Technical Papers


The following technical papers describe our instruments and how to use them:

Amp Clips for Corrosion Control

Contents:

 


 

Introduction

Swain Meters® are non-contact ammeters for corrosion protection, fault location, and quality assurance.

DC Amp Clips™ and AC Amp Clips™ are ¼ inch to 5 foot diameter aperture, field-portable, clamp-on ammeters with high sensitivity and accuracy.

They measure current from 10 mA to 200 amp., while the system is on line and working normally.

Clips are widely used. Examples include auto plants, wooded areas, the desert, shipboard, and hundreds of feet under the sea.

DC Amp Clips are used in cathodic protection of gas, oil, & water lines and offshore oil platforms. Automotive and power people measure the charge, load, and parasitic drain current of batteries without disconnecting the cables.

DC Amp Clips measure direct current, both magnitude and direction of flow, with the system intact. They are used to find Differential control leakage with the control still operational.

Telephone cable and pipe line ground faults are located by measuring the line current and its direction of flow, with the line in service.

AC Amp Clips are used to find leakage in grounds & power cable, and stray current in dairy farms. They measure alternating current in pipe lines which can cause corrosion & magnetic fields. They also measure induced or foreign short current which can be a hazard to persons and equipment.

Digital models are error resistant and tend to be smaller and lighter. The analog models show the trend of current changes better, and they are more resistant to severe environments.

The recorder or rectifier output provides DC for a data logger or oscilloscope. It is also a backup if the panel meter is damaged.

Fig. 1: Digital DC Amp Clip indicator with 1 mA resolution and 200 amp. maximum reading, with ¾" Sea Clip® and 13" Sea Clamp™ sensors.

Contents

What can be done, and how to do it are given in the first section of this paper.

How are they built, what accuracy can be expected, & which model is best for a particular use is included in the second section.

This paper is an update of DC Amp Clips for Corrosion Control given at Morgantown, W.V. in May of 1986 at the Appalachian Underground Corrosion Short Course.

DC Amp Clip

Introduction

Batteries were returned to the manufacturer because "they would not hold a charge". Auto-marine ¾" clips were used to show that the fault was parasitic drain in the .1 to 1 amp. range.

It was time consuming to find defective anodes and open feed cable along the cathodically protected lines of a major gas transmission company. Time was saved using the CP-¾" model, especially in the 20 mA to 1 amp range.

In some spots transcontinental telephone cable was losing cathodic protection current to the earth, causing local corrosion. DC Amp Clips with 4" clips were used to find leaks in the 20 to 100 mA range.

Interference to telephone cable, gas pipe and even the reinforcing steel in concrete pillars was traced to electric rail lines. Clips and clamps to 30" dia. were used to measure interference current from under 1 amp. to over 10 amp.

It was difficult or not feasible to locate foreign shorts to gas transmission line in an urban area. There was too much cross over of the high frequency current used in conventional pipe tracers. However, the gas company did find the shorts using a DC current injection process they originated together with an 18" DC Amp Clamp. This is shown in Fig. 8.

Fig. 2: Automarine Indicator with 5 mA resolution and 400 amp. maximum reading. The cable from the car to the battery carries about 60 mA. It is charging current because the ¾" Sea Clip's cabled arm is up, and the Indicator reads to the right.

Fig. 3: Analog DC Amp Clip Indicator with 1 mA resolution and 100 amp. maximum reading, with 10" Sea Clamp Sensor, in a carrying case (Box).

Clamp & Clip Defined

The Clip shown in Fig. 2 can be used with one hand. The Clamp shown in Fig 3 comprises two half circles ("C"s) bolted together at the flat sectors called lips. Clamps are further defined on p. 5.

Earth Field Effect (He)

These DC Amp Clips measure current by measuring the magnetic field intensity set up by the current flowing in the aperture of the clip or clamp (sensor). Therefore a magnet acting on the sensor will shift its zero (more so in large sensors than in small ones) if the sensor is not perfect.

It isn't. One departure from the ideal is that the sensor splits into two halves when the jaws are opened so that it can be closed around a conductor without the need to unhook anything.

We specify the change in zero offset in terms of the magnetic field of the Earth. This is the Earth Field Effect -- He for short.

To measure He the sensor is rotated full circle in a North-South vertical plane and the peak-to-peak change in zero offset noted. For a 4" Clip this should be less than 60 mA equivalent input current. We call this 0 ± 30 mA peak.

In the "how to" sections which follow it is assumed that the reader is familiar with the operating instructions and has had some practice using his DC Amp Clip.

Cars, Trucks, and Marine

The Auto-Marine, digital, and 200 amp analog DC Amp Clips are used on vehicles and offshore platforms to measure at least 4 classes of direct current while the vehicle is working normally: Parasitic drain, usually 0.05 to 3 amp.; battery charging, usually ½ to 40 amp.; heavy load, and cranking, 20 to 400 amp.; and marine cathodic protection, 0.1 to 20 amp.

To measure these there is no need to unhook any cables or wires.

Parasitic Drain

At some auto dealer's shops perfectly good batteries were pulled out of cars on warranty because they "would not hold a charge." It turned out that the fault was in the cars: a small current was being drained from the battery when the ignition was off. This was a glove or trunk compartment lamp which stayed on (1 amp.), or excessive drain in the electronic package (1/3 amp.), etc.

Parasitic drain trouble shooting requires measuring the total battery current. To do this, turn the motor off, turn the DC Amp Clip on, set the zero knob so that the meter reads near zero on the most sensitive range, and then put the clip around all the cables connected to either the (+), or alternatively the (-) battery terminal.

Polarity

Positive current direction is marked on the clip.

The meter reads (+) when current flows from left to right through the aperture of the clip when the cabled arm is up., as shown in Fig. 4A. The meter reads (-) when current flows from left to right with the cabled arm down, as shown in Fig. 4B.

Fig. 4A: The meter reads positive when current flows from left to right through the aperture of the clip when the clip's cabled arm is up.

Parasitic Drain, continued

Observe polarity, so that you know whether the meter is reading charge or discharge current. Charge current enters the (+) terminal, or leaves the (-) terminal. This helps to avoid error when reading current less than 100 mA. The battery is not being charged when the motor is off and no charger is connected.

The first meter reading may be off scale. There is no harm in overloading the meter for a few seconds. Turn to a higher range until the meter reads well up on the scale. The reading may be +0.9 amp. leaving the (+) terminal. It looks like the battery has a drain of about 1 amp., but this should be checked with the Floating Zero Procedure.

Fig. 4B: The meter reads negative when current flows from left to right through the aperture of the clip when the clip's cabled arm is down.

Floating Zero, Short Form

To check the +0.9 amp. reading turn the clip over and put it back on the battery cables in exactly the same place and way as before (with care, to have the same clip placement, but turned over. This is important). Ideally the meter will read -0.9 amp. However, if the meter was off zero a bit to start, or there was a magnetized bolt or sector of sheet metal near by, the zero will have been shifted somewhat, probably for both readings. The meter may read -1.1 amp.

The most probable true current is the average of the two readings, +1.0 amp., discharge.

This is the short form Floating Zero (FZ) Procedure. It was done by putting the clip on the battery line, once with the clip's cabled arm up, and another time with the clip's cabled arm down. This reversed the current in the aperture of the clip so the meter read positive one time and negative another time. When the average of the two readings was used (reversing the sign of the negative reading) there was no need to carefully set the zero, because zero offset was likely largely canceled out in the process.

Battery Charging

One way to measure battery charge is shown in Fig. 2, which represents a clip on the battery cable. The indicator is reading about 1/3 amp. charge on the 1 amp. range. If the motor stops with the ignition on the meter will swing to the left of zero, indicating a negative or load current. With this setup it is convenient to cycle the vehicle through a variety of loads, engine speeds, etc. to see how the alternator and regulator respond to service conditions.

Heavy Load

Full service load, or cranking current up to 400 amp. can be measured as shown in Fig. 2. The current should not exceed 500 amp. because this might damage the DC Amp Clip. Models that are rated for less than 200 amp. should not be used for cranking current measurement.

Marine Cathodic Protection

Shipboard rectifier & anode current in an impressed current cathodic protection system can be measured with a ¾" Sea Clip and one of the indicators shown in Figs. 1, 2, or 5. Measuring sacrificial anode current can be harder, but there are ways.

Undersea Current Measurement

Sea Clips are used underwater to hundreds of feet depth when they are equipped with water-proof connectors, cables, and a suitable surface Indicator.

Offshore oil & gas platforms frequently have sacrificial anodes held to the structure by 2" to 4" standoffs. The anode current is measured by measuring the current in the standoffs as shown in Fig. 5B, preferably using at least the two step Floating Zero Procedure. This has been done with divers, and more recently, with ROVs. It is best to call us about your particular need.

Fig. 5A: CP-¾" Sea Clip with 5 mA resolution and 40 amp. maximum reading. This ¾" dia. aperture Sea Clip has Earth Field Effect rating He = 0 ± 5 mA peak.

Some offshore platforms use a large sacrificial anode at some distance from the platform, with connection through a heavy cable on the sea bottom. The current is measured by placing the clip around the cable.

One reason for measuring the current is to make sure that the anodes on standoffs (and the sea bed anode with cable) are connected electrically as well as physically to the platform. Apparently the connection can look good to a camera on an ROV, but not be good electrically. Another is to find what current is required to protect the platform, and thus to determine what anode weight is required for this, and future platforms.

Water Current

Apparently it is not always feasible to locate an anode cable on a ship, or there may be none - as in an anode on a prop shaft. In this case we suggest the less accurate but useful method of holding a sea clamp around the anode's surface so that the anode current flowing in the sea water passes through the aperture of the clamp. This works. DC Amp Clamps measure the current flowing through the aperture, be it in water, plasma, steel, etc.

Shaft Current

Pump and propeller shafts may carry a direct current (or alternating current -- we make meters for AC also). This can be measured by placing the clamp (loose fitting) around the shaft, whether rotating or stationary. There may be noise, so we suggest you phone to discuss the conditions. Of course, if the shaft is rotating very special care is required to avoid harming a person.

Fig. 5B: Analog indicator with 1 mA resolution and 100 amp. maximum reading. The 5" Sea Clip is suited for use measuring current in pipes, either on land or under the sea.

Corrosion Control

Anodes, Bonds, and Rectifiers

Parts of an impressed current cathodic protection system for a pipeline are outlined in Fig. 6. The rectifier is connected between the pipe and the anodes so that current flows in the earth between them. The current in each part is measured by placing the clip around the cable, observing polarity. The system stays on line and operates normally during the test. There is no need to disconnect any lines. If the current is under 100 mA at least the short form Floating Zero Procedure should be used.

The DC Amp Clip model CP-¾" Sea Clip shown in Fig. 5A can be used to measure the current output of the rectifier IR, and compare this with the drains to anodes distributed along a string. Anodes 1, 2, 3, & 4. each represent one of a group.

The rectifier output in this illustration is IR = 3 amperes.

Anode 1 is typical of a good unit in this illustration. Its drain is I1 = 1 amp. String current Ia is measured and found to be 2 amp., which seems reasonable.

Conduit

Rectifier or anode current can be measured through conduit - plastic, copper, or steel. This was shown in the lab., and later verified at a power plant on an anode line in steel conduit over 50 ft. long. There was just one wire in the conduit, and the conduit itself did not carry a current, so we were able to read the anode line current to within 3% of what it showed outside the conduit.

Fig. 6: Rectifier and anodes in a distributed impressed current cathodic protection system. DC Amp Clip model CP-¾" Sea Clip shown in Fig. 5A may be used to measure the anode cable current.

The clip reads the algebraic sum of all currents flowing through the aperture. If there are two lines enclosed by the clip it will indicate the one plus the other. If these happen to be the (+) and (-) leads of a rectifier carrying 1 amp. the clip will show zero if all the current going out on one line comes back on the other line.

Leakage to Ground

However, if the rectifier sends +1 amp. out on the (+) line, but there is leakage to earth at the rectifier so that only -0.9 amp. returns on the (-) line, then the clip around both lines will show +0.1 amp., i.e., the leakage.

Foreign Interference

There is foreign line interference, represented by VF, at anode 2. This causes normal anode 2 to draw an unusually large current I2 = 2 ½ amp. Since Ia is only 2 amp., one would expect that I2 would be 2 amp at the very most. This is a clue that foreign interference is present.

Stringer current Ib is ½ amp., but in the wrong direction. This suggests that anode 3 is weak, and that anode 2 is subject to interference.

The current Id at anode 4 is practically zero, meaning that the cable is broken between anodes 3 and 4. Back a bit more than half way the clip is put on the cable at Ic, which is found to be a few milliamperes, headed the wrong way. This probably means that the break (X) is in earth between Ic and Id.

The pipeline may be broken into electrical sections by insulating flanges with bonds across. The DC Amp Clip is used to measure the bond currents with a view to finding coating insulation flaws, shorts to foreign pipes, interference from foreign lines, or newly installed foreign anode beds.

If the insulating flanges are widely separated, and if there is a severe problem as happens in some urban areas, then the corrosion engineer will want to get a clamp that fits around the whole pipe. This way he can measure the actual pipe current at several locations, and thus locate the interference. This is discussed in the section- Locating an Electrical Short.

Clamp & Clip Defined

A Sensor is either a Clip or a Clamp.

The Clip shown in Fig. 2 can be used with one hand. The Clamp shown in Fig 3 comprises two half circles ("C"s) bolted together at the flat sectors called lips. The stud bolts are captive to the low C which has only the bridle cable attached. There are oversize holes in the lips of the top C which has attached both the bridle and the main cable. The stud bolts are put through the holes and secured with two brass hex thumb nuts.

The "nose" is the pair of lips far from the bridle. The "tail" is the pair of lips near the bridle. The main cable has a female connector to the Indicator.

Clamp Polarity

Positive current direction is marked on the clamp.

The direction of current flow through a clamp (Fig.7) is analogous to the clip. In a clip positive current flows from left to right through the aperture when the cabled arm is up. Similarly, in a clamp positive current flows from left to right when the half circle ("C") having both the main cable to the indicator and the bridle cable to the other "C" is on top. This is shown in Fig. 7.

Another way to look at it is that positive current flows from the bridle side of the clamp, through the aperture, to the side more remote from the bridle.

Fig. 7: Clamp polarity. The arrow shows the direction of positive current flow through a clamp.

Measuring Direct Current in Pipe

The process for measuring DC in 4" pipe or smaller is, in some ways, similar to that for parasitic drain given on p. 3. Differences appear because the clip is larger and the pipe may be steel.

If the current to be measured in copper pipe is more than 10 times the He rating of the clip the straight foreword method should work, but it is prudent to use the short form FZ procedure on p. 3. The He spec. for a 5" clip is 0 ± 40 mA.

If the current is small it is likely to be more difficult to get accurate results with a simple process on iron or steel pipe because it usually has high magnetic permeability which distorts the Earth's magnetic field and so shifts the zero of the clip. An interrupter discussed on page 11, or the full FZ procedure given on page 12 may be needed.

On steel pipe the accuracy expected when the full FZ is used by a skilled and experienced person is 0 ± 2/3 He. Then if 1 amp. is measured with a 5" clip on steel pipe the result should be within 2/3 of 40 mA, i.e., 0.97 to 1.03 amp. using the process shown on page 12.

Large Clamps

Large clamps differ from clips in that they have:

     

  • Less gain. A 30" dia clamp may have ¼ the sensitivity of a 2 ½" clip.

     

     

  • Greater He. The He rating of a 30" clamp is 0 ± 410 mA peak, but a 2 ½" clip is 0 ± 10 mA.

     

The large He usually causes a substantial zero offset change as the clamp is moved near a big steel pipe. Fortunately, the current that is important in a 30" pipe is much greater than that of concern in a 2" pipe, so the real problem of the larger He is mitigated. However, it is usually a good idea to plan on using the FZ procedure. "Nose" and other terms are defined on p. 5, "Clip and Clamp Defined".

Two people are needed to do the FZ procedure properly when a 30" clamp is used. Shims will be needed to hold the clamp in one set position. Two or 3 pieces of plastic foam, ¾" or 2" board will usually do.

Special Adapters; No Thumb Nuts

When feasible we make things a bit special at the request of customers. One example is an 8" clamp with lips adapted to be secured with large copper clips instead of thumb nuts. One of our Canadian customers said it was a trouble to put thumb nuts on the captive studs in snow, so we flattened and grooved the lips to match the clips. Please telephone if you need something special.

Locating an Electrical Short

An electrical short of a pipeline may make cathodic protection difficult or impossible. If a water pipe shorts a 12" gas line in an urban area it can be located as shown in Fig. 8.

A battery (VA) is temporarily connected to the 12" line in manhole A. The negative terminal of a truck battery in series with a lamp to limit the current to 5 or 10 amp. can be connected to the pipeline. A water main usually works as a ground.

The clamp is placed over the line at position 1 to the left of VA in manhole A. The current i1 is small, and does not change much when VA is connected and disconnected i.e., interrupted. This means that the short is not likely to be to the left of manhole A.

The clamp is moved to position 2 to the right of VA. Current i2 is much larger, probably several amp., flowing toward the battery when VA is connected, and greatly reduced when VA is disconnected. Since i2 is large and follows the interrupt pattern of VA the operator expects to find the short to the right of manhole A.

The battery and DC Amp Clamp are moved to the right of manhole A, to manhole B. The process is repeated. This time the large current following the interrupt pattern of VB is i3, and it is flowing toward the battery. A check of i4 shows that it is small and does not much follow the interrupt pattern of VB.

Fig. 8: DC Amp Clamp used to locate an electrical short to a pipeline by driving the pipe with a switched current at first one manhole and then another until the short is bracketed. A SEA Clamp similar to that in Fig. 1 or Fig. 3 is suited for this work.

The large current following the interrupt pattern of VB is i3, and it is flowing toward the battery. A check of i4 shows that it is small and does not much follow the interrupt pattern of VB.

This says that the short is most likely to the left of manhole B. And it is between holes A & B. This may be a good enough clue to the location of the short. If not, the suggested procedure is to repeat the process in a manhole half way between A & B.

Telephone Cable

Lead sheath cable, and to some extent, the steel armor on fiber optic cable are apt to corrode where current leaves the cable. Fig. 9 shows a way to find out where current is leaving the cable by measuring the normal direct current on the cable's sheath.

Phone cable is shown going underground from bell hole to bell hole, probably in an urban area. The current is 70 mA at a start in bell hole #1, and the same in #2. Since there were no additions, it is likely that there is no leakage to earth between holes 1 & 2.

However, at bell hole #3 the current is only 30 mA, so the operator expects that 40 mA left the cable and went in to the earth between holes 2 & 3. This may be a good enough clue to find the current leak, but if not, the user will want to drill a new hole between bell holes 2 & 3, and repeat the process.

Fig. 9: Finding telephone cable leakage between bell holes. A 4" version of the DC Amp Clip shown in Fig. 5B is suited for this work.

Clip Definitions

The attitude of a clip is specified in terms of the "nose" and the axis of the aperture.

"Lips" are the flat areas where the aperture of the clip opens up to admit the guy wire when the arms are squeezed.

The "nose" is the pair of lips of the clip farthest from the arms, or handles. The clip points north when the lips are nearer the north pole than the arms.

The "tail" is the pair of lips nearer the arms.

The lips should always be clean and free to close when the arms are released.

When a vertical guy wire is in the aperture of the clip, it is best held so that the axis of the aperture lines up with the wire.

Flange Leakage (Simplest Way)

Cathodic protection current leakage across a defective insulated flange in a pipe line can be measured using one or more of the methods shown in Fig. 10.

If the current is quite high, say ½ to 5 amp. the simplest way is to put the clamp on the pipe close enough to the flange so that there is no path for current to enter or leave other than through the flange, and measure the current with the DC Amp Clamp. The battery and voltmeter are not required.

However, three or four checks are advisable, especially if the current is small, say less than ten times the He rating of the clamp used.

To verify the reading of flange current, repeat the measurement of pipe current on the other side of the flange. The two measurements should be in reasonable agreement if there is no other way for current to enter or leave the pipe line between the measurement points.

Use the full Floating Zero Procedure, or at least the short form. Results should be consistent.

Use a current interrupter as shown in Fig. 11 if the current source can be switched.

Use the full switched battery setup shown in Fig. 10. In each case results should be consistent, or the discrepancy explained.

Fig. 10: DC Amp Clamp used on a pipeline to measure insulating flange leakage current if. The flange voltage Vf is also measured as current iB from a battery in series with a lamp is switched on and off. The flange resistance Rf is equal to the flange voltage Vf divided by the flange current if.

Flange Current c/o Flange Resistance

Fig. 10 shows the arrangement for measuring small flange leakage current. First flange resistance is determined, and then flange voltage is used to get the current.

The DC Amp Clamp is placed on the pipeline close to the flange so that there will be no current entering or leaving the pipe between the clamp and the far side of the flange.

A dc voltmeter (Vf) is connected across the flange. It may be connected spanning the clamp and flange, or directly across the flange if this is more convenient, because the pipe has low resistance.

A switched current source (iB) consisting a battery, lamp, and interrupter (switch) are connected in series across the flange and spanning both the voltmeter and clamp. The current source may put out something like 1 amp. This 1 amp. will likely go both through the flange and back away from the flange and around the system the long way. The purpose of the DC Amp Clamp is to measure the change in the actual flange current.

In operation the change in flange current is noted together with the corresponding change in flange voltage. Their ratio is the flange resistance.

For example, with the switch open the DC Amp Clamp may read +0.15 amp. while the voltmeter Vf reads +0.03 volt. When the switch is closed the clamp may read +0.35 amp., while the voltmeter reads +0.23 volt. The current change with the switch closed was +0.2 amp, and the corresponding voltage change was +0.2 volt. So the flange resistance is 1 ohm. At least under these conditions. Some leaky type resistors are non-linear. They change resistance when the current changes, temperature, etc. And it may be that it is not the flange, but a conductive liquid in the pipe.

Finally we get the flange current. Since the flange voltage was +0.03 volt when the switch was open this is presumed to be the normal voltage across the flange. Since the resistance is 1 ohm, the normal flange current is +0.03 amp.

This process also helps solve other problems.

URD Concentric Neutral Cable Resistance

Corrosion can eat away part of the neutral on URD power cable, especially when the concentric neutral is bare metal in the earth. But since this corrosion is usually concentrated in a small sector of land, it is useful to be able to measure the neutral resistance.

The problem of locating a corroded sector is complicated by the fact that AC load current can take alternate paths, so that the AC voltage drop is not reliable in locating corrosion.

A solution is the setup in Fig. 10. Replace the leaky flange with a sector of URD cable between 2 manholes. And the clamp with a clip. Usually 2 ½" is big enough. The process of finding the resistance between the 2 manholes is the same as for the flange. The key is that the DC Amp Clip measures the current in the section of URD under test.

One Man Does the Work of Two

One of our Canadian customers said that, with the right equipment, he can work alone and do the work of two men when the second man would be needed for remote switching or data taking. For example, in the case of the flange current measurement above, suppose that an interrupter is not available. Then a co-worker can switch the breaker as required if voice or radio communication is available.

To avoid having to hire another man, our Canadian friend bought a well known digital data logger (names on request) which includes a clock and connected it to the recorder (Rcdr.) jack voltage output of the DC Amp Clip so as to record both pipe current and the time of day for a specific current magnitude. And in Fig. 10, he would also record the flange voltage on another channel. Then he would go to the breaker and key it off and on, recording in his notebook the time of each action.

When the needed tests are done he would go to his office, down load the data logger into his computer, and work to a solution.

Zero Cancelled by Current Interrupter

A current interrupter can be used to remove the zero offset problem associated with measuring small currents with a large clamp; PROVIDED that it is known that the only current of interest comes from a rectifier or some interruptible source. Current from other sources will be missed when using an interrupter. The full floating zero procedure must be used to be sure of getting all currents in the pipeline.

If all the flange current is known to come from a rectifier, arrange to have the rectifier turned on and off (10 sec. on, 20 sec. off) by a current interrupter. Then the flange current is the difference between the on and off readings. Zero setting, and zero offset do not matter. The direction of flow of the current is known, because the direction of change of the meter reading during the 10 sec. on time shows the polarity.

For example, if the meter reads -45 mA during the 20 sec. off time, but -15 mA during the 10 sec on time, the pipe and flange current during the on time is +30 mA because the meter changed to a more positive reading when the rectifier was switched on.

Fig. 11: Current interrupter used to eliminate the zero offset problem when measuring flange current. The digital DC Amp Clip shown in Fig. 1 is suited for this work. This process is also good for measuring a small current with a small clip.

Guy Wires

Current flowing from a guy wire or its anchor into the earth generally causes corrosion. Real attention was given to this some time ago when a not-too-strong windstorm took down a whole line of poles. Examination showed that the guy wire anchor rods pulled out of the earth easily because there were only vestiges of anchor left. The anchors had all been corroded away.

It was found that the cause was current going down the guy wire to the anchor and into the earth. This often corrodes the anchor, but at times it corrodes the guy rod itself. Since the guy rod has a smaller mass than the anchor, a current which would represent only slow corrosion to the anchor is serious to the rod

Mr. Orville W. Zastrow*, Mr. S. A. Potocny**, and others have written at length about this. From a casual reading it, 10 mA for 30 years is significant for the typical anchor. If it is primarily the rod that is primarily corroding, 10 mA could be serious in a few years.

The process for measuring guy wire current greater than 100 mA is similar to that for that given on p. 3 for measuring parasitic drain current at a battery. At least the short form Floating Zero Procedure should be used.

* Zastrow, Orville W., REA Bulletin 161-23, pp. 13-15.

** Potocny, S. A., Telephone guy rod corrosion by stray currents, Materials Performance, Dec. 1979, pp. 19-25.

Full Floating Zero Procedure

To measure guy wire current around 20 mA requires one of our best DC Amp Clips and the full Floating Zero Procedure (full FZ).

Most guy wires are under ¾" dia., so a ¾" Sea Clip will do nicely. Some heavy guys are up to .85" dia. If this is the case at your plant, call and we will arrange to supply oversize clips to you.

The best ¾" Sea Clip is specified to have Earth Field Effect (He) less (better) than 0 ± 1 ½ mA peak. This would seem to be stable enough to measure 10 mA, and it is, on copper wire away from magnetized bolts or metal.

However, most guy wires are steel which can be magnetized by the Earth's magnetic field. And if not magnetized, they tend to distort and concentrate the Earth's magnetic field. This causes a zero shift which can lead to important error if ignored.

Most of the error due to zero offset is likely to be removed if the full FZ is used properly. By this the average measured current will probably be within ± 2/3 the present He of the clip, provided the user has studied the operating instructions and this procedure, and uses the same care and skill as when he successfully practiced measuring a known small current flowing in steel rod or cable, preferably in the comfort of his shop.

It is not easy, and it is not absolutely sure to work every time. It can be done. One of the Delco engineers told me that he could get 0 ± 2 mA accuracy reading parasitic battery drain- a similar challenge. This has been done similarly.

Setup for FZ

Look for a location on the guy wire (or rod) which is relatively free of magnets. Do this by sliding the clip longitudinally up and down on the wire while looking at the meter. Choose a spot where the meter reading does not change much. Set the range switch for 1 mA resolution. Avoid a location near bolts or special fittings.

For simplicity, the guy wire is vertical.

Prepare a data sheet convenient for writing down readings in pairs. Leave space for average calculations.

FZ Process

The objective is to get at least 3 pairs of guy wire current readings, all at the same position on the wire, all on the same current range, and all with the same zero setting. The Zero setting does not have to cause the meter to read particularly close to zero. It is more convenient to set the Zero control so that it reads less than ± 50 mA when the clip is not on the wire.

The pairs of guy wire current readings are taken at at least three different attitudes of the clip on the wire. four are preferred. Each pair includes a "normal" or positive polarity reading as in Fig 4A on p. 3, and also a "reverse" or negative reading, with the clip turned over, as in Fig 4B. The attitudes are preferably symmetrical about the wire; the four points of the compass if the wire is vertical.

By the same position on the wire it is meant that the wire is centered inside the aperture of the clip to the same extent for all readings. And it holds its position vertically. It is not necessary that the clip be exactly centered on the wire, but this will not hurt. It is necessary that the clip be off center the same amount for each reading, whether the clip is normal or reversed. And the clip should keep the same longitudinal position along the length of the wire for each reading. This is quite important.

Some users make wood or plastic jigs to center the wire in the clip. Others use a free hand. For example, ..IF SAFE- WATCH OUT FOR ELECTRIC SHOCK.. the left hand can be put on the wire so as to feel the clip - just touching - no force. The gentle touch of the side of the clip serves to locate the clip with respect to the wire as it is positioned for first the normal and then the reverse reading. Hold the clip by just the cabled arm. This avoids the problem of cracking the lips open by a mild squeeze on the two arms. When proceeding to the next attitude, keep the hand at the same height on the wire, just rotate around the wire.

Attitude is specified in terms of the "nose" and the axis of the aperture. The nose is the pair of lips of the clip farthest from the arms, or handles. The clip points north when the lips are nearer the north pole than the arms. When a vertical guy wire is in the aperture the clip is best held so that the axis of the aperture lines up with the wire.

FZ Data Example

In the example below the first reading is the normal or (+) meter indication in mA, with the cabled arm on the right. Then current from the top of the pole to the anchor reads positive, and tends to be corrosive. The second is the reverse or (-) reading. The average is the sum of the normal and reverse readings, but with the sign of the reverse reading inverted.

The zero control is not touched during the whole series of readings. This is important. Start over if the Zero control is moved by accident.

Heading of pair Readings
mA
Average
mA
North +40 +33
-25
East +30 +25
-20
South* +55 +25
+5
West +25 +20
-15
Sum of averages +103
Average of 4 pairs +26

* Note that the meter read (+5) at the reverse reading. When the sign of the +5 is inverted and added to the +55 normal reading the sum of the two is +50, so the average is +25.

The accuracy expected when the full FZ is used by a skilled person on a steel conductor is 0 ± 2/3 He rating for the clip. This is He = 0 ± 1.5 mA for our best ¾" Sea Clip. So we expect that the true current is between 25 and 27 mA. However, especially at small current levels, it is better to add one or two mA to the likely uncertainty. For example, the accuracy rating of an analog Indicator alone is 0 ± 3 % of full scale. If this is 100 mA, we need to add ± 3 mA to the uncertainty.

From this it is concluded that the true guy wire current in this example is likely to be +26 mA, ± 2 or 3 mA; i.e., +23 to 29 mA. It is positive, so it tends to be corrosive. However, the damage to the anchor may not be serious until the current has persisted for several years. But if the current is primarily leaving the rod the damage could be serious much sooner*.

* Please note: I am an instrument builder, not a corrosion engineer. These are my impressions from casual readings. The user should consult the literature.

Checks

Each pair of readings should be checked to see if it is fairly consistent with the others. In the example above the maximum deviation of the average of a pair is 7 mA from the average of all pairs. This is about 5 times the He = 0 ± .5 mA rating of the clip. It is reasonable on steel wire. In contrast, if a pair of readings had been +70 and -80 mA the data should be rejected. Use 3 instead of 4 headings, or go to a different spot on the guy wire.

If time permits, the whole series of readings should be repeated in the same spot on the wire. In general they will differ somewhat, but the average of all pairs to be the same within 2 or 3 mA is expected.

If feasible, a complete set of readings should be taken at another spot on the wire at least a foot away from the first. Again, individual readings may differ by 10 mA, but the average of all pairs should be the same within 2 or 3 mA.

The user should also be on the lookout for errors due to RFI, AC flowing in the guy wire, etc. If not sure, call us at 941-957-3110, or Fax: 941-378-0712.

AC Rejection

DC Amp Clips reject AC, and vice versa. The best analog and digital DC Amp Clips will change their reading less than 0 ± 5 mA because of up to 10 amp. AC flowing in the line. And the change due to 30 amp. AC may be less than 15 mA.

RFI

Radio Frequency Interference (RFI) can shift the zero and may make readings erratic. If RFI is suspected, cover the bottom and sides of the DC Amp Clip with aluminum foil, and then put it back inside the leather case. This usually stabilizes the meter.

Alternating Current

Alternating current needs to be measured because a large AC flowing in a pipe or cable can be a threat to property and personal safety. For example:

It has been estimated that 1% to 3% of AC in a pipe is direct current. If so, 2 amp. AC pipe to soil current can represent 20 mA DC. A DC Amp Clip is usually able to read the 20 mA, give or take 5 to 10 mA, and say which way it is going.

An oil company's engineer told me how AC put a good sized pit in one of their gasoline lines. Somehow a water line had come close to their line, and it was carrying substantial alternating current. Trucks going over the lines pushed them together, but they separated when the truck passed. The AC shifted in and out of the gas line until the arc had worn a fair pit. It is fortunate that they found the fault before the pit went deeper.

Another engineer told me of occasional surges of induced current to over 100 amp. in a gas pipeline running in the same corridor as a major power transmission line. Apparently there was concern that this would cause corrosion, and might endanger persons at the pumping station.

A power company engineer told me about URD cable that had corroded until AC shifted from the line to the local water system. Residents got a small shock when the turned the water spigot.

Another power engineer told of concern about considerable current in the leg of a transmission line tower.

A small AC can also be a problem. For example:

A contractor in an urban area is concerned that AC flowing in copper plumbing can cause corrosion, and/or create magnetic fields that some may consider harmful to persons.

A dairy farMER™told me that his estimate of lost production of milk due to stray power current in dairy cows was a million dollars a day. Ten mA is said to be the threshold.

How to Measure AC

There are at least two ways to measure AC with the system operating normally. There is no need to unhook any wires or break open any pipe lines.

Simplest

The simplest (least equipment to carry) is shown in Fig. 11, where the clamp is shunted with a few ohms resistance and then a Fluke meter is used to read the voltage across the shunt. The resistor R can be adjusted so that the Fluke model 87 meter, while really reading AC millivolts rms, shows a number the same as the current in amperes.

Suppose the line current ii is 12 amp., and the sensor (a clip or clamp) has N = 1000 turns. Then under ideal conditions the sensor current is = 12 mA. If the shunt R = 1 ohm, the voltage across R will be 10 mV, so the user can interpret this as ii = 12 amp.

The problem is that sensitivity is limited. If two digit readings are needed and the resolution of the Fluke (one of the best for field portable use) is 0.1 mV, the minimum current reading is 1 amp. The dairy cattle and people begin to get uneasy at 0.01 amp. More sensitivity is needed for some uses.

Fig. 12: Measuring AC on a pipe with a 1 ohm shunt resistor across the sensor's coil. Calibration resistor "R" is set so that a Fluke 87 true rms meter reads 12 mV when 12 amp flows in the pipe.

Fig. 13: Digital AC Amp Clip having 0.1 mA resolution and 20 amp maximum reading on a 5" clip. The output voltage can be either AC, or rectified AC, proportional to the current.

High Sensitivity

We make AC Amp Clips and Clamps from ¾" to 5 feet diameter. If properly calibrated they use the same sensors as the DC Amp Clips. The maximum sensitivity of the ¾" analog model is 1.0 mA rms on a sine wave, full scale. The digital model has a resolution of 0.1 mA, and like the analog, a maximum current reading of 20 amp. Larger clips and clamps have more turns (N), more stray pickup, and less sensitivity.

In addition for viewing the waveform with an oscilloscope both the analog digital models can have an AC voltage output proportional to the current input (ii) usable from 10 Hz to over 2000 Hz. The digital meters can have an output which is a rectified form of the current input. This also permits use of an oscilloscope to spot pulse distortion, and in addition it provides a DC signal suited for data logging. The user can record current surges which occur when he is not there.

Stray Pickup & DC Rejection

On the more sensitive range a direct current flowing in the aperture of a ¾" clip may reduce the sensitivity about 3% when 5 amp. DC is present.

Of course, the DC must be really steady. The AC component of a fluctuating direct current is the peak-to-peak of the change divided by 2.8. For example, 1 amp. DC which fluctuates only 1% p-p has a 3.6 mA rms AC component. The meter will show this 3.6 mA, but depending on frequency, it may add algebraically, or rms wise, to the AC intended for measurement.

Stray pickup in a ¾" clip is usually magnetic. If an interfering current is flowing in a cable touching a ¾" clip the rejection may be 100 amp. per amp. For example, If the clip is measuring 20 mA but a wire carrying 1 amp. touches the outside of the clip there may be induced an interfering current of 10 mA. This can add phasewise (algebraically) if the currents are at the same frequency. But if they are at a different frequency they tend to add rms. wise.

This 100 amp. per amp. magnetic rejection may increase to 1000 if the wire touching the side of the clip is oriented for least pickup. If the wire carrying the interfering current is moved away from the ¾" clip by 1 ¼" the rejection may again increase by a factor of 10 to 10,000.

A nearby transforMER™can cause magnetic pickup. For example, a 2 ½" clip had 0.1 mA magnetic pickup when held above the bench. But this might increase to 0.3 mA if there were a fluorescent light ballast transforMER™within 3 feet.

Larger sensors have greater pickup, magnetically, and electrostatically.

Electrostatic pickup is basically capacitive coupling of the clip to an AC voltage source. It increases with the voltage of the interfering wire, not its current. It also increases when the user grounds the Indicator by connecting it to an oscilloscope or recorder, especially if these run on the AC mains power. A 2 ½" Clip located about a foot from a small radio plugged into the AC mains but turned off caused the meter to read 0.6 mA when the Indicator was connected to an oscilloscope.

[Text from page 16 on is missing!]

DC & AC Amp Clip Characteristics

Gain & Zero Offset

Maintenance

Selecting a Swain Meter™

AC Amp Clip

Conclusion