EC TRACK · ELECTRICAL BASICS FOR CP

AC vs. DC Electricity: Characteristics and Differences

Why CP runs on DC, what AC mains look like before they're rectified, and where each shows up in the field.

Foundation ~10 minutes PDH/CEC eligible

You’re at a test station on a stretch of pipeline that runs parallel to a 138 kV transmission corridor. The towers march along the right-of-way a couple hundred feet to the east, exactly the way they have for the last forty miles of pipe. You open the lid on the test post and clip your meter leads to the pipe header and to a Cu/CuSO₄ half-cell pressed into moist soil at the base of the post.

Meter on V DC. The display settles at −1.05 V. The pipe meets the −0.85 V criterion at this location with comfortable margin. CP is doing its job here.

Same lead pair, same half-cell, same pipe. You flip the meter to V AC. The display jumps to 6.5 V AC. Steady. Repeatable.

Two readings. Same conductor pair. Two completely different stories. The DC reading is a CP question and the answer is good. The AC reading is a different question entirely — induced from the power line above, having nothing to do with the rectifier feeding this section, and not something more CP current is going to make go away. This module is about why those are two different regimes, why CP only addresses the first one, and how the meter mode is the discipline that keeps them straight.

Why this module sits here in the rung

The hinge between the math and the hardware

EC-001 named the shapes of CP circuits — series, parallel, and the rules that govern them. EC-002 walked the math that runs inside those shapes. EC-003 distinguished voltage, current, and resistance and showed where each one is read at a real CP test point. Every one of those modules assumed something we never said out loud: the current is DC. The shapes are DC shapes. The Ohm’s Law math is DC math. The structure-to-soil readings are DC voltages.

That assumption is correct, and it’s load-bearing. Cathodic protection is a DC technique. But CP systems live in a world where AC is everywhere — feeding the rectifier, riding on cables that pass nearby, induced onto the pipeline itself by parallel power lines. The meter you take into the field reads both regimes, and a fair share of CP fieldwork is knowing which one you are reading at any given moment, and what that reading does and does not tell you.

Three jobs sit on this module:

Compare AC and DC as electrical regimes — waveform, frequency, peak vs. RMS, where each shows up in a CP system, what mode the meter is in to read each.
Explain why CP requires DC — and why no amount of AC can substitute, regardless of how strong it is.
Name how AC ends up on a pipeline from sources unrelated to the CP system, and why it is a separate problem on its own work track, with its own techniques and its own reading.

The math here is light — one small piece of arithmetic on peak vs. RMS — because the work of this module is conceptual. EC-005 will pick up power and energy calculations in CP circuits. The deeper treatment of AC interference — coupling models, induced-current thresholds, decoupling devices, mitigation design — lives in a later EC module. EC-004’s lane is to make sure the difference between the two regimes is wired in cleanly before any of that downstream work has to land.

DC — constant in one direction

Direct current is electrical current that flows steadily in one direction. The polarity is fixed: there’s a positive terminal and a negative terminal, and current flows from one to the other without reversing. Plotted on a graph of current versus time, pure DC is a flat horizontal line — the value doesn’t change as time passes.

Voltage in a DC circuit behaves the same way. Source voltage is a fixed level. Drops across resistors are fixed levels. Read it on a meter and the display sits at one number until something in the circuit changes.

Where DC lives in CP work

Every part of a cathodic protection system that does protective work is on the DC side:

Rectifier output. The DC bus inside an impressed-current rectifier cabinet — the (+) terminal feeding the anode header cable, the (−) terminal returning from the structure. Typical values: 12 V to 50 V on V; a few amps to fifty amps on I.
Galvanic anode systems. A magnesium or zinc anode wired to a buried structure produces DC by simple electrochemistry — no rectifier needed. The anode sits at one potential, the structure at another, and the difference drives a small DC current through the soil and back through the bond cable. Typical bond currents: tens of milliamps to a few amps.
Structure-to-soil potential readings. The −0.85 V Cu/CuSO₄ criterion is a DC voltage between the structure and the soil. The whole reason a Cu/CuSO₄ half-cell works as a reference is that its own electrochemistry sits at a stable, known DC potential.
Bond shunt readings. The millivolts you read across a calibrated shunt to find a bond current — those are millivolts DC. The current through the shunt is DC.
Batteries. Where DC is needed for a small load with no utility power available — coupon cells, monitoring equipment, cathodic-disbondment test rigs in the lab.

The meter mode for every one of those readings is DC: V DC for voltages, mA DC or A DC for currents, mV DC for the small voltage drops across shunts. A meter on AC mode looking at the same conductors will read close to zero — because pure DC has no alternation for the AC mode to register.

AC — alternating, sinusoidal

Alternating current is electrical current that reverses direction periodically. The “wave” of an AC system is a sine wave — current rises smoothly from zero up to a positive peak, falls back through zero down to a negative peak, then rises back to zero again. One full rise-and-fall is one cycle. The number of cycles per second is the frequency.

DC sits at a steady level. AC swings sinusoidally above and below zero. Same axes, two regimes.

The standard utility frequency in the United States is 60 Hz — sixty full cycles per second. (Most of the rest of the world runs at 50 Hz; the principles are identical, only the number is different.) Each cycle has two reversals — once on the way down through zero, once on the way back up — so US-grid AC reverses direction 120 times per second. Faster than a human eye perceives, but well-defined and the dominant signal everywhere on the utility grid.

Peak vs. RMS

An AC waveform is described by two voltage numbers, and they are not the same. The peak voltage is the maximum instantaneous value the waveform reaches at the top of its swing. The RMS voltage (root-mean-square) is the equivalent steady DC voltage that would deliver the same average power into a resistive load. The two are linked by a fixed factor for a clean sine wave:

V_RMS = V_peak × 0.707

V_peak = V_RMS × 1.414

So a 120 V RMS outlet has a peak voltage of about 120 × 1.414 ≈ 170 V. A 240 V RMS service has a peak of about 240 × 1.414 ≈ 339 V. A 480 V three-phase line has a line-to-line peak of about 480 × 1.414 ≈ 679 V. Catalog ratings, breaker labels, and nameplates use RMS by convention — when somebody says “120 volt outlet,” they mean 120 V RMS, not 120 V peak.

The 0.707 isn’t a memorized constant; it’s a derivation. RMS is literally the square root of the time-averaged square of the waveform. Run that integration on a sine wave with peak amplitude 1 and you get exactly 1/√2 ≈ 0.7071. Inverting gives √2 ≈ 1.4142 for peak from RMS. Different waveforms (square, triangle, half-wave rectified) have different RMS-to-peak ratios — but for the clean sinusoidal AC on the utility grid, 0.707 / 1.414 is the pair to keep in your head.

Where AC lives in CP work

Three places, three different stories:

Utility input to the rectifier. Every impressed-current CP system starts with utility AC at the cabinet — typically 120 V or 240 V single-phase for small units, 240 V or 480 V three-phase for larger ones. That AC enters the cabinet, crosses through the transformer, and only then becomes the DC the system actually uses. This AC is on purpose, on the utility side of the cabinet, and the rectifier wouldn’t work without it.
Induced AC on the pipeline. When a buried pipeline runs parallel to a high-voltage transmission line for any meaningful distance, the pipe acts like the secondary of an enormous transformer — the AC current in the power line induces a smaller AC current and voltage on the pipe itself. This AC is incidental, not on purpose, and it has nothing to do with the rectifier. We unpack it in the next section.
Ripple on rectified DC. The DC coming out of a rectifier isn’t perfectly smooth. There’s a residual AC component — ripple — riding on top of the DC level, at twice the input frequency (120 Hz for full-wave rectification of 60 Hz AC). Modern rectifiers reduce this with filtering, but a small amount remains. We treat it briefly in Scenario C below.

The meter mode for any of those readings is AC: V AC for voltages. A meter on DC mode looking at clean AC reads close to zero — because the average of a symmetric sine wave over time is zero, and the DC mode reports the average.

Why CP is fundamentally a DC technique

This is the load-bearing section of the module. Cathodic protection cannot run on AC. Not at low voltage, not at high voltage, not at any frequency. Three reasons explain why, and they are all rooted in the electrochemistry that CP exists to drive.

1. Polarity has to be fixed.

The whole point of CP is to make the structure the cathode of a deliberate electrochemical cell — to push it to a more negative potential than it would naturally sit at, so that the metal-loss reactions that normally happen on the structure surface stop. That requires the structure to be the cathode continuously, not on average and not most of the time.

AC reverses polarity 120 times a second on a 60 Hz system. For a 60th of a second the structure would be cathodic; for the next 60th it would be anodic. Anodic means metal loss — exactly what CP exists to prevent. You don’t get net protection from polarity that flips on you that fast; you get a structure that is corroding for half of every cycle and protected for the other half, which from the structure’s point of view is no protection at all.

2. The reference electrode only reads steady DC.

The Cu/CuSO₄ half-cell, the silver/silver-chloride cell used in seawater work, the zinc reference embedded in some test stations — all of them depend on their own electrochemistry sitting at a stable potential. We measure structure-to-soil potential by reading the difference between the structure’s potential and the half-cell’s known fixed potential. A 0.94 V difference means something. A reading that swings from +6 V to −6 V at 60 Hz means nothing — the average is zero, and the only number the meter can extract from it (the AC RMS) doesn’t tell us anything about whether the structure is sitting at a protective potential.

The −0.85 V criterion is a DC criterion. Every CP criterion in every governing standard, every survey procedure, every coupon-based polarization measurement — all DC. There is no AC version because there can’t be one.

3. The electrolyte responds to direction, not magnitude.

Current flowing through soil from an anode to a structure isn’t a flow of electrons — it’s a flow of ions. Positively charged ions move one way, negatively charged ions move the other, and the electrochemical reactions at each electrode (oxidation at the anode, reduction at the cathode) only proceed if the ions keep moving in their respective directions. Reverse the polarity and the ions reverse too — and the chemistry that the CP system is trying to drive at the cathode unwinds in the half-cycle the polarity is wrong, then has to start over again.

If the current averages to zero over time, it does no net protective work. AC is the textbook example of a current that averages to zero. CP is the textbook example of a process that requires net work in a fixed direction.

Put the three together and the conclusion is unavoidable: CP requires unidirectional, polarity-stable current. The only way to deliver that on a system fed by utility power is to convert the utility AC to DC inside the rectifier. The transformer steps the voltage up or down. The rectifier diodes (or SCRs) flip every other half-cycle so the output is unidirectional. Filter capacitors smooth the result. What comes out of the cabinet onto the cable is DC — sometimes with a little ripple still on it, but DC at heart. That’s the system the rest of CP is built around.

AC on the pipeline — the second story

The first story — CP runs on DC — is the whole reason rectifiers exist. The second story is what happens when AC ends up on a pipeline that has nothing to do with the rectifier feeding that section.

A buried pipeline running parallel to a high-voltage transmission line for any significant distance is electromagnetically coupled to that line. The transmission line carries an AC current — typically tens to hundreds of amps at 60 Hz, depending on the line’s loading. The magnetic field around the line oscillates at the same frequency. That oscillating field cuts through the pipeline’s path, and the result is the same as the secondary winding of a transformer: an induced AC voltage and current on the pipeline itself.

Inductive coupling. The AC in the transmission line induces an AC voltage and current on the parallel pipeline below.

How big the induced AC ends up being depends on the geometry — how close the pipe runs to the line, how long the parallel run is, what the line’s current is, what the soil resistivity is along the route, and where the pipeline is grounded. On a long parallel run with a heavily-loaded line, induced pipe-to-soil AC voltages of several volts to tens of volts are not unusual. We saw 6.5 V AC at the test station in the hook; on heavier corridors, readings can exceed 50 V AC at unprotected points.

Why this matters — AC on the pipe is its own corrosion mechanism

What you read on the meter is V AC pipe-to-soil. What actually drives AC corrosion is the AC current density at coating defects (holidays). The two are linked — higher V AC means more current can leak through a holiday — but the corrosion mechanism lives in the current density, not the voltage reading itself. At around 4 V AC and above, conditions on a typical pipeline can support enough current density at holidays to drive AC-induced corrosion — a regime that proceeds independently of, and unmitigated by, the cathodic protection system. The mechanism involves alternating polarization at the holiday, partial film disruption during the anodic half-cycle, and pitting that continues even while the structure-to-soil DC potential meets the −0.85 V criterion. The exact V AC threshold varies with soil resistivity, coating quality, and holiday geometry; field practice uses the V AC reading as the trigger to investigate further.

AC interference is also a personnel safety issue. Industry standards generally treat 10 to 15 V AC and higher pipe-to-soil as a worker shock hazard — including for corrosion techs reading test stations, opening valve boxes, or working at flanges and other above-ground appurtenances. Even a few volts AC can be enough to deliver a startling shock under wet hands and a good return path; double-digit V AC pipe-to-soil reliably is. Mitigation systems address both the corrosion side and the safety side.

What’s NOT in this module: the design of AC mitigation systems — coupling models, induced-current threshold details, decoupling devices (gradient control mats, polarization cells, solid-state coupling devices), AC current density math at coating holidays, NACE SP21424 evaluation procedures. All of that lives in a later EC module dedicated to AC interference. EC-004 names the phenomenon and the mitigation gap; it does not work out the fix.

Three readings, three meter modes

Three measurement vignettes from real CP work. Each one shows the same lesson from a different angle: the meter mode is part of the measurement. Switching modes on the same lead pair gives different numbers because they are different questions.

Scenario A — At the rectifier cabinet

One enclosure, two regimes

Setup: impressed-current rectifier cabinet on a small distribution system. Inside, the AC service drop lands on the input lugs at the top. A transformer steps the voltage down. Diodes rectify. The DC bus runs out the bottom to the anode header and the structure return.

Reading 1 — input lugs, meter on V AC: 240 V AC line-to-line. That is the utility service feeding the cabinet. AC by design — the rectifier needs AC at the input to drive the transformer.

Reading 2 — output bus, meter on V DC: 22 V DC. That is the rectified output, what the system is actually putting on the cable that runs to the anodes and the structure. DC by design — that is the regime CP works in.

What it tells you: the rectifier is doing its job — converting the AC source into DC of the right magnitude for the system. The same enclosure spans two regimes; the regime changes as you move from the input side to the output side, and the meter mode has to follow.

Scenario B — At the test station next to the power line

The hook scenario, fully spelled out

Setup: test station on a pipeline running parallel to a 138 kV transmission line. Cu/CuSO₄ half-cell pressed into moist soil at the post, lead pair clipped from the half-cell to the pipe header.

Reading 1 — meter on V DC: −1.05 V. Structure-to-soil potential. More negative than the −0.85 V criterion. CP is working at this location.

Reading 2 — same leads, meter flipped to V AC: 6.5 V AC. Induced AC on the pipe from the parallel transmission line. At this level, conditions could support AC current density high enough at coating holidays to drive AC-induced corrosion — possible, not certain, and worth flagging for an AC interference review.

What each reading does and does not tell you: the −1.05 V says the CP system is delivering the protective potential the criterion calls for at this point. The 6.5 V AC says the pipe is sitting in a coupled-AC environment that will need its own purpose-built mitigation — not more rectifier current. Both are real measurements; both belong in the field notes; neither one tells the whole story without the other.

Scenario C — Ripple on the rectified output

Same conductor pair, V DC and V AC tell different stories

Setup: at the rectifier output bus inside the cabinet. The output is rated 24 V DC, and the system is operating below that.

Reading 1 — meter on V DC across the output: 22 V DC. The working DC level the system is putting on the cable.

Reading 2 — same leads, meter on V AC: 0.4 V AC. That is rectifier ripple — the residual AC component that survives rectification, riding on top of the DC level. For a full-wave rectifier on 60 Hz input, the ripple is at 120 Hz.

What it tells you: ripple under about 5% of the DC level (here, 0.4 ÷ 22 ≈ 1.8%) is normal for a healthy filtered rectifier. Ripple climbing to 10% or more can suggest a failing filter capacitor, a missing diode in a multi-diode bridge, or a transformer issue. The reading is a quick proxy for rectifier health that costs nothing to take and that fits naturally into a routine cabinet visit.

Meter-mode discipline

Every CP measurement starts with a question we mostly leave implicit: which regime is this reading actually in? The answer decides the meter mode (V DC vs. V AC, mA DC vs. mA AC), the unit interpretation (RMS vs. peak vs. steady-state), and what the reading actually means for the system.

The discipline that keeps the readings honest is small but non-negotiable: name the mode in the field notes. Write “−1.05 V DC,” not “−1.05 V.” Write “6.5 V AC,” not “6.5 V.” On a routine visit you will read both regimes on the same conductors within a few minutes of each other. The notebook entry that distinguishes them is what makes it possible — months later, after the visit is forgotten — to know which reading was which, and what each one was doing.

The CP-tester habit of always recording the meter mode comes from exactly this lesson. Two different regimes. Two different questions. Two different stories. The mode is part of the answer.

Back at the test station

Close the lid on the math for a minute and stand back at the test station you opened in the hook. Two readings on the same lead pair: −1.05 V DC and 6.5 V AC. Two different regimes, two different questions, two different parts of the field-notes page.

The DC reading was the CP question. The −1.05 V Cu/CuSO₄ potential meets the −0.85 V criterion with a comfortable margin, and that is the only thing the CP system itself is responsible for. The rectifier feeding this section is doing its job. The pipe is at a protective potential. From the rectifier’s point of view, the visit could end here.

The AC reading is something else. The 6.5 V AC is induced from the transmission line above and has nothing to do with the CP rectifier — turning the rectifier output up to 28 V or down to 16 V will not change that 6.5 V. The 6.5 V is on its own work track: AC interference assessment, soil and coating evaluation, mitigation design with decoupling devices and gradient control where warranted, and ongoing monitoring. That track does not run through this module — it runs through later work in this rung and beyond.

What the field-notes page captures, then, is two readings on two regimes, distinguished by mode, both real, neither one swept up by the other. The math gives you the numbers; the meter mode tells you which question the numbers are answering; the job tells you what to do with each.

Side by side — DC and AC at a glance

Aspect	DC	AC
Direction	Constant in one direction; fixed (+) and (−)	Reverses periodically; 120 reversals per second at 60 Hz
Waveform	Flat horizontal line over time	Sine wave; rises and falls smoothly above and below zero
Voltage description	Single steady value	Peak and RMS; for sine waves, `V_RMS = V_peak × 0.707`
Where it lives in CP	Rectifier output, galvanic anode bonds, structure-to-soil readings, shunts, batteries	Utility input to rectifier, induced on pipelines from parallel power lines, ripple on rectified output
Meter mode	V DC, mV DC, A DC	V AC, mV AC, A AC
Role in CP	The regime CP runs in — protective work happens here	Source for rectifier conversion, plus a separate interference phenomenon to manage on the pipeline

Key takeaways

DC flows constantly in one direction. Voltage and current sit at steady values. Plotted against time, DC is a flat line. Rectifier output, galvanic anode bonds, structure-to-soil potentials, and shunt readings are all DC.
AC reverses direction periodically. US utility AC is sinusoidal at 60 Hz — 120 reversals per second. AC voltages are usually quoted as RMS; for a sine wave, V_RMS = V_peak × 0.707 and V_peak = V_RMS × 1.414.
CP requires DC. Polarity must be fixed for the structure to remain cathodic; reference electrodes only return interpretable readings against DC; ions in the electrolyte respond to direction, not magnitude. AC averages to zero and provides no net protection regardless of magnitude.
Rectifiers convert utility AC to DC. The transformer scales the voltage; diodes flip every other half-cycle so the output is unidirectional; filtering smooths the result. What comes out of the cabinet onto the cable is DC, often with a small ripple riding on top.
AC on a pipeline is a separate problem with its own mitigation track. Inductive coupling from parallel transmission lines, ground-fault events, and other sources can put several volts AC pipe-to-soil on a buried structure. At around 4 V AC and above, conditions can support enough AC current density at coating holidays to drive AC-induced corrosion — independent of the CP system, which does not mitigate it. 10 to 15 V AC and higher is also a worker safety threshold at exposed appurtenances per industry standards.
Meter-mode discipline matters. The same conductor pair reads different numbers on V DC versus V AC because they are different questions. Always record the mode in field notes — “−1.05 V DC,” “6.5 V AC” — never just “the volts.”
One conductor pair can carry two readings. At a test station next to a power line, a single pipe-to-soil clip pair gives both a CP-criterion reading on V DC and an AC-interference reading on V AC. Both belong in the notes; neither one substitutes for the other.

References & further reading

AMPP CP 1 Cathodic Protection Tester Course Manual — foundation treatment of AC and DC, peak vs. RMS, transformers, and rectification.
AMPP CP 2 Cathodic Protection Technician Course Manual — extended treatment of rectifier operation, ripple, and rectifier types.
AUCSC Basic Course Manual — companion treatment with utility-side context and an introduction to AC interference on pipelines.
Peabody’s Control of Pipeline Corrosion — A.W. Peabody. Load-bearing DC framing alongside the pipeline-side AC story.
Corrosion Basics: An Introduction — foundation cathodic protection alongside AC-on-pipelines.
AC Corrosion of Pipelines — Brenna, Lazzari, Ormellese, et al. Modern treatment of induced AC and its consequences on buried pipelines.
Corrosion Engineer’s Reference Book — Robert Baboian, ed. General electrical reference covering AC and DC fundamentals, conductor properties, and rectification.
NACE/AMPP SP21424 — the standard governing AC mitigation engineering on pipelines.

Apply — three problems

Read the regime

Three readings. Three different questions about the same conductors. Each one rests on the same discipline the L1 walked through: name the regime, set the meter mode, and read the number for what it actually says — not what you might want it to say. Work each problem in your head or on paper before clicking the steps to compare.

How to use this lesson. Read the setup. Solve before you click. Each step reveals our working — match your answer; if it doesn’t match, the steps are there to compare against.

Problem 1 · Two readings, one bus

Rectifier output health from the same conductor pair

Setup. You’re at the cabinet of an impressed-current rectifier on a 36-mile section of distribution. The cabinet plate says 50 V / 30 A rated output. You clip your meter leads across the rectifier’s positive and negative output bus bars, set the meter to V DC, and read 18.5 V. Same leads, same bus, you flip to V AC — display reads 0.6 V AC.

What is each number telling you, are they consistent with a healthy rectifier, and what action (if any) do they drive?

Step 1 — name what each reading is

Two regimes, two stories on the same conductor pair:

18.5 V DC is the working output — the steady DC level the rectifier is putting on the cable that runs out to the anode header. This is the regime CP runs in.
0.6 V AC is the residual ripple — the AC component that survives rectification and sits on top of the DC level. For a full-wave rectifier on 60 Hz utility input, ripple is at 120 Hz.

The same physical leads, the same bus bars, two completely different things being measured. The mode is the question.

Step 2 — express the ripple as a percentage of the DC level

Ripple is conventionally reported as a percentage of the DC output:

ripple % = V_AC ÷ V_DC × 100%

= 0.6 ÷ 18.5 × 100% ≈ 3.2%

So the rectifier is delivering 18.5 V of working DC with about 3.2% ripple riding on top of it.

Step 3 — compare to healthy bands

Typical healthy ranges for a filtered impressed-current rectifier:

Under ~5% ripple — normal. Filter capacitors are doing their job; output is clean enough that the structure sees a steady protective potential.
5–10% ripple — worth a closer look on the next visit. Possibly a slightly weak filter; not an emergency.
Over ~10% ripple — investigate. Likely candidates: failing filter capacitor, missing or shorted diode in a multi-diode bridge, or a transformer issue.

3.2% sits comfortably in the “normal” band. The rectifier is healthy.

Step 4 — what these readings do and don’t tell you

The DC reading speaks to output magnitude — the rectifier is delivering 18.5 V at the bus, well below its 50 V ceiling, so the system has plenty of headroom if anode consumption or rising soil resistance demands more push later. Whether 18.5 V is the right output depends on the structure-to-soil potential survey along the line — that’s a separate measurement campaign at the test stations, not something this cabinet reading answers.

The AC reading speaks to output quality — the DC the rectifier is producing is clean enough that the system is doing its job without the structure seeing a noisy potential. That’s a quiet finding; it doesn’t drive any action today, but the cabinet visit captured it for the trend.

Action: log both numbers, no further intervention needed at the cabinet today, and walk the test stations next.

One conductor pair, two meter modes, two independent readings. The DC speaks to magnitude, the AC speaks to quality. A healthy rectifier produces a steady DC output with small AC ripple — and the small AC reading is itself a quick proxy for filter health that costs nothing to take.

Problem 2 · Peak vs. RMS

Reading the transformer’s primary-side waveform

Setup. An oscilloscope probe is on the primary-side terminals of a CP rectifier’s input transformer — the AC service drop, before any rectification. The scope shows a clean sine wave with a peak voltage of V_peak = 170 V. The cabinet’s input nameplate says it expects a single-phase service of “120 V.”

What is the RMS voltage, does it match the nameplate, and why does the catalog rating not just list 170 V?

Step 1 — convert peak to RMS

For a clean sine wave:

V_RMS = V_peak × 0.707

V_RMS = 170 V × 0.707 ≈ 120 V RMS

The 0.707 factor comes from 1 ÷ √2 — derived from integrating the squared waveform over one cycle and taking the root of the average. For a sinusoid, that integration always lands on this same constant.

Step 2 — cross-check by going the other direction

If RMS is 120 V, the peak should be:

V_peak = V_RMS × 1.414

V_peak = 120 V × 1.414 ≈ 169.7 V

That matches the 170 V the scope is showing (within reading precision). The arithmetic closes both directions — the conversion factors are reciprocals: 0.707 × 1.414 ≈ 1.000.

Step 3 — does the reading match the nameplate?

The nameplate calls for a 120 V service. The scope is showing 170 V peak, which is 120 V RMS. The reading matches the nameplate — because catalog and nameplate ratings for AC are RMS by convention, not peak.

This convention is everywhere in the trade: a “240 V” service is 240 V RMS (peak ≈ 339 V); a “480 V” three-phase line is 480 V RMS line-to-line (peak ≈ 679 V). When a tag says volts on an AC line, it almost always means RMS volts unless explicitly labeled otherwise.

Step 4 — why use RMS, not peak, for the catalog

RMS is the equivalent steady DC voltage that would deliver the same average power into a resistive load. So a 120 V RMS source heats a resistor at the same rate a 120 V DC source would, even though the AC waveform is swinging up to 170 V on each peak. RMS is the right number for power, current ratings, breaker sizing, and anything else where the average effect over time is what matters.

Peak voltage matters when insulation breakdown is the question — the insulation has to withstand the highest instantaneous voltage, which is the peak. So nameplate ratings list RMS for normal operation; insulation specs list peak (or its first cousin, “peak-to-peak”) for dielectric work.

For CP work, the only AC voltage we typically need to convert between peak and RMS is the rare scope reading like this one. Field meters on V AC mode read RMS directly, so the 0.707 / 1.414 conversion is mostly a hand-tool for interpreting an oscilloscope or a manufacturer datasheet.

Peak and RMS are two ways to describe the same sine wave, and they are linked by a fixed factor: 0.707 down from peak, 1.414 up from RMS. The trade quotes RMS by convention because RMS is the right number for power and current ratings — what the AC actually does, on average, into a load.

Problem 3 · CP-on plus induced AC

One conductor pair, two regimes, two questions

Setup. A scheduled survey visit at a test station on a pipeline that runs roughly 200 ft from a 230 kV transmission corridor. Cu/CuSO₄ half-cell pressed into moist soil at the post; lead pair clipped from the half-cell to the pipe header. Same leads, both readings:

V DC reading: −1.08 V
V AC reading: 5.2 V AC

Is the structure protected at this location, and what (if any) action does the AC reading drive — including whether it is something the rectifier feeding this section can address?

Step 1 — interpret the DC reading against the CP criterion

The DC reading is a structure-to-soil potential, referenced through the Cu/CuSO₄ half-cell. The classic CP criterion for a buried steel structure is −0.85 V Cu/CuSO₄ or more negative.

−1.08 V is more negative than −0.85 V ✓

The pipe meets the criterion at this location with comfortable margin — about −1.08 − (−0.85) = −0.23 V below the criterion floor. From the CP system’s point of view, this location is protected.

Step 2 — interpret the AC reading against the AC threshold

The AC reading is on the same conductor pair but a completely different regime — induced AC, almost certainly from the parallel transmission corridor. Above roughly 4 V AC pipe-to-soil (the exact threshold varies with soil and coating), AC current density at coating defects can reach levels that drive AC-induced corrosion independently of the CP system.

5.2 V AC is above the 4 V threshold — this site has AC interference at a level worth investigating.

It’s also at a level worth taking seriously as a personnel safety question. Several volts AC on a pipe is enough to give a hazardous shock to a worker contacting the pipe and ground at the same time at an above-grade flange or test station.

Step 3 — does increasing rectifier output help?

No. The AC on the pipe is induced from the transmission line above; it has nothing to do with the rectifier feeding this section. Pushing the rectifier output from (say) 22 V DC to 28 V DC drives the structure-to-soil potential more negative — useful for CP — but does nothing to the 5.2 V AC, because that reading is set by the geometry and loading of the power line, not by the rectifier.

This is one of the most common misreadings in early CP work: treating an AC pipe-to-soil reading as a CP problem. It isn’t. The CP system is doing its job at this location (the −1.08 V DC says so). The 5.2 V AC is a separate finding.

Step 4 — what the AC reading drives, instead

The 5.2 V AC sets up a different chain of work, on its own track:

Document and trend — log the reading, compare against prior visits, note the local coating condition and access points.
Soil resistivity at the corridor — drives mitigation device sizing.
Mitigation design — gradient control mats, polarization cells, solid-state coupling devices, additional grounding at peak-AC locations. All of this is a separate work track from CP.
Personnel safety controls — at above-grade fittings inside the AC zone, signage and step-and-touch potential measures may be warranted.

None of those steps is a rectifier adjustment.

Step 5 — record both readings, name the mode

The field-notes entry should capture both regimes, distinguished by mode:

−1.08 V DC, Cu/CuSO₄ reference, half-cell at post
5.2 V AC, same lead pair

Months from now, when this visit is forgotten, that mode-tagged entry is what makes it possible to know which reading was the CP question and which was the AC-interference question. Two readings, two regimes, two work tracks — and the only thing keeping them straight on the page is the mode tag.

The DC reading and the AC reading are answering different questions about the same pipe. The CP system owns the DC answer; AC interference work owns the AC answer. More rectifier current does not reach the AC reading at all.

Three readings, three meter modes, three different questions about the same conductors — and the same shape of work behind each: name the regime, set the mode, read for what the number actually says, and route the finding to the right work track. That’s the practice.

Most of the readings you take in a working career will be DC — that’s the regime CP runs in. But the AC reading is real, the AC reading is increasingly common as transmission corridors and pipelines share more right-of-way, and the AC reading deserves the same disciplined treatment as the DC one.

Up next: a quiz to confirm the regimes and the meter-mode discipline are wired in.