time, time span selectable from 48 s to 24 hours.Spatial Average Bar graph of results for each measurement position (≤100) and the spatial average line. Timer Logging Timeline during measurement, results as a graph vs. time after measurement.Spectrum Frequency spectrum and selectable limit line. All axes are measured, one can be displayed. Shaped Time Domain Exposure index (WPM or WRM) in % vs. time, time span selectable from 4 min to 24 h. Scope Sign-based recorded signal with 25 % pretrigger. Recording time selectable from 1 ms to 30 s.Screenshots Manually initiated screenshot or automatically when saving a measurement result.Comments Voice and/or text comments can be assigned to a measurement result.Alarm Alarm sound and alarm message when an adjustable field strength is exceeded.Audible field indicator Acoustic hotspot search with field strength-dependent audio frequency (available for RF-probes).Scheduled measurements Mode Timer Logging with automatic wake-up and shutdown after measurement. Start time pre-selection: up to 24 h or immediate startTimer duration: up to 100 hStorage interval: 1s to 6 min (in 11 steps, up to 32000 intervals)Correction factors Post-processing for broadband probes to increase the accuracy at a known field frequency(direct frequency entry, interpolation between calibration points)Probe interface Digital probe interface for direct connection or via the optional extension cable.Optical port Serial, full duplex, ≥ 1 Mbit/s, to connect the Field Analyzer EHP-50F/G, the Magnetometer HP-01or the Digital Probe Repeater. Recommended interface for PC controlled measurements.USB 2.0 USB-C connection for battery charging, remote control and data transfer.Ethernet Gigabit Ethernet LAN connectivity for remote control and data transfer.Bluetooth (Option) BT 4.0 for remote control via smartphone app (Android).WiFi (Option) WLAN connectivity for remote control and data transfer.AUX MMCX connector, reserved for future use.Result StorageStorage triggers Manual (by keypress) or scheduled (Timer Logging Mode).Storage medium Removable micro SD card for storing measurement data, setups and comments.Storage capacity Up to 128 GB.16 GB micro SD card included.Screenshots Screenshots can be saved for documentation as PNG files.Voice recorder Voice comments can be added to measurement results (recording and playback).Text editor Text comments can be added to measurement results (integrated virtual keyboard).Photos / videos (WiFi/BT Option) Photos and videos from a smartphone can be transferred to the device using the FieldMan app.Printouts (WiFi/BT Option) Saved measurement results can be printed locally by using the FieldMan Android app for on-sitedocumentation (requires a compatible wireless printer).General SpecificationsRecommended calibration interval Calibration of the basic unit is not required. Only the probes are calibrated.Power supply internal Li-Ion rechargeable battery pack, included and replaceable external USB-C PD (maximum 12 V / 3A, compatible with BC1.2 and QC 3.0)Operating time (nom.) 16 hours (with broadband probes and analyzers)Charging time (nom.) 4 hours (80% charged in 2½ h)RF Immunity 200 V/m (100 kHz to 60 GHz); can be below the permissible measuring range of a probe. Operation in static magnetic fields ≤ 30 mT (to avoid high force on the device)Dimensions (H x W x D) 51 mm x 93 mm x 312 mm without probeWeight 695 g (without probe)Country of origin GermanyEnvironmental ConditionsRange of application Suitable for outdoor use and an operating altitude of up to 5000 mOperating temperature -20 °C to +50 °C during normal operation with battery0 °C to 40 °C during the charging process with an external chargerHumidity < 29 g/m³ (< 93 % RH at +30 °C), non-condensingIngress protection IP54 (probe screwed on, protective flap closed, stand folded in)Climatic conditions Storage 1K4 (IEC 60721-3) extended to -30 °C to +70 °C (battery removed)1K3 (IEC 60721-3) extended to -20 °C to +50 °C (battery inserted) Transport 2K3 (IEC 60721-3) extended to -30 °C to +70° COperating 7K2 (IEC 60721-3) extended to -20 °C to +50 °CMechanical conditions Storage 1M3 (IEC 60721-3) Transport 2M3 (IEC 60721-3) Operating 7M3 (IEC 60721-3)EMC European Union Complies with Directive 2014/53/EU, EN 301489-1, EN 301489-17 and EN 61326 -1 Immunity IEC/EN: 61000-4-2, 61000-4-3, 61000-4-4, 61000-4-5, 61000-4-6, 61000-4-8, 61000-4-11 Emissions IEC/EN: 61000-3-2, 61000-3-3, IEC/EN 55011 (CISPR 11) Class BSafety Complies with European Low Voltage Directive 2014/35/EU and IEC/EN 61010-1 Material Complies with European RoHS Directive 2011/65/EU and (EU)2015/863ORDERING INFORMATIONInstrument SetsDescription Part number FieldMan Basic Set-Probes are not included –Includes:›FieldMan Basic Unit›Hard Case for FieldMan and up to 5 Probes ›Power Supply USB-C PD, AU/EU/UK/US Plugs ›Cable, 2x USB-C(M), 3 A, 2 m›Shoulder Strap, 1 m ›Marking Rings for FieldMan Probes›Quick Start Guide›Safety Instructions›USB Stick: Manuals and Documents›Software Narda-TSX (free download)2460/101Digital Broadband ProbesDescription Part number Probe HFD-3061, H-Field, 300 kHz–30 MHz 2462/05 Probe HFD-0191, H-Field, 27 MHz–1 GHz 2462/06 Probe EFD-0391, E-Field, 100 kHz–3 GHz 2462/01 Probe EFD-0392, E-Field, High Power, 100 kHz–3 GHz 2462/12 Probe EFD-0691, E-Field, 100 kHz–6 GHz 2462/14 Probe EFD-0692, E-Field, 600 MHz–6 GHz 2462/20 Probe EFD-1891, E-Field, up to 18 GHz2462/02 Probe EFD-4091, E-Field, up to 40 GHz 2462/19 Probe EFD-5091, E-Field, 300 MHz–50 GHz, Thermocouple2462/03 Probe EFD-6091, E-Field, 100 MHz–60 GHz2462/17 Probe EFD-9091, E-Field, 100 MHz–90 GHz2462/18 Probe EAD-5091, FCC 1997 Controlled, Shaped, 300 kHz–50 GHz, E-Field 2462/07 Probe EBD-5091, IEEE 2019 Restricted, Shaped, 3 MHz–50 GHz, E-Field 2462/21 Probe ECD-5091, SC 6 2015 Controlled, Shaped, 300 kHz–50 GHz, E-Field 2462/16 Probe EDD-5091, ICNIRP 2020 Occ, Shaped, 300 kHz–50 GHz, E-Field 2462/22 Note: Separate data sheets are available for the probesDigital Selective ProbesDescription Part number Probe BFD-400-1, B-Field, 100 cm2, 1 Hz–400 kHz, selective 2463/01 Probe BFD-400-3, B-Field, 3 cm2, 1 Hz–400 kHz, selective2463/02 Note: Separate data sheets are available for the probesField AnalyzersDescription Part number EHP-50F E&H Field Analyzer Set, 1 Hz–400 kHz (no Transport Case included) 2404/105 EHP-50F E&H Field Analyzer Set, 1 Hz–400 kHz, Stand-alone/PC use 2404/104 HP-01 Magnetometer Set DC–1 kHz 2405/101OptionsDescription Part number Option, Narda-TSX Live Measurements, for FieldMan Digital Probes (expected from Q3 2023) 2460/95.01 Option, GPS/ Range Finder for FieldMan 2460/95.11 Option, WiFi/ Bluetooth for FieldMan (expected from Q4 2023) 2460/95.12AccessoriesDescription Part number Digital Broadband Probe Repeater 2464/01 Test-Generator 27 MHz 2244/90.38 Tripod, Non-Conductive, 1.65 m, with Carrying Bag 2244/90.31 Tripod, Benchtop, 0.16 m, Non-Conductive 2244/90.32 Tripod Extension, 0.50 m, Non-Conductive (for 2244/90.31) 2244/90.45 Handle, Non-Conductive, 0.42 m 2250/92.02 Car Charger Adapter, USB-C PD 2259/92.28 Cable, Digital Probe Extension, 2 m 2460/90.02 Cable, Digital Probe to USB 2.0 (Type A), 3 m 2460/90.03 Cable, FO Duplex (1000 µm) RP-02, 2 m 2260/91.02 Cable, FO Duplex (1000 µm) RP-02, 5 m 2260/91.09 Cable, FO Duplex (1000 µm) RP-02, 10 m 2260/91.07 Cable, FO Duplex (1000 µm) RP-02, 20 m 2260/91.03 Cable, FO Duplex (1000 µm) RP-02, 50 m 2260/91.04 Cable, FO Duplex, F-SMA to RP-02, 0.3 m 2260/91.01 O/E Converter RS232, RP-02/DB9 2260/90.06 O/E Converter USB, RP-02/USB 2260/90.07 Cable, Adapter USB 2.0 - RS232, 0.8 m 2260/90.53Narda Safety Test Solutions GmbH Sandwiesenstrasse 772793 Pfullingen, GermanyPhone +49 7121 97 32 0****************** Narda Safety Test SolutionsNorth America Representative Office435 Moreland RoadHauppauge, NY11788, USAPhone +1 631 231 1700******************Narda Safety Test Solutions S.r.l.Via Benessea 29/B17035 Cisano sul Neva, ItalyPhone +39 0182 58641****************************Narda Safety Test Solutions GmbHBeijing Representative OfficeXiyuan Hotel, No. 1 Sanlihe Road, Haidian100044 Beijing, ChinaPhone +86 10 6830 5870********************® Names and Logo are registered trademarks of Narda Safety Test Solutions GmbH - Trade names are trademarks of the owners.。
(完整word版)电气专业英语课后练习翻译
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PART1U1T1、In addition to the various power transformers, two special-purpose transformers are used with electric machinery and power systems。
The first of these special transformers is a device specially designed to sample a high voltage and produce a low secondary voltage directly proportional to it. Such a transformer is a potential transformer. A power transformer also produces a secondary voltage directly proportional to that the potential transformer is designed to handle only a very small current。
The second type of special transformer is a device designed to provide a secondary current much smaller than but directly proportional to its primary current. This device is called a current transformer。
除了各种电源变压器、两个专用变压器使用电动机械和电力系统。
第一个特殊变压器是一个高电压设备专门设计的样品和生产较低的二次电压成正比。
这样一个变压器电压互感器。
电力变压器也产生二次电压成正比的电压互感器的设计目的是处理只有一个很小的电流。
麦克斯韦方程组 英文
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麦克斯韦方程组英文English: The Maxwell's equations are a set of fundamental equations in classical electromagnetism that describe how electric and magnetic fields interact with each other and with electric charges and currents. They were formulated by the physicist James Clerk Maxwell in the 19th century and played a crucial role in the development of electromagnetic theory. The equations consist of four equations: Gauss's law for electric fields, Gauss's law for magnetic fields, Faraday's law of electromagnetic induction, and Ampère's law with Maxwell's addition. These equations are mainly concerned with the spatial and temporal changes of electric and magnetic fields, and they are usually written in differential form or integral form. In the differential form, the equations express how the fields change at each point in space, while in the integral form, they describe the flux of the fields through closed surfaces or the circulation of the fields along closed paths. The Maxwell's equations have important implications in many areas of physics and engineering, as they govern the behavior of electromagnetic waves, the propagation of signals through transmission lines, the behavior of antennas, the operation of electric motors and generators, andvarious other electromagnetic phenomena. In addition, the Maxwell's equations also played a crucial role in the development of the theory of relativity, as they led to the realization that electric and magnetic fields are two different manifestations of a single electromagnetic field, and they can transform into each other under certain conditions. Overall, the Maxwell's equations are of fundamental importance in understanding the behavior of electric and magnetic fields and their interactions with matter, and they have paved the way for numerous technological advancements and scientific discoveries.中文翻译: 麦克斯韦方程组是经典电磁学中描述电场、磁场与电荷电流相互作用的一组基本方程。
电生磁知识点
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电生磁知识点Electromagnetism is a fundamental branch of physics that studies the interactions between electric currents and magnetic fields. 电磁学是研究电流与磁场之间相互作用的物理学基础学科。
This field plays a crucial role in our daily lives, as it is responsible for a wide range of technological devices such as electric motors, generators, and transformers. 这一领域在我们日常生活中扮演着至关重要的角色,因为它负责许多技术设备的运作,比如电动机、发电机和变压器。
One of the key concepts in electromagnetism is electromagnetic induction, which refers to the generation of an electromotive force (EMF) in a conductor when it moves through a magnetic field or when there is a change in the magnetic field around it. 电磁感应是电磁学中的一个关键概念,它指的是当导体穿过一个磁场或磁场的变化时,在导体中产生电动势(EMF)。
This phenomenon is the basis for many important technologies such as power generation and transmission, as well as the operation of electric motors. 这一现象是许多重要技术的基础,比如发电和输电,以及电动机的运作。
Electric and Magnetic Fields - Houston Independent …
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Notice that the same number of lines emerges from each charge because they are equal in magnitude
Electric Field Lines
If the charges are unequal, then the number of lines emerging from them will be different
The electric field is strong where the field lines are close together and weaker when they are far apart
Electric Field Lines
The lines for a positive charge point away from the charge
Moving charges produce magnetic fields If there is a current moving through a wire, a magnetic field is produced around the wire
Magnetic Field of a wire
+ F -
Answer: 3.2 x 10-15 N along the negative x axis (to the left)
Sample Problem p. 656 #38
Find the electric field at a point midway between two charges of +30 nC and 60 nC separated by a distance of 30.0 cm
外研社新时代职业英语专业篇 电力英语教学课件u4
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课
1
Practical Reading
2
Intensive Reading
3
Extensive Reading
4
Reading into China
1
Practical Reading
2
Intensive Reading
3
Extensive Reading
4
Reading into China
Practical Reading
How to handle and store transformers after transportation
To handle transformers
• Are the transformer tanks damaged?
• Check the information on the rating plates.
Practical Reading
To store transformers
1. Make preparations and check the transformers before storage.
• If the liquid level is visible, is it high enough?
• Are there cracks in the bushings?
译
• Is there rust or paint on the transformers or their accessories?
课
电气工程及其自动化专业英语课后练习题含答案
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电气工程及其自动化专业英语课后练习题含答案Chapter 1: Introduction to Electrical EngineeringExercise 1.11.What is electrical engineering?2.List some common applications of electrical engineering. some famous electrical engineers.Answers:1.Electrical engineering is a field of engineering that dealswith the study and application of electricity, electronics, and electromagnetism.mon applications of electrical engineering include powergeneration, transportation systems, communication systems,lighting systems, and control systems.3.Some famous electrical engineers include Nikola Tesla,Thomas Edison, Michael Faraday, James Clerk Maxwell, and Samuel Morse.Exercise 1.21.What is the difference between DC and AC?2.What is the purpose of a transformer? some common electrical units.Answers:1.DC (direct current) is the flow of electric charge in asingle direction, whereas AC (alternating current) is the flow of electric charge that reverses direction periodically.2.The purpose of a transformer is to transfer electricalenergy from one circuit to another by means of electromagnetic induction.mon electrical units include voltage (volts), current(amps), resistance (ohms), power (watts), capacitance (farads), and inductance (henries).Chapter 2: Circuit AnalysisExercise 2.11.W hat is Kirchhoff’s current law?2.What is Kirchhoff’s voltage law? some common circuit elements.Answers:1.Kirchhoff’s current law states that the total currententering a junction must equal the total current leaving thejunction.2.Kirchhoff’s voltage la w states that the total voltagearound a closed loop must equal zero.mon circuit elements include resistors, capacitors,inductors, diodes, transistors, and operational amplifiers.Exercise 2.21.What is the difference between an open circuit and a shortcircuit?2.What is a series circuit?3.What is a parallel circuit?Answers:1.An open circuit is a circuit that is not complete and doesnot allow the flow of current, whereas a short circuit is acircuit that has a very low resistance and allows the flow ofcurrent to bypass the normal path.2.A series circuit is a circuit in which the components areconnected end to end so that the same current flows through each component.3.A parallel circuit is a circuit in which the components areconnected in parallel so that the voltage across each component is the same and the total current is divided among the components. Chapter 3: ElectromagnetismExercise 3.11.What is an electromagnetic wave?2.What is Faraday’s law of electromagnetic induction?3.What is Lenz’s law?Answers:1.An electromagnetic wave is a wave that is composed ofelectric and magnetic fields that are oscillating at right angles to each other and to the direction of propagation.2.Faraday’s law of electromagnetic induction states that achanging magnetic field induces an electromotive force (EMF) in a conductor that is proportional to the rate of change of themagnetic field.3.Lenz’s law states that the direction of the induced EMF issuch that it opposes the change that produced it.Exercise 3.21.What is a solenoid?2.What is the Lorentz force law?3.What is magnetic hysteresis?Answers:1.A solenoid is a coil of wire that is used to create amagnetic field when an electric current is passed through it.2.The Lorentz force law states that a charged particle that ismoving through a magnetic field experiences a force that isperpendicular to both the direction of motion and the direction of the magnetic field.3.Magnetic hysteresis is the tendency of a magnetic materialto remn magnetized even after the external magnetic field isremoved.ConclusionIn conclusion, electrical engineering is a fascinating field that involves the study and application of electricity, electronics, and electromagnetism. It is used in many common applications, such as power generation, transportation systems, and communication systems. To besuccessful in this field, it is important to have a good understanding of circuit analysis, electromagnetism, and other key concepts. These exercises should help to reinforce your understanding of the material and prepare you for future challenges in this field.。
光学英语知识点总结
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光学英语知识点总结1. Nature of LightLight is a form of electromagnetic radiation that is visible to the human eye. It travels in the form of waves, with a specific wavelength and frequency. It can also be described as a stream of particles called photons. The wave-particle duality of light is a fundamental concept in quantum mechanics, and it has important implications for the behavior of light in different situations.2. Behavior of Light WavesLight waves can exhibit several important phenomena, including reflection, refraction, diffraction, and interference. When a light wave encounters a boundary between two different media, it may be reflected, refracted, or both. The laws of reflection and refraction describe how light waves behave at such boundaries, and they are fundamental to our understanding of optics.Diffraction is the bending of light waves around obstacles or through small openings, which leads to the spreading of light into a pattern of bright and dark regions. Interference is the interaction of multiple light waves, which can lead to the reinforcement or cancellation of the waves, producing a pattern of bright and dark fringes. These phenomena are important in many optical applications, such as the design of lenses, mirrors, and optical instruments.3. Polarization of LightPolarization is another important property of light waves, which describes the orientation of the oscillations of the electric and magnetic fields in the wave. Light waves can be polarized in different ways, including linear, circular, and elliptical polarization. Polarization has important applications in various optical technologies, such as 3D movie glasses, glare-reducing sunglasses, and liquid crystal displays (LCDs).4. Applications of OpticsOptics has many practical applications in various fields, including astronomy, microscopy, photography, telecommunications, and laser technology. In astronomy, telescopes and other optical instruments are used to study the universe and observe distant objects in the sky. In microscopy, optical techniques are used to visualize and analyze tiny structures and particles, such as cells and molecules.In photography, cameras and lenses are used to capture and record images using the principles of optics. In telecommunications, optical fibers are used to transmit and receive data at high speeds over long distances, enabling the internet and other communication networks. Laser technology is another important application of optics, with a wide range of uses in medicine, industry, and research.In conclusion, optics is a fascinating and important branch of physics that studies the behavior and properties of light. It covers a wide range of topics, including the nature of light, the behavior of light waves, and the applications of optics in various fields. Understanding the principles of optics is essential for many technological and scientific advancements, and it continues to be a vibrant and active area of research and innovation.。
麦克斯韦方程组英文
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麦克斯韦方程组英文The Maxwell's equations are a set of four fundamental equations in classical electromagnetism, which describe the behavior of electric and magnetic fields and their interactions with matter. These equations were formulatedby James Clerk Maxwell in the 19th century and played a crucial role in advancing our understanding of electromagnetism.The first equation is Gauss's law for electricity, which states that the electric flux through a closed surface is proportional to the total electric charge enclosed by the surface. Mathematically, it can be written as ∮E⋅dA=Q/ε0, where E is the electric field, dA is an infinitesimal area vector, Q is the total charge enclosed, and ε0 is the vacuum permittivity.The second equation is Gauss's law for magnetism, which states that the magnetic flux through a closed surface is always zero. This implies that there are no magnetic monopoles, and that magnetic field lines always form closed loops. Mathematically, it can be written as ∮B⋅dA=0,where B is the magnetic field.The third equation is Faraday's law of electromagnetic induction, which describes how a changing magnetic field induces an electric field. Mathematically, it can bewritten as ∮E⋅dl=−dΦB/dt, where E is the electric field, dl is an infinitesimal path element, ΦB is the magnetic flux, and t is time.The fourth equation is Ampère's law with Maxwell's addition, which relates the circulation of the magneticfield to the electric current and the rate of change of the electric field. Mathematically, it can be written as ∮B⋅dl=μ0I+μ0ε0(dΦE/dt), where B is the magnetic field, dlis an infinitesimal path element, μ0 is the vacuum permeability, I is the electric current, ΦE is theelectric flux, and t is time.这些方程组共同描述了电磁场的行为,是电磁学理论的基础。
电磁场与电磁波英文版第二版教学设计
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Electromagnetic Fields and Waves, Second EditionTeaching DesignIntroductionThis teaching design is intended for a university-level course on electromagnetic fields and waves, using the second edition of the textbook Electromagnetic Fields and Waves by Lorrn and Corson. The course is med at students majoring in physics and engineering.Course Objectives1.Understand the principles and laws of electromagnetism.2.Develop the ability to calculate electric and magneticfields in simple cases.3.Understand the propagation of electromagnetic waves in freespace and in various media.4.Develop the ability to analyze electromagnetic wave behaviorin different materials and structures.5.Apply the principles of electromagnetic fields and waves topractical problems in physics and engineering.Course OutlineWeek 1-2: Introduction to Electromagnetism•Electric charge and Coulomb’s law•Electric field and Gauss’s law•Electric potential and electric potential energy•Conductors, insulators, and dielectrics•Capacitance and electric energy storageWeek 3-4: Magnetic Fields and Forces•Magnetic field and Ampere’s law•Magnetism and magnetic materials•Magnetic forces on charged particles•Magnetic forces on current-carrying wires and loops•Magnetic energy and inductanceWeek 5-6: Time-Varying Fields and Maxwell’s Equations•Electromagnetic induction and Faraday’s law•Lenz’s law and electromagnetic forces•Maxwell’s equations and electromagnetic waves•Electromagnetic wave solutions and polarization•Reflection, refraction, and standing wavesWeek 7-8: Waveguides and Transmission Lines•Waveguides and resonators•Transmission lines and impedance•Smith charts and matching networks•Radiation and antennas•Applications to wireless communicationsTeaching MethodologyThe course will consist of lectures, problem sets, and laboratory experiments. Lectures will cover the fundamental principles and concepts of electromagnetic fields and waves, and will be supplemented by numerical examples and demonstrations. Problem sets will providestudents with opportunities to develop their problem-solving skills and gn deeper insights into concepts. Laboratory experiments will allow students to apply their theoretical knowledge to real-world situations and gn practical experience with electromagnetic equipment and measurement techniques.AssessmentAssessment will be based on the following criteria:•Short quizzes on lecture topics (10%)•Problem sets on course content (30%)•Laboratory reports on experiment results (30%)•Midterm exam on course material (15%)•Final exam on course material (15%)The grading scale will be based on the following scheme:•A: 90-100%•B: 80-89%•C: 70-79%•D: 60-69%•F: below 60%ConclusionThis teaching design provides an overview of the topics, objectives, and assessment for a course on electromagnetic fields and waves, using the second edition of the textbook Electromagnetic Fields and Waves by Lorrn and Corson. The course will cover the fundamental principles and laws of electromagnetism, as well as the propagation and behavior ofelectromagnetic waves in various media and structures. The course will use a combination of lectures, problem sets, and laboratory experiments to enhance students’ understanding and mastery of the subject matter.。
电磁场英文作文
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电磁场英文作文English:An electromagnetic field is a physical field produced by electrically charged objects. It affects the behavior of charged objects in the vicinity of the field. The electromagnetic field extends indefinitely throughout space and describes the electromagnetic interaction. This field is comprised of two types of energy: electric and magnetic. The electric field is created by electric charges, while the magnetic field is created by the movement of those charges. Electromagnetic fields are essential in our daily lives, as they are the basis for all electric and magnetic phenomena. They are used in various technologies such as radios, televisions, and microwave ovens, as well as in medical equipment like MRI machines.中文翻译:电磁场是由带电物体产生的物理场。
它影响附近的带电物体的行为。
电磁场无限地延伸于空间并描述了电磁相互作用。
这个场包含两种能量:电场和磁场。
电场由电荷产生,而磁场是由这些电荷的运动产生的。
9059年级下册物理电与磁的知识点
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9059年级下册物理电与磁的知识点Physics is a branch of science that deals with the nature and properties of matter and energy. 物理是研究物质和能量的性质和本质的一门科学。
It encompasses a wide range of topics, including mechanics, thermodynamics, electromagnetism, and optics. 它涵盖了广泛的主题,包括力学、热力学、电磁学和光学。
One of the key topics in physics is electricity and magnetism, which play a crucial role in our daily lives. 物理学中的一个关键主题是电和磁,它们在我们日常生活中起着至关重要的作用。
Understanding the principles of electricity and magnetism is essential for various applications, such as electrical engineering, electronics, and telecommunications. 理解电和磁的原理对于各种应用至关重要,比如电气工程、电子学和电信。
Electricity is a fundamental force in nature that is responsible for the flow of electric charge. 电是自然界的一种基本力量,负责电荷的流动。
It is created by the movement of electrons within a conductor, such as a wire. 它是由导体内电子的运动而产生的,比如金属导线。
大学物理:7-1 电荷 库仑定律
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处,在基态下,电子在半径r=0.529×10-10m的球面
附近出现的概率最大.试计算在基态下,氢原子内电子和 质子之间的静电力和万有引力,并比较两者的大小.引力
常数为G=6.67×10-11N﹒m2/kg2.
解: 按库仑定律计算,电子和质子之间的静电力为
F
1
4
e2 r2
1.60 1019 2 =8.89 109 0.529 1010 2 N
静电场
电场 强度
电势
电通量
高斯定理 环路定理
静电场 的基本
性质
与带电粒子 的相互作用
导体的静电平衡
电
电介质
电位移矢量
容
极化 介质中高斯定理
电 场 能
稳恒电场
要点:
1. 两条基本实验定律:库仑定律,静电力叠加原理。
2. ▲ 两个基本物理量:电场强度 E ,电势 U 。
3. ▲ 两条基本定理:静电场高斯定理,环路定理。 揭示静电场基本性质(有源场、保守场)。
0
=8.22 108 N
库仑定律
应用万有引力定律, 电子和质子之间的万有引力为
F
G
m1m2 r2
6.67
10
11
9.111031 0.529
1.67 10 1010 2
27
N
3.631047 N
由此得静电力与万有引力的比值为
Fe 2.26 1039 Fg
库仑定律
Fe 2.26 1039 Fg
的大小为
6.5105 8.6 105
F31 9.0 109
0.6 2
N 140N
力 F 31 沿x轴和y轴的分量分别为
Fx F31 cos 30 120N
万物原理英文版
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万物原理英文版The Principle of Everything1. The Law of Conservation of Energy: Energy cannot be created or destroyed, only converted from one form to another.2. The Law of Cause and Effect: Every action has an equal and opposite reaction.3. The Law of Universal Gravitation: Every object in the universe attracts every other object with a force that is directly proportional to their masses and inversely proportional to the square of the distance between them.4. The Law of Relativity: The laws of physics are the same for all observers, regardless of their relative motion.5. The Law of Entropy: The entropy (disorder) of an isolated system always tends to increase over time.6. The Law of Electromagnetism: Electric and magnetic fields are interconnected and can be generated by moving charges or changing electric currents.7. The Law of Quantum Mechanics: The behavior of particles at the atomic and subatomic level is governed by wave-particle duality and probabilistic nature.8. The Law of Evolution: Living organisms evolve and adapt to their environment through the process of natural selection.9. The Law of Conservation of Mass: Mass is conserved in any physical or chemical process, meaning that the total mass of a closed system remains constant.10. The Law of Thermodynamics: Energy can flow from one form to another, but it tends to dissipate over time, leading to a decrease in the availability of useful energy.These principles form the foundation of our understanding of the physical world and shape our scientific theories and technologies.。
林芝电气氧化炭氧化物橡胶接触器手持式操作手册说明书
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IM207406/2016REV00 LTP SERIES HAND HELD TIG(GTAW) TORCHES CE OPERATOR’S MANUALENGLISH GRAPHICS MAY VARYLINCOLN ELECTRIC EUROPE S.Lc/o Balmes, 89 - 80 2a, 08008 Barcelona, Spainwww.lincolnelectric.euEasy StartDownloadYou can download this manual: from /en-gb/support/Pages/operator-manuals-eu.aspxDeclaration of conformityLincoln Electric EuropeDeclares that the TIG torches:LTP17/18/18SC/20/26conform to the following directives:Low Voltage Equipment (2006/95/EC) Electromagnetic Compatibility (2004/108/EC)and has been designed in compliance with the following standards:EN 60974-74th May 2016Pietro TerranovaAccessories Product Manager EMEALincoln Electric Europe S.L, c/o Balmes, 89 – 8° 2a , 08008 Barcelona, Spain12/05For having choosen the QUALITY of the Lincoln Electric products.and Equipment fordamaged in shipment must be notified immediately to the dealer.in the table belowModel Name: ………………...…………………………….…….…………………………………………………………..Code & Serial number: ………………….………………………………….. ………………….…………………………………..Date & Where Purchased: ………………….………………………………….. ………………….…………………………………..ENGLISH INDEXSafety (1)Preparation and Operator Instructions (2)Specifications (4)Installation (5)Maintenance (7)WEEE (8)Spare Parts (8)Warranty Information (8)Safety01/11WARNINGThis equipment must be used by qualified personnel. Be sure that all installation, operation, maintenance and repair procedures are performed only by qualified person. Read and understand this manual before operating this equipment. Failure to follow the instructions in this manual could cause serious personal injury, loss of life, or damage to this equipment. Read and understand the following explanations of the warning symbols. Lincoln Electric is not responsible for damages caused by improper installation, improper care or abnormal operation.Preparation and Operator InstructionsGeneralThese high quality TIG welding torches were specifically developed for more delicate welding and easier handling.They are available in gas-cooled and water-cooled versions. If properly used and maintained, our welding torches are extremely durable. In order to ensure a long life cycle, please read these instructions carefully.This manual is only for the experienced user. Do not allow untrained persons to install, handle or maintain our LTP TIG welding torches. Welding torches must be checked regularly in order to guarantee optimum life expectancy.The user is fully responsible for possible defects arising out of misuse, inadequate maintenance, damage,poor repairs, or modifications by other parties than the original manufacturer or his authorised dealers.The welding torch is a component of a complete welding system. The torch will generate an electric arc when connected with the appropriate welding machine. Ensure that you read the weldingThe manufacturer reserves the right, whenever necessary and without prior notice, to amend these instructions as a result of clerical or printing errors, incorrect information, or the addition of improvements.Except for the tungsten electrode – which must be ordered separately – our welding torches are delivered ready for immediate connection to our welding machines.Before welding•Check the torch is firmly connected to welding machine.•Check the torch is fitted with the correct parts for task.•Check the parameters in the welding machine.•If water cooled: is the cooling unit properly working and is there sufficient coolant flow? •Has gas been tested to prevent contamination and / or to check gas pressure ?TIG operations•Set the tig torch to the required start position.•Ignite the arc with the on/off button (when torch is fitted with a gas valve (V-torch), open the gas valve and assure the gas coverage is available. After this, start the ignition by contacting work piece).•After ignition keep the torch at the start point until establish a weld pool.•Guide the torch constant during the whole seam length following the instructions.•Press the stop button at the end of the welding job (when torch is fitted with a gas valve (V-torch), lift the torch until the arc tears off. Then close the gas valve).•Continue to hold torch at final position for a few seconds to allow molten pool to solidify without atmospheric disturbances (shielded by gas flow).WARNING•Avoid contact with hot torch parts and work pieces.•The operator must wear protective clothing and adequate ventilation must be available.SpecificationsOperating Temperature -10°C ~ 55°C (14°F ~ 131°F) Storage Temperature -25°C ~ 55°C (-4°F ~ 158°F) Relative air humidity Up to 90% at a temperature of 20°C“Ergo” / “Flex Ergo” types“V” type (Valve)TECHNICAL DATA (*)17 Ergo/17V 18 Ergo /18 Flex Ergo18SC Ergo 20 Ergo 26 Ergo /26Flex Ergo/26VPower rating AC100A 230A 280A 165A 130A DC 140A 320A 400A 220A 180ADuty Cycle 35% 100% 100% 100% 35% Electrode Φ (mm) 1.0÷2.4 1.0÷4.0 1.0÷4.0 1.0÷3.2 1.0÷4.0 Torch lenght 4-8 mt 4-8 mt 4-8 mt 4-8 mt 4-8-12(**) mtVoltage class L L L L L Welding gas Argon DIN 32 526/1 Argon DIN 32 526/1 Argon DIN 32 526/1 Argon DIN 32 526/1 Argon DIN 32 526/1 Gas flow rate (lt/min) 7÷15 7÷20 7÷20 8÷22 7÷18 CoolingGas Water Water Water Gas Highest temperature cooling mediumat entry hose package -60°C60°C60°C-Minimum quantity of cooling flow - 1.0 lt/min 1.0 lt/min 1.0 lt/min - Lowest pressure of entry - 2.5 bar 2.5 bar 2.5 bar - Highest pressure of entry - 5.0 bar 5.0 bar 5.0 bar - Net weight (g) (4mt) 2025/1825 2515/2515 ---- 1715 2545/2545/2445 Net weight (g) (8mt) 3555/3395 4515/4515 4565 2915 4305/4305/4205 Net weight (g) (12mt)----/--------/------------6065/----/----(*) LTP 17/18/20/26 are also available with French lever (cylindric handle, only 8mt and std neck). Optional 3-button and potentiometer modules aren’t available for the French lever versions. (**) LTP26 12m is available only with Ergo handle and Fixed neckInstallationWARNINGAlso follow operating instructions provided with the welding machine. WARNING! The power source must be deactivated!Gas-cooled connectionConnecting power cable and gas hoseConnect the power cable and the gas hose to the appropriate connectors on the welding machine and ansure tight connections by properly affixing the couplings.ExceptionWhen torch is fitted with a gas valve (V-torch), connect separate gas hose to an external gascylinder. But before connecting it to the gas cylinder, open the gas bottle’s pressure regulator a few times briefly to flush away any dirt. After that, make the connection and tighten with a wrench. You can then set the desired pressure using the pressure regulator.The pressure will depend on the item to be welded and the gas cup size.Connecting switching cableConnect the welding torch plug into the appropriate socket on the welding machine, and check for a solid connection.Water-cooled connectionConnecting power cable and gas hoseConnect the power cable and the gas hose to the appropriate connectors on the welding machine and ansure tight connections by properly affixing the couplings.Connecting (blue) water inlet hose and (red) water outlet hoseConnect the blue water inlet hose and red water outlet hose by inserting gas nipple into theappropriate nipple receptors on the welding machine according to the colour markings. Ensure that the connections are solid.Connecting switching cableConnect the welding torch plug into the appropriate socket on the welding machine, and check for a solid connection.Read the instructions of your welding machine prior to use so as to be sure how to attach your welding torch.Read the instructions of your welding machine priorto use so as to be sure how to attach your weldingtorch.Colour coding switching cableThe LTP torches can be fitted to a large variety of welding machines according to the diagram below and according to the switching module functionality of the torch.SWITCH MODULE FUNCTION WIRE/COLOR MARKING1 button switch start/stop orange + brown3 button switch start/stop orange + browndown red + blackup yellow + black1 button switchwith potentiometer start/stop orange + brown potmeter red + black + yellowstart: start welding process stop: stop welding processup/down: increasing/decreasing welding current/browsing machine program (depends on machine) potmeter: stepless up/down functionLTP TIG welding torches are normally supplied with a single button switch.In order to inter-operate with the new generation of welding machines, LTP TIG welding torches can be fitted with optional 3-button switch and/or an integrated potentiometer.The following switching modules are available:(Dis)assembly of the LTP handle and switch module Single-button (works with standard 5 pins plug) Single-button with potentiometer (works with optional 6 pins plug) 3-button(works with standard5 pins plug)(1) (2) (3) (4) (5) (6)MaintenanceWARNINGBefore carrying out maintenance work: switch off power and gas supply.Check regularly the function of the torch. Make regularly maintenance work and cleaning. Maintenance and cleaning should be done only by authorized persons. Replace any damaged, deformed or worn parts immediately. If repairs are necessary contact your local Lincoln dealer.Check TIG welding torch if:• All parts are undamaged and in the correct place.• Electrode and fastening parts are undamaged and properly fastened.• If surface of tungsten electrode is not smooth, the electrode should be grinded. • Flow of shielding gas is free and even.• Gas nozzle is in good condition.Check cable assembly if:• Insulation of handle and torch cable are undamaged.• All power, coolant and gas connections are clean and fastened.• Leather and sheathing show no external damage such as cracks or (fire-) holes. • There are no sharp bends in torch cable (or hose).Tips for grinding the electrodeA properly grinded electrode determines the consistency of the current density and direction of the arc. Electrodes must always be ground in longitudinal direction. The type of electrode and angle of sharpening depends on the material you want to weld. For professional grinding please consult your local dealer.Purchase of wear partsThe most important and common wear parts are given in the tables on the following pages. For ordering or locating omitted components, please contact your local Lincoln dealer.Assembly front side of welding torchA) Place collet (1) in collet body (2) and screw these by hand on torch body (3) B) Screw ceramic cup (4) on collet body (2)C) Insert Tungsten electrode (5) from the rear; make sure electrode has sufficient length. D) Screw back cap (6) onto torch body (3) from rear.Maximum length of electrode depends on type of back cap. Important: • As a standard, the LTP TIG torches are not be supplied with tungsten electrodes. Contact your dealer for more info. • Electrode can be sharp! • Collet, collet body and tungsten electrode must have the same diameter.WEEE07/06 EnglishDo not dispose of electrical equipment together with normal waste!In observance of European Directive 2012/19/EC on Waste Electrical and ElectronicEquipment (WEEE) and its implementation in accordance with national law,electrical equipment that has reached the end of its life must be collected separatelyand returned to an environmentally compatible recycling facility. As the owner of theequipment, you should get information on approved collection systems from our localrepresentative.By applying this European Directive you will protect the environment and humanhealth!Spare Parts08/12 Part List reading instructions•Use the illustration of assembly page and the end of the catalogue to determine where the part is located for your particular code.•Do not use this part list for an item if its code number is not listed. Contact the Lincoln Electric Service Department for any code number not listed.First, read the Part List reading instructions above, then refer to the "Replacement Parts" chapter, that contains a picture-descriptive part number cross-reference.Warranty InformationLincoln will assume both the parts and labor expense of correcting defects during the warranty period. All warranty periods start from the date of purchase from Lincoln or Lincoln Authorized Distributor to the original End User.Warranty period is 90 days.。
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Electric and magnetic fields inside neurons and their impact upon the cytoskeletal microtubulesDanko Dimchev Georgiev 1, 21 Division Of Electron Microscopy, Medical University Of Varna, Bulgaria2 Department Of Emergency Medicine, Bregalnitsa Street 3, Varna, BulgariaIf we want to better understand how the microtubules can translate and input the information carried by the electrophysiologic impulses that enter the brain cortex, a detailed investigation of the local electromagnetic field structure is needed. In this paper are assessed the electric and the magnetic field strengths in different neuronal compartments. The calculated results are verified via experimental data comparison. It is shown that the magnetic field is too weak to input information to microtubules and no Hall effect, respectively QHE is realistic. Local magnetic flux density is less than 1/300of the Earth’s magnetic field that’s why any magnetic signal will be suffocated by the surrounding noise. In contrast the electric field carries biologically important information and acts upon voltage-gated transmembrane ion channels that control the neuronal action potential. If mind is linked to subneuronal processing of information in the brain microtubules then microtubule interaction with the local electric field, as input source of information is crucial. The intensity of the electric field is estimated to be 10V/m inside the neuronal cytoplasm however the details of the tubulin-electric field interaction are still unknown. A novel hypothesis stressing on the tubulin C-termini intraneuronal function is presented replacing the current flawed models (Tuszynski 2003, Mershin 2003, Hameroff 2003, Porter 2003) presented at the Quantum Mind II Conference held at Tucson, Arizona, 15-19 March 2003, that are shown in this presentation to be biologically and physically inconsistent.Foreword (4)Neurobiology (5)Brain cortex structure (5)Electromagnetic sensory input to the cortex (6)Neuronal morphology (8)The neuronal cytoskeleton (12)Electrodynamics (16)Right-handed coordinate systems (16)Vectors (17)Electric field (18)Physical and vector fluxes (20)Electric current (21)Magnetic field (23)Electromagnetic induction (26)Maxwell’s equations (27)Electromagnetic fields in vivo (31)Neuronal membranes as excitable units (31)Cable equation and dendritic modeling (33)Electric field in dendrites (36)Electric field structure under dendritic spines (41)Electric currents in dendrites (43)Magnetic field in dendrites (44)Electromagnetic field in soma (45)Axonal morphophysiology (46)The Hodgkin-Huxley model (48)Magnetic field in axons (52)Electric field in axons (53)Implications for microtubule function (54)No Hall effect in microtubules (54)Microtubule lattice structure (58)Problems in the ferroelectric model of microtubules (60)GTP hydrolysis and dynamic instability (63)The importance of the water microenvironment (65)Tubulin C-termini biological function (68)Post-translational modification of tubulin tails (71)Tubulin tail defects and cerebral pathology (73)Processing of information by brain microtubules (73)Elastic and piezoelectric properties of microtubules (77)Discussion (77)References (79)ForewordThe realization of this project was for the sake of elucidating the mechanisms of inputting the sensory information carried by the membrane potentials that enter the brain cortex and constructing biologically feasible model of subneuronal microtubule based processing of information.The electric currents are relevant stimuli eliciting conscious experience like memorization of past events (Wilder Penfield, 1954a; 1954b; 1955) and are used to restore the visual image perception in blind man via implanted in the occipital cortex electrodes linked to bionic eye-camera (Dobelle, 2000). The link between the EM field and the cytoskeletal microtubules however was not thoroughly understood. Indeed in the current models presented at the Quantum Mind II Conference, held at Tucson, Arizona, 15-19 March 2003, have been found severe biological and physical inconsistencies. The ferroelectric model (Tuszynski, 2003; Mershin, 2003) leads to extremely high electric field strength needed to polarize microtubules and does not take into account that the suggested α − βelectron hopping leads to conformational transitions that assemble - disassemble the microtubule. The same error is found in the Orch OR model (Hameroff, 2003a; 2003b) plus additional experimentally disproved predictions about the microtubule lattice, and too slow protein dynamics (25ms). The third model predicting topologically stabilized quantum states and anyons suggested by Porter (2003)depends on the magnetic field strength that is responsible for putative quantum Hall effect in the 2D electron layers presented on the microtubule surface. This idea is not realizable in vivo because of the extremely small magnetic field strength inside neurons assessed to be in the range 10–10- 107tesla and because of the millikelvin temperatures needed for QHE. In addition there is little or no data in the presented models how exactly microtubule conformations produce biologically important effects inside neurons.NeurobiologyBrain cortex structureThe brain cortex is the main residence of consciousness. All sensory stimuli are realized only when they reach the brain cortex and not before that! Nieuwenhuys (1994) outlines the origin and evolutionary development of the neocortex. A cortical formation is lacking in amphibians, but a simple three-layered cortex is present throughout the pallium of reptiles. In mammals, two three-layered cortical structures, i.e. the prepiriform cortex and the hippocampus, are separated from each other by a six-layered neocortex. Still small in marsupials and insectivores, this "new" structure attains amazing dimensions in anthropoids and cetaceans. Neocortical neurons can be allocated to one of two basic categories: pyramidal and nonpyramidal cells. The pyramidal neurons form the principal elements in neocortical circuitry, accounting for at least 70% of the total neocortical population. The evolutionary development of the pyramidal neurons can be traced from simple, "extraverted" neurons in the amphibian pallium, via pyramid-like neurons in the reptilian cortex to the fully developed neocortical elements designated by Cajal as "psychic cells".Typical mammalian pyramidal neurons have the following eight features in common: (1) spiny dendrites, (2) a stout radially oriented apical dendrite, forming (3) a terminal bouquet in the most superficial cortical layer, (4) a set of basal dendrites, (5) an axon descending to the subcortical white matter, (6) a number of intracortical axon collaterals, (7) terminals establishing synaptic contacts of the round vesicle/asymmetric variety, and (8) the use of the excitatory aminoacids glutamate and/or aspartate as their neurotransmitter. The pyramidal neurons constitute the sole output and the largest input system of the neocortex. They form the principal targets of the axon collaterals of other pyramidal neurons, as well as of the endings of the main axons of cortico-cortical neurons.Indeed, the pyramidal neurons constitute together a continuous network extending over the entire neocortex, justifying the generalization: the neocortex communicates first and foremost within itself!The neurons from different layers communicate via axo-dendritic synapses, which are chemical informational junctions that transfer information via neuromediator molecules. The neuromediator molecules released from the axonal terminal under depolarization (membrane firing; incoming electric impulse) bind to postsynaptic (dendritic) ion channels, modulate their ion conductivity and generate again electric impulses. Thus the electromagnetic events are essential in neuronal functioning, informational transfer and processing.Electromagnetic sensory input to the cortexThe experiments with implanting electrodes directly into the brain cortex suggest that the cortex is the residence for conscious experience. This notion is well supported with clinical data.William Dobelle, M.D. (2000)has helped a blind man to see again using electrodes implanted into his brain and connected to a tiny television camera mounted on a pair of glasses. Although he does not "see" in the conventional sense, he can make out the outlines of objects, large letters and numbers on a contrasting background, and can use the direct digital input to operate a computer. The man, identified only as Jerry, has been blind since age 36 after a blow to the head. Now 64, he volunteered for the study and got a brain implant in 1978. There has been no infection or rejection in the past 24 years.Scientists have been working since 1978 to develop and improve the software that enables Jerry to use the device as a primitive visual system. Jerry’s “eye” consists of a tiny television camera and an ultrasonic distance sensor mounted on a pair of eyeglasses. Both devices communicate with a small computer, carried on his hip, which highlights the edges between light and dark areas in the camera image. It then tells an adjacent computer to send appropriate signals to an array of 68 small platinum electrodes on the surface of Jerry's brain, through wires entering his skull behind his right ear. The electrodes stimulate certain brain cells, making Jerry perceive dots of light, which are known as phosphenes. Jerry gets white phosphenes on a black background. With small numbers of phosphenes you have (the equivalent of) a time and temperature sign at a bank. As you get larger and larger numbers of phosphenes, you go up to having a sports stadium scoreboard.If he is walking down a hall, the doorway appears as a white frame on a dark background. Jerry demonstrated by walking across a room to pull a woolly hat off a wall where it had been taped, took a few steps to a mannequin and correctly put the hat on its head. A reproduction of what Jerry sees showed crosses on a video screen that changed from black to white when the edge of an object passed behind them on the screen. Jerry can read two-inch tall letters at a distance of five feet. And he can use a computer, thanks to some input from his 8-year-old son, Marty. "When an object passes by the television camera ... I see dots of light. Or when I pass by it," Jerry says. The system works by detecting the edges of objects or letters. Jerry, currently the only user of the latest system, must move his head slightly to scan what he is looking at. He has the equivalent of 20/400 vision - about the same as a severely nearsighted person - in a narrow field. Although the relatively small electrode array produces tunnel vision, the patient is also able to navigate in unfamiliar environments including the New York City subway system.Another interesting fact is that lesions in the primary visual cortex cause amaurosis corticalis - a condition with decreased visual acuity or even blindness, but with normal pupillar reactions i.e. although there is subcortical neural processing of information, it is not realized because it does not enter the cortex. It can also be concluded that relevant stimulus for the cortical neural cells is the membrane potential, which is then converted into specific quantum states if the Q-mind hypothesis proves true!Neuronal morphologyThe morphology of a single neuron is relatively simple. In this study is presented a hippocampal pyramidal CA3 (cornu ammonis 3 region) neuron that is typical cortical pyramidal neuron. The neuron has body called soma and two types of projections: dendrites that input electrophysiologic information and axon branching into axonal collaterals that output information via neuromediator release (exocytosis) under membrane firing (depolarization).Fig. 1 Structure of hippocampal CA3 neuron. AD, apical dendrites; BD, basal dendrites; S, soma; AX, axon. From Eichler West et al. (1998).When cortical pyramidal cells are stained using the immunohistochemical methods we observe that long apical dendrites are extended toward the surface cortical layer and basal dendrites are extended in all directions in the area adjacent to the soma. Dendrites can be thought of as extensions of the cell body with maximal length ~ 1-2 mm in the largest neurons (Fiala & Harris, 1999), which provide increased surface area at much lower cell volumes. For example, 97% of the surface area of a motor neuron (excluding the axon) is dendritic (Ulfhake & Kellerth, 1981). The dendrites have 3.7x105 µm2 of surface area while occupying only 3x105µm3. To provide an equivalent surface, a spherical cell body would be 340 µm in diameter and consume 2x107 µm3. The fact that 80% of the surface area of proximal dendrites of motor neurons are covered with synapses (Kellerth et al., 1979) suggests that this increased surface area is indeed valuable for increasing the number of inputs to a neuron.The most common synaptic specializations of dendrites are simple spine s. Spines are protrusions from the dendrite of usually no more than 2 µm, often ending in a bulbous head attached to the dendrite by a narrow stalk or neck. Spine heads usually have diameter ~ 0.6 µm; when this diameter is exceeded we speak about mushroom spines. The spines are usually pedunculated(i.e. they have narrow neck) but sessile spines with no neck are also known. The total spine length for CA1 pyramidal neuron is 0.2-2µm, neck diameter 0.04-0.5µm, neck length 0.1-2µm, total spine volume 0.004-0.6µm3, total surface area of a single spine 0.1-4µm2, postsynaptic density (PSD) area 0.01-0.5µm2.Neurons are classified as spiny, sparsely spin y, and nonspiny (or smooth) according to the density of simple spines on their dendrites (Peters & Jones, 1984). Such a classification is complicated by the fact that different dendrites of a given neuron may exhibit widely different spine densities (Feldman & Peters, 1978). Even along the length of a dendritic segment, spine densities can vary widely. Nominally nonspiny dendrites often exhibit a few simple spines.Table I Dendrites in rat CA1 pyramidal cellDendritic type Number ofdendritesProximaldiameterBranchpointsDistaldiameterDendriteextendBasaldendrites5 1µm30 0.5-1µm 130µmStratumradiatum1 31µm 30 0.25-1µm 110µmStratummoleculare15 0.25-1µm 500µmThe cytoskeleton of dendrites is composed of microtubules, neurofilaments, and actin filaments. Microtubules are long, thin structures, approximately 25 nm in diameter, oriented to the longitudinal axis of the dendrite. In regions of the dendrite free of large organelles, they are found in a regular array at a density of 50-150 µm–2. Microtubules are typically spaced 80-200 nm apart, except in places where mitochondria or other organelles squeeze in between them. Microtubules are the “railroad tracks” of the cell and they play an important role in the transport of mitochondria and other organelles (Overly et al., 1996).The cell body (soma) is the trophic center of the neuron and in CA1 neuron has diameter ~ 21µm. The cell body (soma) contains the nucleus and the principal protein synthetic machinery of the neuron. Axons have essentially no ability to synthesize protein, since they do not contain ribosomes or significant amounts of RNA. Thus, axons depend entirely on proteins produced in the cell body, which are delivered into the axon by important transport processes. Dendrites do contain small amounts of both mRNA and ribosomes, and this protein synthetic machinery is thought to play an important role in dendritic function, but most of the proteins that are present in dendrites are transported from the cell body.Because of the large concentrations of ribosomes, neuronal cell bodies stain heavily with basic dyes such as thionin and cresyl violet, which are routine stains for neuropathological studies. In many of the larger neurons, thionin and cresyl violet stains reveal clumps of heavily stained material, termed Nissl bodies. Nissl bodies represent the stacks of rough endoplasmic reticulum visible at the electron microscopic level.The distribution of Nissl substance is an indication of the protein synthetic activity of the neuron. When conditions lead to decreases in protein synthesis, there are decreases in Nissl staining. For example, when neurons are axotomized, they often exhibit a response termed chromatolysis, which is characterized by a dispersal of Nissl substance. During the time that the Nissl substance is dispersed, protein synthesis is decreased. Neuronal cell bodies also contain a prominent Golgi apparatus, like other secretory cells. As in other cell types, an important function of the Golgi apparatus of neurons is terminal glycosylation of proteins synthesized in the rough endoplasmic reticulum.The axon is the output projection that branches into axonal collaterals that reach distant dendrites of target neurons. Study of CA3 -> CA1 axo-dendritic synapses shows that the synapses are formed at 2.7 µm intervals along the axons, the axonal shafts are 1.4 ± 1.2 µm long and the varicosities have oblong form and length – 1.1 ± 0.7 µm (Shepherd & Harris, 1998). It is also possible axo-axonal electric synapses known as gap junctions to account for ultrafast (200Hz) signalling between neurons. Axons contain microtubules, usually with closer spacing than in dendrites.The neuronal cytoskeletonThe neuronal cytoskeleton is protein lattice composed from microtubules, intermediary and actin filaments. It was conjectured that the neuronal microtubules are essential subneuronal processors of information i.e. they act as quantum computers that’s why in this study we will focus our attention on the interaction between the microtubules and the local electromagnetic field.Microtubules are hollow cylindrical tubes, of about 25 nm in diameter on the outside and 14 nm on the inside, whose walls are polymerized arrays of protein subunits. Their lengths may range from tens of nanometers during early assembly, to possible centimeters in nerve axons within large animals. The protein subunits assemble in longitudinal strings called protofilaments, 13 parallel protofilaments laterally align to form the hollow tubules. The protein subunits are peanut shaped dimers, which in turn consists of two globular proteins, monomers known as α− and β−tubulin.The α− and β−tubulin monomers are similar molecules with identical orientation within protofilaments and tubule walls. In the polymerized state of the MT, one monomer consists of 40% α-helix, 31% β-sheet and 29% random coil. Each monomer consists of about 500 aminoacids, is about 4nm x 4nm x 4nm and has a local polarity. Each dimer, as well as each MT, appears to have an electric polarity or dipole, with the negative end oriented towards the α−monomer and the positive end towards the β−monomer. The dipole character of the dimer originates from the 18 calcium ions bound within each β−monomer. An equal number of negative charges required for the electrostatic balance are localized near the neighboring α−monomer (Mavromatos et al., 2002).The cytoplasmic structural and dynamical organization of cells is due to the presence of networks of interconnected protein polymers, referred to as the cytoskeleton. The cytoskeleton consists of microtubules, actin microfilaments, intermediate filaments and an organizing complex, the centrosome with its chief component the centriole, built from two bundles of microtubules in a separated T-shape. The centrosomal microtubules are unstable and undergo intense dynamics. Much of the dynamic nature of microtubules is attributed to regulated growth and shrinkage of the polymer plus ends (dynamic instability) or to the addition of subunits at the plus end while they are simultaneously lost from the minus end (treadmilling).The first stage of microtubule formation is called nucleation. The process requires tubulin, Mg 2+ and GTP and also proceeds at 370C. This stage is relatively slow until the microtubule is initially formed. Nucleation of microtubule assembly can occur spontaneously in a solution of purified tubulin subunits, or it can be stimulated by addition of seeds. Several studies have examined the pathway of early assembly, and conclude that the crucial event in nucleation is formation and growth of a 2-D polymer, the microtubule wall. Investigation by Erickson & Stoffler (1996)shows that third type of tubulin subunit, namely γ−tubulin is important for nucleation. γ−tubulin forms spiral that extends a short length of straight protofilament, which serves as a stable seed for nucleation of a second protofilament. α/βsubunits form lateral bonds to the γ−tubulin protofilament, and longitudinal bonds to each other. When this second protofilament has achieved three consecutive α/βsubunits, growth is more favorable than disassembly and the microtubule should be nucleated. The second phase, called elongation proceeds much more rapidly. The α−and β−tubulin molecules join to form heterodimers. The heterodimers attach to other dimers to form oligomers, which elongate to form protofilaments. Each dimer carries two GTP molecules. However the GTP that appears to function binds to the β-tubulin molecules. When a tubulin molecule adds to the microtubule, theGTP is hydrolyzed to GDP. Eventually the oligomers will join to form the ringed microtubule. The hydrolysis of GTP of course is facilitated at a temperature of 370C and stopped at temperatures of 40C. As the oligomers assemble, they form a series of rings, 25 nm in diameter.In the cell itself, microtubules are formed in an area near the nucleus called aster. This is also called the microtubule organizing center(MTOC), or centrosome. Microtubules are polar with a plus end (fast growing) and a minus end (slow growing). Usually the minus end is the anchor point in the MTOC. The plus end carries the GTP molecules, which may be hydrolyzed to GDP. Hydrolysis is not necessary, however. Tests have shown that microtubules will form normally with nonhydrolyzable GTP analog molecules attached, however they will not be able to depolymerize.It should be stressed that in neurons the microtubule severing by specific enzyme called katanin(Quarmby, 2000) is important for the production of non-centrosomal microtubules, which are stable and thus good candidate for quantum computation. Ahmad et al. (1999) have shown that in neurons a large number of non-centrosomal microtubules is required for the growth and maintenance of neuronal processes.Injection of an anti-katanin antibody into neurons leads to an accumulation of centrosomal microtubules and a loss of neuronal processes, which indicates that centrosomal katanin, is important for the production of non-centrosomal microtubules primarily through severing of the microtubules near the centrosome. In the neurons the minus end might be capped, which would allow the persistence of centrosome-free microtubules (Rodionov et al., 1999).Recent computational study by Baker et al. (2001)has shown that the microtubules have electronegatively charged inner and outer surface and positively charge core. This result suggests existence of two 2-D electron layers (inner and outer) and interesting possibility for anyon formation. Anyons have been found in Nature and could exist in microtubules. They are 2D quasiparticles with partial spin made out of groups of electrons and are ideal candidates for fault-tolerant quantum computation (Porter, 2003; Kitaev, 1997; Mochon, 2003). According to Mitchell Porter (2003) there are four ways in which the microtubule has what it takes to be an anyonic medium: (1) it’s two-dimensional – necessary for anyons; (2) it’s a cylinder rather than a plane – should turn useless “abelian” anyons into useful “nonabelian” anyons; (3) it’s a hexagonal array of qubits – can form domain walls and anyonic defects; (4) the Fibonacci numbers define the geometry of the microtubule. The dependence of the topological anyon model on the magnetic field strength and putative quantum Hall effect (QHE) however is detrimental for its applicability in vivo.Fig. 2 Microtubule sandwich structure. Cartesian coordinate system attached to the microtubule. The inner and the outer 2D surface of the microtubule are electronegatively charged (red), while the core is electropositive (blue).ElectrodynamicsRight-handed coordinate systemsIn order to investigate the electromagnetic field structure it is appropriate to be acquainted with the basic mathematical definitions and physical postulates in classical electrodynamics. First it is worth pointing out that a quantity is either a vector or a scalar. Scalars are quantities, which are fully described by a magnitude alone. Vectors are quantities, which are fully described by both a magnitude and a direction. Because we will work mostly with vectors we have to define what is positive normal to given surface s, what is positive direction of given contour Γ and what is right-handed coordinate system?Right-handed coordinate system Oxyz is such system in which if the z-axis points towards your face the counterclockwise rotation of the Ox axis to the Oy axis has the shortest possible path. The positive normal +n of given surface s closed by contour Γ is collinear with the Oz axis of right-handed coordinate system Oxyz whose x- and y-axis lie in the plane of the surface. The positive direction of the contour Γis the direction in which the rotation of x-axis to the y-axis has the shortest possible path.Fig. 3 Direction of the positive normal and right handed coordinate system.VectorsBecause we will work with vectors it should be noted that there are two types of multiplication of vectors - the dot product and the cross product . Geometrically, the dot product of two vectors is the magnitude of one times the projection of the other along the first. The symbol used to represent this operation is a small dot at middle height (·), which is where the name dot product comes from. Since this product has magnitude only, it is also known as the scalar product .(1)cos A B AB β⋅=G Gwhere β is the angle between the two vectors.Geometrically, the cross product of two vectors is the area of the parallelogram between them. The symbol used to represent this operation is a large diagonal cross (×), which is where the name cross product comes from. Since this product has magnitude and direction, it is also known as the vector product .(2)β×=G G G sin A B AB n where the vector G n is a unit vector perpendicular to the plane formed by the two vectors. The direction of G n is determined by the right hand rule .The right hand rule says that if you hold your right hand out flat with your fingers pointing in the direction of the first vector and orient your palm so that you can fold your fingers in the direction of the second vector then your thumb will point in the direction of the cross product.Electric fieldThe electromagnetic field is composed from electric and magnetic field. The electric field could be described via vector field of the electric intensity E G . The electric intensity is defined as the ratio of the electric force E F G acting upon charged body and the charge q of the body.(3)0lim E E q F dF E q dq ∆→∆==∆G G GIt should be noted that the electric field is potential field – that is the work W along closed contour Γ is zero.(4)0W dW ΓΓ==∫v (5)0E F dl Γ⋅=∫G G vwhere l is the length of the contour Γ.Every point from the electric field has electric potential V defined with the specific (for unit charge) work needed to carry a charge from this point to infinity. The electric potential of point c of given electric field has potential V defined by:(6)c V E dl K ∞=⋅+∫G Gwhere 0V K ∞==. The electric potential difference between two points 1 and 2 defines voltage V ∆ (synonyms: electric potential, electromotive force, potential, potential difference, potential drop).。