Lecture 3 Assignment 1. In addition to reading through Chapter 1 , read one paper on the exposures that you get from a low frequency source and write.

Slides:



Advertisements
Similar presentations
Chapter 22 Electromagnetic Waves. Units of Chapter 22 Changing Electric Fields Produce Magnetic Fields; Maxwell’s Equations Production of Electromagnetic.
Advertisements

PH0101 Unit 2 Lecture 4 Wave guide Basic features
Radio Frequency Fundamentals Wireless Networking Unit.
ECEN5341/4341Bioelectromagnetics Spring 2015 Frank S. Barnes Contact Info: (303) ECOT 250
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Electromagnetic induction Lenz’s law Faraday’s law The nature of electromagnetic.
Antennas Lecture 9.
Electromagnetic Wave Theory
AERIALS AND RADIO FREQUENCY PROPAGATION By Farhan Saeed.
Bioelectromagnetics ECEN 5341/4341 Lecture 3 1. Environmental and Occupationally Encountered Electromagnetic Fields 2. The objective is to get a feel for.
Chapter 5 Lecture 10 Spring Nonlinear Elements 1. A nonlinear resistance 2. A nonlinear reactance 3. A time varying element in you circuit or system.
DTR/H&D Joint Venture1 Radio Frequency Exposure and Compliance Issues for a Shortwave May 2008 Matthew W. Folkert, MSEEE Stephen S. Lockwood, P.E. dTR/H&D.
Waves? Chapter 17 Notes.
RF Safety Measurements IOSH meeting Emley 4 th July
Electromagnetic Waves Chapter Introduction: Maxwell’s equations Electricity and magnetism were originally thought to be unrelated Electricity.
Chapter 9 Electromagnetic Waves. 9.2 ELECTROMAGNETIC WAVES.
TELECOMMUNICATIONS Dr. Hugh Blanton ENTC 4307/ENTC 5307.
Radio Transmission Music and words are sent to your radio by radio waves. The metal antenna of your radio detects radio waves. As the electromagnetic.
© 2010 Pearson Education, Inc. PowerPoint ® Lectures for College Physics: A Strategic Approach, Second Edition Chapter 25 Electromagnetic Induction and.
Chapter 13 Sound. Section 1 ► ► Electromagnetic waves   made by vibrating electric charges and can travel through space. ► ► Electric and magnetic.
Electromagnetic Waves
Author: Bill Buchanan Wireless LAN Unit 6 Radio and RF Wireless LAN Unit 6 Radio and RF.
Certified Wireless Network Administrator (CWNA) PW0-105 Chapter 2 Radio Frequency Fundamentals.
ECE 3317 Prof. David R. Jackson Notes 15 Plane Waves [Chapter 3]
Electromagnetic Waves and Their Propagation Through the Atmosphere
ECE 1100: Introduction to Electrical and Computer Engineering Notes 10 Antennas Transmission and Reception of waves Wanda Wosik Associate Professor, ECE.
Bellwork What is a transformer? What is a transformer? A device for increasing or decreasing voltage through electromagnetic induction A device for increasing.
ultraviolet radiation
Physics 102: Lecture 14, Slide 1 Resonance Electromagnetic Waves Today’s lecture will cover Textbook Sections 21.6, 22.1, 4-5, 9 Physics 102: Lecture.
Lecture 3 Assignment 1. In addition to reading through Chapter 1 and starting chapter 2 read one paper on the exposures that you get from a low frequency.
The Plain Facts About Electric System Radio Signals An Advanced Mesh Network SmartMeter™ electric meters include two low power radio frequency (RF) transmitters.
WIRELESS CHARGING Presented by: K.MAHESH (08T81A1236)
LC Circuit Section 22.5 There is a characteristic frequency at which the circuit will oscillate, called the resonance frequency.
LC Circuit Section 22.5 There is a characteristic frequency at which the circuit will oscillate, called the resonance frequency.
DIATHERMY Diathermy was once one of the most popular modalities used in rehab. Became less popular with development of more modern tech like US and because.
20 Overview current  magnetic field magnetic field  current
The Electromagnetic Spectrum
The signal range radio decametre
EELE 5490, Fall, 2009 Wireless Communications
How does a klystron work? TE-MPE Section Meeting Karolina Kulesz
Chapter 8 Antennas Propagation Dave Piersall, N6ORB.
ECEN5341/4341Bioelectromagnetics
Lecture 19 Electromagnetic Waves.
ECEN5341/4341 Spring 2017 Lecture 2 January 20,2017.
Electromagnetic Waves
The Electromagnetic Spectrum
Electromagnetic Waves & The Electromagnetic Spectrum
Chapter 3– Electromagnetic Waves
The Earth is {image} meters from the sun
L 30 Electricity and Magnetism [7]
From last time… Faraday: Inductance: flux = (inductance) x (current)
Lecture 4: Wave Propagation Concept
Lecture 4 January 25, 2017 Two Reference Formats.
Chapter 13: EM Waves Section 3: Radio Communication
Lecture 3 Assignment 1. In addition to reading through Chapter 1 , read one paper on the exposures that you get from a low frequency source and write.
Electromagnetic Dosimetry
Phys102 Lecture 20 Electromagnetic Waves * (skipped)
L 30 Electricity and Magnetism [7]
Electromagnetic Waves
ELECTROMAGNETIC WAVES Radio Communication
L 30 Electricity and Magnetism [7]
ECEN5341/4341 Spring 2019 Lecture 2 January 16,2019.
An Overview of Antennas:
Anything that can carry information from a source to a destination.
General Licensing Class
Lecture 33: FRI 03 APR Ch.33.1–3,5: E&M Waves
Electromagnetic Waves
Electromagnetic Waves
L 30 Electricity and Magnetism [7]
ANTENNA THEORY by Constantine A. Balanis Chapter 2.13 –
PH0101 Unit 2 Lecture 4 Wave guide Basic features
Presentation transcript:

Lecture 3 Assignment 1. In addition to reading through Chapter 1 , read one paper on the exposures that you get from a low frequency source and write up a one page summary. Also you should start looking for papers on a topic you want to follow up on and write a one page summary of it. 2. This is due Wednesday

Bioelectromagnetics ECEN 5341/4341 Lecture 3-4 1. Environmental and Occupationally Encountered Electromagnetic Fields 2. The objective is to get a feel for the size of both the natural fields we are exposed to and the size of the fields that we are now exposed to resulting from the wide spread use of electricity.

Atmospheric Sources 1. Static and ELF (0 to 3khz) 2. Earth’s Static Magnetic Fields range from 24μT to 65μT with variation up to about 1μT with the Northern Lights over several minutes 3. Electric fields Static 100 to 300V/m with the earth negative. Up to 100kV/m in thunderstorms.

Natural EM Power Density at the Earths Surface

B Field for Underwater Cable Normal load 400A shielded so no E field outside

High Voltage AC Lines Standards in US limit Fields to 1 to 5kV/m

Magnetic fields from Power Lines as a Function of Distance

The Effects of Power Pole Configurations and Phasing on Magnetic Fields

1

Some Typical Magnetic and Electric Field Strengths vs Some Typical Magnetic and Electric Field Strengths vs. Distance (Error 1mG=0.1µT)

Fourier Spectrum of A Current Wave Form

Typical Magnetic Field Exposure Levels At Home

1

Variations with time of Day

Variations in Magnetic Field Exposures Over the Course of a Day

Some Current Wave Forms

The Fourier Spectra of Figure 1.7

Magnetic Fields Around Appliances

1

Wave Shapes Near Fluorescent Light

Common Exposures

Exposures on Electric Trains

Electric Field Scaling and Induced Currents

Induced Electric Fields

A More Complete Model

1

Electric and Magnetic Induced Current Densities

Internally Generated Voltages

1

IF and RF Exposure Measurements Intermediate Frequencies, IF 3kHz 10MHz Radio Frequencies, RF, 10MHz 300GHz These are approximate frequency ranges and overlap. Bio-effects standards below 10MHz are set on nerve stimulation . Above 10MHz they are set on the basis of heating and temperature rise of ½ oC As the temperature rise depends on the shape of the biological material, the conductivity, the dielectric constant, the incident power density, frequency and time we go to other measurements that are related but easier to measure.

Measureable Quantities Power density , PD, S in watts/m2 Electric Fields in V/m Specific Absorption Rate SAR Magnetic field H in A/m Magnetic Flux Density B in Tesla/m2 In general the power emitted from a source decreases as 1/rn at large distances from the source. In the far field n=2 or for r >>λ and free space.

Some Common Transmitters.

Sources of Intermediate and Radio Frequency Fields 1. Scanners , Libraries, Airport Security 920MHz , B = 10µT and Deactivate at 50-60Hz 500µT 2. Video Display Terminals, VDT, Cathode Ray Tubes CRT Up to 20KV inside the Tube, ≈10V/m at 0.5m

Computer Display Fields 1

RF Sources 2. RF heaters for sealing plastic etc. 3. RF Transmission Short Wave 2 -27MHz 3-20V/m at 10’s of meters. 4. Radio TV 5. Base Stations and Cell Phones, WiFi

RF and Microwave Sources 1 Microwave oven leakage 20 V/m (at an average distance of 20 cm) (Mantiply et al., 1997; Plets et al., 2016) 2 Dielectric Heaters 27 MHz, average E-field levels around 400 V/m and maximum values up to 2,000 V/m (Hitchcock and Patterson, 1995). Magnetic fields of approximately 1 A/m are also present around the sealer. 3. Plastic heaters Typical frequencies used by these devices range from 4 to 50 MHz. Mean exposure levels range from 30 to 300 V/m for electric fields and 0.1 to 0.7 A/m for magnetic fields (Joyner and Bangay, 1986; Stuchly et al., 1980)

RF and Microwave Sources Induction heaters use eddy currents to heat metals or semiconductors by generating a strong alternating magnetic field inside a coil. Frequencies in the RF range can reach 27 MHz although lower frequency units (50 Hz) are also commonly used, which produce stronger magnetic fields with deeper penetration. Magnetic field mean exposure levels associated with RF units are about 0.6 A/m at the operator position, where mean electric field levels are about 50 V/m. Lower frequency units can lead to higher exposure levels around the operator, with magnetic field mean exposures about 5 A/m and electric field mean levels about 300 V/m (Allen et al., 1994; Cooper, 2002; Floderus et al., 2002; Mantiply et al., 1997)

Diathermy Devices The most common technologies used are continuous or pulsed shortwave (13.56 or 27.12 MHz) and microwave (915 MHz or 2.45 GHz) diathermy. Average electric field levels at about one meter from the source are approximately 60 V/m for pulsed shortwave devices and 300 V/m for continuous shortwave systems. Average magnetic field levels are about 0.20 and 0.70 A/m, respectably. However, maximum exposure levels can reach up to 5,000 V/m for electric fields and 10 A/m for magnetic fields (Allen et al., 1994; Mantiply et al., 1997; Martin et al., 1990; Mild, 1980; Shah and Farrow, 2013; Stuchly et al., 1982).

Cell Phone 1. Base station transmitting antennas are formed of vertical arrays of collinear dipoles phased to give a narrow beam width (typically between 7 and 10 degrees). 2. Mean electric fields of an operator can range from around 0.5 V/m, while working on the ground near the mast, to around 13 V/m, while working on the mast (Cleveland et al., 1995; Cooper et al., 2004) Mean electric field strength values are around 500 V/m near the antenna, although maximum levels up to 1,000 V/m are possible (Bernhardt and Matthes, 1992; Mantiply et al., 1997). Mean magnetic field strength levels are around 0.2 A/m, but maximum levels can reach up to 1 A/m (Vermeeren et al., 2015).

RF Environments The majority of measurements tend to be below 1 V/m and only around 0.1% are above 20 V/m. The strictest reference level established by this legislation for environmental (residential) exposure is 28 V/m, which corresponds with the limit set for the 10-400 MHz frequency, typically associated with FM radio and VHF TV broadcasting.

TV and Base Stations

Exposure Levels 1. US average about 50µW/m2 to 100µW/m2 2. We have measure E =1 to 2 V/m in Boulder, peak power density < 10 mW/m2 3. Peak Power from transmitter about50 KW 4. Radar Peak at Megawatts, over the horizon

Frequencies