Understanding, Finding, & Eliminating Ground Loops
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Filtering and Suppressing Transients
Another EMC resource from EMC Standards EMC techniques in electronic design Part 3 - Filtering and Suppressing Transients Helping you solve your EMC problems 9 Bracken View, Brocton, Stafford ST17 0TF T:+44 (0) 1785 660247 E:[email protected] Design Techniques for EMC Part 3 — Filtering and Suppressing Transients Originally published in the EMC Compliance Journal in 2006-9, and available from http://www.compliance-club.com/KeithArmstrong.aspx Eur Ing Keith Armstrong CEng MIEE MIEEE Partner, Cherry Clough Consultants, www.cherryclough.com, Member EMCIA Phone/Fax: +44 (0)1785 660247, Email: [email protected] This is the third in a series of six articles on basic good-practice electromagnetic compatibility (EMC) techniques in electronic design, to be published during 2006. It is intended for designers of electronic modules, products and equipment, but to avoid having to write modules/products/equipment throughout – everything that is sold as the result of a design process will be called a ‘product’ here. This series is an update of the series first published in the UK EMC Journal in 1999 [1], and includes basic good EMC practices relevant for electronic, printed-circuit-board (PCB) and mechanical designers in all applications areas (household, commercial, entertainment, industrial, medical and healthcare, automotive, railway, marine, aerospace, military, etc.). Safety risks caused by electromagnetic interference (EMI) are not covered here; see [2] for more on this issue. These articles deal with the practical issues of what EMC techniques should generally be used and how they should generally be applied. Why they are needed or why they work is not covered (or, at least, not covered in any theoretical depth) – but they are well understood academically and well proven over decades of practice. -
Using Ferrite Beads Keep RF out of TV Sets, Telephones, VCR's Burglar Alarms and Other Electronic Equipment
Using Ferrite Beads Keep RF Out of TV Sets, Telephones, VCR's Burglar Alarms and other Electronic Equipment RFI and TVI have been with us for a long time. Now we have microwave ovens, VCR's and many other devices that do wrong things when they pick up RF. There are several ways to tackle the problem but most of them involve opening the affected equipment and adding suppressor capacitors, filters, and other circuit modifications. Unfortunately there is a serious disadvantage associated with this approach. Any modifications made to domestic entertainment equipment can - and often are - blamed for later problems that arise in it. Modifying your own equipment is not so bad, but taking a soldering iron to your neighbor's stereo is risky. An alternative approach is to use ferrite beads to reduce the amount of RF entering the equipment. If the equipment is in a metal box, or even if it's in a plastic box, if RF is prevented from entering the box on the antenna lead, the power cable, the speaker leads, the phono pickup leads, and on any other wires entering the box, it is possible to solve the problem without any modification to the equipment. Ferrite beads just slip over the wires and stop RF from going in. Ferrite beads are made of the same materials as the toroid cores used in broadband transformers but are used at much higher frequencies. For example, ferrite Mix 43 is used for tuned circuits in the frequency range 0.01 to 1 MHz. It is efficient and losses are low. -
Chapter 21 Some Aspects of the Balun Problem
Chapter 21 Some Aspects of The Balun Problem (Adapted from QST, March 1983) type baluns which prove that with a 50-ohm resis• tive load, the transformers in typical 1:1 or 4:1 Sec 21.1 Introduction baluns do not yield a true 1:1 or 4:1 impedance transfer ratio between their input and output termi• nals. This is because of losses, leakage reactance, hy all the mystery surrounding baluns? and less than optimum coupling. My findings have Here's some straight talk to dispel the been substantiated by the work of the late John rumors! The balun—to use, or not to W Nagle, K4KJ (Ref 80). Furthermore, the imped• use—is one of the hottest topics in amateur radio. ance-transfer ratio of such baluns degrades even Because certain aspects of the connection between a further when used with an antenna that is reactive coaxial feed line and a balanced antenna have been from operation away from its resonant frequency. ignored, misunderstanding still exists concerning This degradation of impedance transfer associated the function of baluns. Many commercial baluns with transformer-type baluns poses no serious embody some form of impedance transformer, pro• operational problems. However, SWR curves plot• moting our tendency to misconstrue them as little ted from measurements of an antenna using such a more than a matching device, while their primary balun differ significantly from those using a choke function is to provide proper current paths between balun that has no impedance-transfer error. Thus, balanced and unbalanced configurations. when a precision bridge is used to measure anten• To help clarify the misunderstanding, this chap• na impedance (R + y'X), the data will be erroneous ter explains some of the undesirable effects that with either a transformer-type balun in the circuit, occur when a balun is not used, and some that or with no balun at all. -
Considerations for Instrument Grounding Many People Have Heard of the Term "Grounding", but Few Fully Understand Its Meaning and Importance
TECHNICAL OVERVIEW Considerations for Instrument Grounding Many people have heard of the term "grounding", but few fully understand its meaning and importance. Sometimes, even experienced electricians do not treat grounding as a serious issue. The impact of an incorrect or absent grounding ranges from noise interference. resonance or humming during the use of electrical equipment to the worst case where electricity leakage through the chassis causes personal injury or damage to instrument components. Grounding, therefore, is a very practical issue that should be dealt with properly. For those who operate electrical equipment frequently, a complete understanding of grounding theories and applications is necessary in order to become a best-in-class technician. In the eighteenth century, Benjamin Franklin performed the famous kite experiment to observe how lightning in the sky was conducted to the earth. This experiment led to the invention of lightning rods to avoid lightning strikes. From then on, people began to realize that the vast ground under our feet is a huge electrical conductor. It may not be the best conductor, but it is certainly a good one. It is so enormous in size that it can sustain a tremendous amount of current. That is why the voltage level of the ground is set to be zero. Safety regulations require that all metal parts which do not carry electricity should be kept at zero or the earth voltage level. There are several reasons for grounding. Some are for safety purposes, and some are for maintaining circuit stability. The following are some examples: – Power system grounding: As you can see in Figure 1. -
How to Use a Multimeter and Build a Simple Circuit
How to use a Multimeter and Build a Simple Circuit Components: 3 assorted resistors, 4 assorted batteries, 3 assorted LEDs, 1 SPST toggle switch, 1 DPDT knife switch, fuse, motor Equipment and tools: Safety Glasses, 4AA battery pack, alligator clips, multimeter All exercises require safety glasses over your eyes, all the time! A multimeter is an electronic measuring instrument that combines several measurement functions in one unit. A typical multimeter includes basic features such as the ability to measure voltage, current, and resistance. 1. Use a multimeter to test the voltage on an assortment of batteries. [Expected voltage is the voltage stamped on the battery.] Set multimeter to The black lead goes in the COM port, the red lead is in the V port. Battery Size Expected Voltage Measured Voltage Good or Bad? C size 1.5 V 1.3 V Bad 2. Use your multimeter to measure the voltage of your 4-AA battery pack. What is the voltage: _____________. These batteries are in series and their voltage is cumulative. 3. Use a multimeter to measure the resistance of the 3 resistors. After measuring the value, verify that the resistor is within +- tolerance. Set multimeter to The black lead goes in the COM port, the red lead is in the V port. Expected Measured Resistor Band Colors Resistance Percentage OK? Resistance (read code) orange, orange, brown 330Ω 328Ω 1 MATE Center 2016 Funding by the National Science Foundation. www.marinetech.org 4. Create a circuit to light up your LED. Using a 4-AA battery pack, alligator clips, your red LED and resistors, create a circuit like the one shown below. -
Variable Capacitors in RF Circuits
Source: Secrets of RF Circuit Design 1 CHAPTER Introduction to RF electronics Radio-frequency (RF) electronics differ from other electronics because the higher frequencies make some circuit operation a little hard to understand. Stray capacitance and stray inductance afflict these circuits. Stray capacitance is the capacitance that exists between conductors of the circuit, between conductors or components and ground, or between components. Stray inductance is the normal in- ductance of the conductors that connect components, as well as internal component inductances. These stray parameters are not usually important at dc and low ac frequencies, but as the frequency increases, they become a much larger proportion of the total. In some older very high frequency (VHF) TV tuners and VHF communi- cations receiver front ends, the stray capacitances were sufficiently large to tune the circuits, so no actual discrete tuning capacitors were needed. Also, skin effect exists at RF. The term skin effect refers to the fact that ac flows only on the outside portion of the conductor, while dc flows through the entire con- ductor. As frequency increases, skin effect produces a smaller zone of conduction and a correspondingly higher value of ac resistance compared with dc resistance. Another problem with RF circuits is that the signals find it easier to radiate both from the circuit and within the circuit. Thus, coupling effects between elements of the circuit, between the circuit and its environment, and from the environment to the circuit become a lot more critical at RF. Interference and other strange effects are found at RF that are missing in dc circuits and are negligible in most low- frequency ac circuits. -
Intermediate Answer Key Chapter 19: Electrical Circuits
CK-12 Physics Concepts - Intermediate Answer Key Chapter 19: Electrical Circuits 19.1 Series Circuits Review Questions 1. There are three 20.0 Ohm resistors connected in series across a 120 V generator. a. What is the total resistance of the circuit? b. What is the current in the circuit? c. What is the voltage drop across one of the resistors? 2. A 5.00Ω, a 10.0Ω, and a 15.0Ω resistor are connected in a series across a 90.0 V battery. a. What is the equivalent resistance of the circuit? b. What is the current in the circuit? c. What is the voltage drop across the 5.00Ω resistor? 3. A 5.00Ω and a 10.0Ω resistor are connected in series across an unknown voltage. The total current in the circuit is 3.00 A. a. What is the equivalent resistance of the circuit? b. What is the current through the 5.00Ω resistor? c. What is the total voltage drop for the entire circuit? Answers 1. a. Using 푅푇 = 푅1 + 푅2 + 푅3 ∶ 20Ω + 20Ω + 20Ω = 60Ω ∶ 퐑퐓 = ퟔퟎ훀 푉 120푉 b. Using 퐼 = ∶ = ퟐ푨 푅 60Ω c. Using 푉 = 퐼푅 ∶ (2퐴)(20Ω) = ퟒퟎ푽 (this is the same for each resistor) 2. a. Using 푅푇 = 푅1 + 푅2 + 푅3 ∶ 5Ω + 10Ω + 15Ω = 30Ω ∶ 퐑퐓 = ퟑퟎ훀 푉 90푉 b. Using 퐼 = ∶ = ퟑ푨 푅 30Ω c. Using 푉 = 퐼푅 ∶ (3퐴)(5Ω) = ퟏퟓ푽 3. a. Using 푅푇 = 푅1 + 푅2 ∶ 5Ω + 10Ω = 15Ω ∶ 퐑퐓 = ퟏퟓ훀 1 푉 45푉 b. Using 퐼 = ∶ = ퟑ푨 푅 15Ω c. Using 푉 = 퐼푅 ∶ (3퐴)(15Ω) = ퟒퟓ푽 19.2 Parallel Circuits Review Questions 1. -
Differential and Common Mode Noise Differential and Common Mode Noise 26
This is the PDF file of text No.TE04EA-1. No.TE04EA-1.pdf 98.3.20 4. Other Filters 4.1. Differential and Common Mode Noise Differential and Common Mode Noise 26 ■ Differential mode noise ■ Suppression method of differential mode noise Signal Signal source source Load Noise Noise Load source N source N ■ Common mode noise ■ Suppression method of common mode noise (1) Signal Stray source capacitance Signal Suppresses noise. Stray source capacitance Noise source Load Noise N source N Load Stray Stray capacitance capacitance Reference ground surface Reference ground surface ■ Suppression method of common mode noise (2) Signal source Noise Load source N Line bypass capacitor Metallic casing Reference ground surface Noise is classified into two types according to the conduction are installed on all lines on which[Notes] noise is conducted. mode. In the examples shown above, the following two suppression The first type is differential mode noise which is conducted on methods are applied. the signal (VCC) line and GND line in the opposite direction to 1. Noise is suppressed by installing an inductor to the signal line each othe. This type of noise is suppressed by installing a filter on and GND line, respectively. the hot (VCC) side on the signal line or power supply line, as 2. A metallic casing is connected to the signal line using a mentioned in the preceding chapter. capacitor. Thus, noise is returned to the noise source in the The second type is common mode noise which is conducted on following order; signal/GND lines ➝ capacitor ➝ metallic all lines in the same direction. -
Use of Ferrites in EMI Suppression
The Use Of Ferrites In EMI Suppression USE OF FERRITES Properties Of Ferrites Introduction Ferrites are a class of ceramic ferromagnetic ma- 600 ohms, and becomes essentially resistive above terials that by definition can be magnetized to 100 MHz. When used as EMI filters, ferrites can produce large magnetic flux densities in response thus provide resistive loss to attenuate and dissi- to small applied magnetization forces. Originally re- pate (as minute quantities of heat) high frequency ferred to as “magnetic insulators,” ferrites were first noise while presenting negligible series impedance used as replacements for laminated and slug iron to lower frequency intended signal components. core materials in low loss inductors intended for use When properly selected and implemented, ferrites above 100 kilohertz (kHz). At these frequencies, can thus provide significant EMI reduction while re- laminated and slug iron are plagued by excessive maining “transparent” to normal circuit operation! For eddy current losses whereas the high volume re- high frequency applications, ferrites should be sistivity of ferrite cores limit power loss to a fraction viewed as frequency dependent resistors. Since of other core materials. Today, Steward ferrites are they are magnetic components that exhibit signifi- the core material of choice for modern high density cant (and useful) loss over a bandwidth of over 100 switch mode power supply and pulse transformer MHz, ferrites can be characterized as high fre- design. quency, current operated, low Q series loss elements. Whereas a purely reactive (i.e., com- Fundamental Properties posed only of inductors and capacitors) EMI filter While frequently nicknamed “magic beads” in may induce circuit resonances and thus establish marketing literature, EMI suppression ferrites are additional EMI problem frequencies, lossy ferrites actually well understood magnetic components. -
Shielding of Electronic Traffic Control Equipment
l l 1 I i l I i l l NATToNAL coopERArrvE HrcHwAy RESEARcH ri::ååi 317 TRANSIENT PROTECTION, GROUNDING, AND SHIELDING OF ELECTRONIC TRAFFIC CONTROL EQUIPMENT H. W. DENNY and J. p. ROHRBAUGH Georgla Tech Research lnstitute Georgia lnstitute of Technology Atlanta, Georgia RESEARCH SPONSORED BY THE AMERICAN ASSOCIATION OF STATE HIGHWAY AND AREAS OF INTEREST: TRANSPORTATION OFFICIALS IN COOPERATION WITH THE FEDERAL HIGHWAY ADMINISTRATION Maintenance operations and Traffic Control (Highway Transportation) TRANSPORTATION RESEARCH BOARD NATIONAL RESEARCH COUNCIL WASHINGTON, D.C, JUNE 1989 NATIONAL COOPERATIVE HIGHWAY RESEARCH NCHRP REPORT 317 PROGRAM Project 10-34 FY'86 Systematic, well-designed research provides the most effec- ISSN 0077-5614 tive approach to the solution of many problems facing high- ISBN 0-309-04ó14-9 way administrators and engineers. Often, highway problems L. C. Catalog Card No. 89-50190 are of local interest and can best be studied by highway de- partments individually or in cooperation with their state universities and others. However, the accelerating growth Price $11.00 of highway transportation develops increasingly complex problems of wide interest to highway authorities. These NOTICE problems are best studied through a coordinated program of The project that is the subject of this report was a part of the National Co- operative Highway Research Program conducted by the Transportation Re- research. cooperative search Board with the approval of the Goveming Board of the National Research Council. Such approval reflects the Governing Board's judgment In recognition of these needs, the highway administrators of thât the program concemed is of national importance and appropriate with the American Association of State Highway and Transpor- respect to both the purposes and resourcc of the National Research Council. -
Or Ferrite Beads Ferrite Is a Magnetic Material Designed for Use at Radio Frequencies Ferrite Beads
HF OPERATORS - • - • -- • -- • • • • • • - • -- • • • - • • • • • - • WHY YOU NEED A CURRENT BALUN by John White VA7JW 10/27/2014 NSARC HF Operators 1 What is a Balun ? - • - • -- • -- • • • • • • - • -- • • • - • • • • • - • A BALUN is a device typically inserted at the feed point of a dipole-like antenna wire dipoles, Yagi’s, quads, loops etc. Vertical antenna usage possible but not discussed here Provides an interface between the coax feed line and the antenna feed point 10/27/2014 NSARC HF Operators 2 What Does It Look Like - • - • -- • -- • • • • • • - • -- • • • - • • • • • - • Typically a cylindrical tube or a rectangular box Has supporting eye bolts Antenna connection terminals Coax cable connector All very handy Supporting Eye-Bolt Eye-Bolts for Antenna wire connection Coax Connector 10/27/2014 NSARC HF Operators 3 Two Types of Balun - • - • -- • -- • • • • • • - • -- • • • - • • • • • - • Two types of Baluns, Electrically different Look identical outwardly The Current Balun – is the topic of discussion The Voltage Balun – is not useful for resolving the problems presented here Ensure the balun label states it is a current balun. If a balun is to remedy issues discussed herein, it must be a Current balun 10/27/2014 NSARC HF Operators 4 What’s Inside - • - • -- • -- • • • • • • - • -- • • • - • • • • • - • A transformer-like structure using a ferrite “core”, or ferrite beads Ferrite is a magnetic material designed for use at radio frequencies Ferrite Beads Windings on different styles of ferrite cores Threaded on coax cable 10/27/2014 NSARC HF Operators 5 What Does It Do? - • - • -- • -- • • • • • • - • -- • • • - • • • • • - • 1. Matches a BALanced antenna to UNbalanced coax connection, hence the name BAL-UN 2. Provides impedance matching between coax characteristic Z and antenna feed point Z 3. -
Preview of Period 13: Electrical Resistance and Joule Heating
Preview of Period 13: Electrical Resistance and Joule Heating 13.1 Electrical Resistance of a Wire What does the resistance of a wire depend upon? 13.2 Resistance and Joule Heating What effect does resistance have on current flow? What is joule heating? 13.3 Temperature and Resistance How does the temperature of a wire affect its resistance? 13-1 Measuring Resistance with a Multimeter 1. Turn the dial to the ohm symbol (Ω). 2. Check that the wire leads are attached to the outlets on the lower right of the meter. 3. To measure resistance, touch the ends of the leads to each end of the resistor wire. Ω V Ω COM 13-2 Act. 13.1: Measuring Resistance Measuring the resistance of the 30 cm wire. Ω 1. Do not connect the battery tray to the green board with resistance wires. 2. Set the multimeter to “ Ω ” to measure resistance. 3. Touch the ends of the multimeter leads across the thin 30 cm wire to measure its resistance. Then move the multimeter leads to the ends of the 15 cm wire to measure its resistance. 13-3 Act.13.1: Resistance of a Wire Resistance of a wire = Resistivity x Length Area ρ L R = A R = resistance (in ohms) ρ = resistivity (in ohm meters) L = length of resistor (in meters) A = cross-sectional area (in meters2) A Wire Resistor of Length L and Cross-Sectional Area A A L 13-4 Joule Heating in Wires ♦ Current flowing through wires encounters resistance, and some electrical energy is transformed into thermal energy.