Is Stick Welding Hard? An Honest Beginner’s Guide
My neighbor Dale bought a beat-up 225-amp stick welder at a yard sale for forty bucks, dragged it…
READ ARTICLE →You’ve got a piece of 1/8-inch steel on the bench, a brand-new E6013 rod, and a dial that runs from 20 to 200 amps. You flip the switch, strike an arc, and either the rod freezes to the plate or you burn a hole clean through it. The difference between those two failures was probably less than 20 amps — and finding that number is exactly what this guide is about.
Stick welding, or shielded metal arc welding (SMAW), is a constant-current (CC) process. That single fact explains almost everything about how you set up a machine. Before the arc even starts, you choose an amperage based on two things: the electrode you’re running and the thickness of the metal you’re welding. Once the rod touches the plate, that setting stays essentially fixed. The power source adjusts voltage to keep the current steady as your arc length changes, but it won’t quietly re-tune your heat for a thinner section or a fat root pass. You have to think it through first.
Quick Note: In SMAW the amperage dial is your heat control — not a wire-feed speed, and not a voltage knob. Set it correctly and the rod burns smooth; set it wrong and no technique can rescue the weld.
That’s a very different mindset from wire-feed welding, where the machine and your travel speed work together to control heat as you go. With gasless MIG (flux-cored) or solid-wire MIG, if a joint starts running hot you simply move faster or dial the voltage down mid-bead. In stick, you commit to a number before you start. That’s why planning matters so much: pick the wrong amperage and you’ll spend the whole bead fighting the arc instead of welding.
Base metal thickness and electrode diameter are the two numbers that drive your amperage. Thicker steel pulls heat away from the arc faster, so it needs more current to reach proper penetration. A larger electrode also needs more amps to burn correctly, but it can’t be run so hot that it melts the base metal underneath it. Balance those two against each other and the arc behaves; ignore one and you get sticking, spatter, or burn-through.
A widely used starting rule of thumb for steel is roughly 1 amp per 0.001 inch of material thickness — about 30 amps per 1/32 inch — for general work. It’s a good place to begin, not a law. Electrode type matters just as much: E7018 is the workhorse for thick structural steel, while E6013 is the go-to for thin sheet metal. The American Welding Society’s AWS A5.1/A5.1M specification governs those carbon steel covered electrodes, and electrode makers such as Miller publish amperage ranges keyed to those codes.
The sections ahead build a complete, repeatable system for setting amperage on any stick job:
Stick welding is famously forgiving about the metal itself — it will happily burn through rust, mill scale, and light dirt that would ruin a MIG bead. It is far less forgiving about amperage. Get the current close and the process feels almost easy; get it wrong and even perfect travel angle and arc length won’t save you.
By the end, you’ll be able to look at a joint, pick an electrode, and dial in a starting amperage with confidence — then fine-tune it on the first inch of the bead. Amateur stick welders guess; good ones follow a repeatable system. Let’s build yours, starting with what the amps are actually doing inside the arc.
Amperage is the master variable in stick welding. It’s the one number you actually dial in, and it decides how hot the arc runs, how deep it bites into the plate, and how fast the rod melts. Change nothing else and bump the amps by 15 to 20, and you get a completely different weld. So before you memorize any chart, it helps to understand what that dial is really doing.
Electrical current flowing through the electrode creates resistance heating, and that heat melts both the rod tip and the base metal. Amperage controls the quantity of that heat. More amps mean a hotter arc, deeper penetration, and faster deposition; fewer amps mean a colder arc that struggles to fuse.
Here’s a detail lots of beginners miss: it isn’t raw amperage alone that drives behavior, it’s current density — amps per square inch of electrode cross-section. A 1/8-inch E6013 running 90 amps has far more current packed into each square inch of its core than a 5/32-inch rod running 90 amps. That crammed current is why thin rods melt fast and dig deep, and why a fat rod at low amps just sits there and stubs.
This is why a thicker electrode happily carries more total amps: the current spreads across a larger cross-section, so the density stays in a workable band even as the absolute number climbs. Match amps to the rod’s diameter and you keep density in range automatically.
Quick Note: A 3/32-inch rod and a 5/32-inch rod might both list 100 amps, but only one runs that current through a cross-section small enough to melt steel efficiently. Always match amps to diameter first, then fine-tune for thickness.
Heat input for arc welding can be estimated as:
(amperage × voltage × 60) ÷ travel speed (inches per minute) = joules per inch
Notice what’s in there. Amps, volts, and how fast you move. Amperage is the biggest lever, but travel speed matters too — drag the arc slowly and even modest amps pile heat into the part. That’s why turning the machine down isn’t the only fix for burn-through; moving faster works as well.
Note: In SMAW, arc voltage is largely a function of arc length, not a dial setting. A long arc raises voltage; a tight arc lowers it. Since amperage is the variable you directly control, it becomes the welder’s primary adjustment.
Thick steel acts like a heat sink — it pulls heat away from the joint, so it needs more amperage to reach fusion temperature across the full thickness. Thin sheet has almost no mass to absorb heat, so the same amps that flatter 1/4-inch plate will blow a hole through 16 gauge.
The consequence of getting it wrong is predictable. Too-low amperage gives you a cold, stubbing arc that sticks and pops, with poor fusion and cold lap — the weld metal sits on top of the plate instead of melting into it. Too-high amperage on thin stock causes burn-through, and on any thickness it brings undercut, excessive spatter, and an overheated electrode whose flux coating degrades and flakes.
None of this is guesswork once you can read the arc. The complete guide to building real welding skills is full of this kind of feedback training — learning to hear and see what the puddle is telling you. Miller’s electrode behavior guide echoes the same point. If you’re used to wire processes, the same heat logic appears in flux-cored welding without gas, though the arc characteristics differ. And when you eventually graduate to automatically fed processes, heat input becomes a formal spec — see robotic submerged arc welding for heavy-duty work.
Get amperage right and everything downstream — bead appearance, penetration, spatter level, and even your own fatigue — falls into place.
If amperage is the engine of a stick weld, electrode diameter is the gearbox. The two are locked together, and neither makes sense without the plate thickness in front of you. Get the pairing wrong and you’ll spend the afternoon either stubbing rods or blowing craters through your workpiece.
Experienced welders carry one rule in their heads: match the electrode diameter to the base metal thickness. Thin metal wants a small rod — 3/32-inch or 1/8-inch. Thick plate wants a big one — 5/32-inch or 3/16-inch. It isn’t physics, but it’s the starting point that keeps you in the ballpark before you fine-tune amps on scrap.
Amperage scales with the electrode’s cross-sectional area. A 1/8-inch rod has roughly 78% more metal cross-section than a 3/32-inch rod, so it carries far more current without overheating its flux coating or melting back uncontrollably. More current across that larger area means a higher deposition rate — the volume of filler laid down per hour.
That’s the logic of stepping up on thick steel. A 3/16-inch plate needs deep penetration and enough deposited metal to fill a joint. A 3/32-inch rod can’t deliver that volume in a reasonable number of passes; you’d chase a mountain of stringer beads all day. Jumping to a 5/32-inch E7018 lets you push more amps, deposit more metal per pass, and finish the job. The trade-off is heat: big rods punch straight through thin sheet. For context, see our guide to 3/16 E7018 amperage, polarity, and technique.
Quick Note: Electrode diameter sets your amperage ceiling. Base metal thickness decides which of those rods is appropriate. Always pick the rod from the plate first, then dial amps within that rod’s range.
Thickness alone doesn’t tell the full story. Joint geometry determines how much heat a section can absorb before it distorts or burns through. Consider the differences:
Root opening and bevel angle are levers you control. Widen the root and you reduce effective thickness at the joint face, making burn-through more likely. A bevel gives you room to deposit metal without cranking amps sky-high. Fit-up discipline pays off here — our fit-up and welding guide for tube fittings shows how small gaps change heat input dramatically.
Note: Preheating shifts the effective thickness calculation. Warm a thick section and the steel near the joint no longer wicks heat away as aggressively, so you can often weld like the part is thinner than it measures. AWS D1.1 ties minimum preheat to the combined thickness of parts — not just the thickest piece — because two 1-inch plates joined in a T behave like a 2-inch mass for heat flow.
Before striking an arc, ask three questions: How thick is the metal? What joint am I filling? Is it preheated? A 1/8-inch plate in a lap joint might happily take a 1/8-inch rod at 110 amps. The same plate butted with a wide root may only tolerate 85. The rod matches the metal; the joint and preheat tell you where inside that range to land. Build the muscle memory through deliberate repetition — our guide to building real welding skills covers how to speed that up.
Get diameter and thickness aligned and you’ve solved half the amperage puzzle before you touch the dial.
Every stick electrode has a personality, and that personality is encoded in its AWS classification. The “E” means electrode, the next two digits give minimum tensile strength in ksi, and the final two identify the coating and the usable current type. So E7018 is a 70,000 psi, low-hydrogen electrode. The AWS A5.1 specification spells out every class in painstaking detail; here’s what those numbers actually mean when you’re standing at the stinger, rod by rod.
Quick Note: The first two digits are tensile strength in ksi, so E60XX is 60,000 psi and E70XX is 70,000 psi. The trailing digits (10, 11, 13, 18, 24) describe the coating and the current each one tolerates.
A cellulose coating gives E6010 a forceful, spray-like arc that digs deep into the plate, making it the choice for open-root and pipeline work. It’s a fast-freeze rod with almost no slag to fight, which keeps the puddle controllable on a steep root. The catch: it’s DCEP only and will not run on AC. Typical windows are 3/32 in at 40–80 A, 1/8 in at 75–125 A, and 5/32 in at 110–165 A.
Same cellulose family, but potassium is added for arc stability on alternating current. It runs on AC or DCEP and delivers much the same deep penetration, which is why it’s a favorite for repair work and dirty, rusty steel. Ranges: 3/32 in at 40–85 A, 1/8 in at 75–125 A, 5/32 in at 110–160 A. Expect a little more cleanup than a 6010, but far more flexibility at the machine.
E6012 uses a rutile-sodium coating that produces a stiff, low-penetrating arc with good gap-bridging ability—handy for poorly fitted joints and lighter sections. It runs on AC or either DC polarity, and its shallower bite makes it forgiving on thin material or a joint that’s been tacked a hair too wide.
E6013 is the beginner’s friend: a soft, stable arc with shallow penetration and a clean finish. It works on AC, DCEP, or DCEN, which makes it forgiving on thin sheet and general fabrication. Watch for cold lap on thick plate—run hotter and slower. Ranges: 3/32 in at 40–90 A, 1/8 in at 80–130 A, and 5/32 in at 110–180 A; 1/16 in rods run roughly 20–45 A. Build consistency with the drills in our welding practice guide.
Iron powder in the coating boosts deposition and smooths the arc beyond E6013, while keeping easy striking and slag control. Run it on AC or DC, mostly for flat and horizontal work where you want a clean bead with less fuss.
The “18” signals a low-hydrogen, iron-powder coating that needs dry storage and prefers DCEP. It’s the structural standard. Ranges: 3/32 in at 65–110 A, 1/8 in at 90–160 A, 5/32 in at 130–220 A, and 3/16 in at 200–275 A. For the big rod in detail, see our 3/16 E7018 amperage guide.
Heavy iron-powder E7024 lays metal down fast when dragged at a tight angle—flat and horizontal fillets only. 1/8 in runs 140–190 A; 5/32 in runs 180–250 A. Don’t take it vertical or overhead. Current type reshapes every arc here, so our polarity for flux core welding breakdown is worth a look.
| Electrode | 3/32 in | 1/8 in | 5/32 in | 3/16 in |
|---|---|---|---|---|
| E6010 | 40–80 A | 75–125 A | 110–165 A | — |
| E6011 | 40–85 A | 75–125 A | 110–160 A | — |
| E6013 | 40–90 A | 80–130 A | 110–180 A | — |
| E7018 | 65–110 A | 90–160 A | 130–220 A | 200–275 A |
| E7024 | — | 140–190 A | 180–250 A | — |
Treat these as starting points, not gospel—machines, lead length, and joint fit all vary. The Miller electrode guide and every manufacturer’s data sheet give the same ballpark, so dial in, run a test bead, and adjust from there. Keep a scrap plate nearby and burn a test bead before every critical joint—a slight tweak in amperage often matters more than a whole change in rod.
Here is the chart I wish someone had handed me the first time I burned a hole straight through 16-gauge sheet. Read it as a launch pad, not a landing strip. Every number below assumes clean steel, snug fit-up, and flat-position work — change any one of those and you will be nudging the dial within the first inch of bead.
| Base Metal Thickness | Starting Electrode | Amperage Range | Polarity Notes |
|---|---|---|---|
| 1/16 in and thinner | 3/32 in E6013 | 40–70 A | DCEP; switch to E6011 if fit-up is sloppy |
| 3/32 in | 3/32 in E6013 / E6011 | 60–90 A | DCEP typical, DCEN for more bite |
| 1/8 in | 1/8 in E7018 | 75–120 A | DCEP for structural work |
| 3/16 in | 1/8 in E7018 | 110–140 A | DCEP |
| 1/4 in | 1/8 in E7018 | 90–160 A | DCEP preferred |
| 3/8 in | 5/32 in E7018 / E6010 | 150–220 A | DCEP for low-hydrogen rods |
| 1/2 in and up | 5/32–3/16 in E7018 | 180–250 A | DCEP; bevel and run multiple passes |
For the thin end of the scale — 1/16 through 1/8 inch — a 3/32-inch electrode at roughly 40–90 A handles almost anything you throw at it. Reach for E6013 on the thinnest stock, because its softer arc and lighter flux resist burn-through far better than a fast-freeze rod. If the metal is dirty or the gap is wide, a 3/32-inch E6011 still fits the same amperage window and tolerates the mess.
Once you cross into 1/8 through 1/4 inch, step up to a 1/8-inch electrode and roughly 75–160 A. This is where E7018 on DCEP earns its reputation as the structural default. A quarter-inch plate run with 1/8-inch E7018 is frequently cited at 90–160 A on DCEP, and our breakdown of 3/16 E7018 amperage and technique shows how much that window shifts with joint design.
From 1/4 to 3/8 inch, a 5/32-inch electrode at roughly 110–220 A gives you enough deposition to fill a bevel without spending all afternoon. The exact figure depends heavily on electrode class — a 5/32-inch E6010 lives near the top of that range, while a low-hydrogen E7018 sits lower for the same thickness. Half-inch plate and up usually means several passes rather than one heroic run.
DCEP (electrode positive) runs hotter into the workpiece and gives deeper penetration, which is why the structural rods lean on it. DCEN favors deposition, and it is the standard for E6010 and many cellulosic electrodes. If you are sorting out which current type belongs to which process, our guide to TIG welding polarity unpacks the same DCEN/DCEP logic in a different context.
Manufacturers publish their own data — the AWS A5.1 specification and Miller’s electrode guidance both give ranges rather than single numbers — precisely because real settings move with fit-up, position, machine, and alloy. Thin plate with a gap needs less heat than tight plate. Thick plate that is cold needs more. A worn machine with a long lead may deliver less than the dial promises.
Out-of-position work is the big one. For vertical-up, overhead, or any out-of-position welding, manufacturers often recommend cutting amperage by about 15 percent from the flat-position optimum. That single adjustment keeps the puddle from running away from you.
Quick Note: Before you trust any chart, grab a scrap coupon of the same thickness and run a test bead. Two minutes on scrap tells you more about your machine than an hour of guessing — the same philosophy behind our welding practice guide.
When the bead sits proud and cold, or the arc keeps sticking, add 5–10 A. When the rod digs in, the puddle spreads, or you are burning through, drop 5–10 A first. If you have already dropped below the electrode’s minimum, change techniques instead — shorten the arc, switch to a smaller rod, or adjust travel angle. Thick, heavily restrained joints may also call for preheat, a step the NCDOT approved welding procedures spell out for structural steel. Getting your shop set up for that kind of work is easier from the start; see our welding facility planning guide.
Print the table, tape it near the machine, and treat it as a compass. The needle that actually matters is the sound and look of the arc — and that comes from practice, not print.
Amperage charts quietly assume one thing you rarely get on a real job: a flat, well-fitted joint. The moment you tilt the work, switch the joint style, or leave a gap, the “correct” number shifts. The dial has no idea whether you’re overhead or welding a square-groove root—it just delivers whatever current you set. Understanding why position, geometry, and fit-up move your target keeps you from blaming the machine for a problem gravity or a loose fit caused.
On a flat or horizontal run, the puddle sits in the joint with nowhere to fall, so you can push heat and travel fast. Go vertical or overhead and gravity turns against you—too many amps and the puddle sags, drips, or balls up before it freezes. The molten metal grows heavier exactly when you need it to stay put, and a puddle that outruns its freeze line droops at the toes or leaves a hole behind.
That’s why out-of-position work calls for lower amperage. Manufacturers commonly suggest roughly a 15 percent reduction from your flat-position setting when moving to vertical-up or overhead. If 120 amps lays a clean flat bead, dial toward 100–105 for vertical-up and tighten your arc length so the arc stays short and focused. Miller’s electrode guidance makes the same point: lower the current for vertical and overhead to keep the puddle controllable. Overhead raises the stakes again, since the puddle hangs above you and any extra heat sends it searching for a path down.
Quick Note: If your flat beads look great but vertical-up turns soupy and convex, drop about 10–15 percent off the dial before you blame the rod. Out-of-position welding is a heat-control game, not a power game.
Geometry controls how fast heat escapes and how much metal you must deposit. A butt joint with a wide root opening invites burn-through because there’s little steel to soak up heat—so you either cut amps or bridge faster with a soft arc like E6013. A tight, unbeveled joint is the opposite: heat has nowhere to go, and a gentle arc just skates across the surface without fusing the root. That’s where a digging electrode like E6010 or E6011 earns its keep, driving penetration into square-groove fits.
T-joints and laps trap heat in the corner, while corners and free edges run hotter because less mass surrounds the arc. Thick plate acts as a heat sink and wants more amps; thin sheet punishes every extra amp with warpage. Root gap widens the same way—an open root needs less current or a faster bridge, while a closed fit needs more penetration. Setup matters here too—clean, consistent fit-up saves more amperage headaches than any dial tweak. Our guide to weld tube fittings and fit-up breaks down how small gaps change heat behavior.
A slight weave on vertical-up lets you control the puddle without cranking amps—the oscillation spreads heat and lets the toes freeze as you climb. Stringer beads suit tight roots and thin material, where a weave would simply overheat the joint. Travel speed is your fastest adjustment: speed up to cool the puddle, slow down to fill and widen; travel angle and arc length fine-tune the rest. On out-of-position passes, nudge speed and arc length first, then amperage last.
Note: Many welders chase poor technique with the dial. If beads are lumpy, wandering, or inconsistent, fix arc length and travel speed before touching the amps—that’s a habit worth drilling in early. Our welding practice guide and the 3/16 E7018 amperage breakdown both show how technique and settings interact. Remember, position, joint, and fit-up decide your starting point—not your final answer. Verify procedure limits against AWS D1.1 when the work is structural.
Two welders can set the dial to 120 amps, run the same E7018 rod, and still produce completely different beads. The difference isn’t technique—it’s polarity. Current type and direction decide where the arc’s heat lands, and that one factor can make an amperage that runs beautifully on DC feel sluggish or too hot the moment you flip to AC.
In stick welding, “polarity” simply means which cable the electrode holder is connected to. That connection decides whether most of the arc’s heat pours into the base metal or into the rod itself.
Direct current electrode positive (DCEP, also called reverse polarity) concentrates more heat in the workpiece. Electrons strike the plate and dump their energy there, producing a wider, deeper penetrating arc with strong fusion at the root. This is the go-to polarity for structural work.
It’s why E7018—a low-hydrogen electrode classified under AWS A5.1—performs best on DCEP. Low-hydrogen rods are widely specified for structural fabrication under codes like AWS D1.1 because their coating resists the hydrogen that causes cracking, and DCEP gives the stable, penetrating arc those procedures call for. For a full breakdown of settings on this rod, see our guide to 3/16 E7018 amperage.
Reverse the leads to direct current electrode negative (DCEN, straight polarity) and heat shifts toward the electrode tip. The rod melts faster, giving you higher deposition and a shallower, wider bead with less dig into the plate.
That’s useful when you want to fill metal quickly without burning through edges, but it’s the wrong choice when you need root penetration.
Alternating current flips between the two states many times a second, so the arc behaves like a blend of both—mild penetration, decent deposition, and a softer, less directional arc that helps tame arc blow on magnetic steel. Many electrodes are designed to run on AC or DC, which makes a basic AC buzz box surprisingly versatile.
That heat balance is also why AC machines sometimes need a slightly hotter dial to match a DC bead of the same thickness—the arc extinguishes and re-strikes every half-cycle, so a little energy is lost at each zero crossing and the arc feels less concentrated.
Not every rod is flexible, and forcing the wrong polarity is a rookie trap:
Here’s the practical takeaway: swapping polarity doesn’t just change the bead shape, it changes what a given number on the dial actually does. Flip from DCEN to DCEP at the same amperage and that setting—which felt gentle a minute ago—now digs hard. Flip the other way and you’ll lose penetration.
So treat polarity and amperage as a package. If you change one, re-test the other on scrap before running a real joint. The same logic applies across processes; our TIG polarity guide walks through how DCEN, DCEP, and AC behave. If you weld with wire instead of rod, the same trade-off shows up in flux core polarity.
Quick Note: Match polarity to the electrode’s spec sheet first, then dial amps to the thickness. Wrong polarity can’t be fixed by cranking the machine.
The best way to make polarity instinctive is repetition. Practicing deliberate polarity changes—and watching how the arc responds—builds the judgment that a chart alone can’t teach. If you’re still building those hours, our welding practice guide lays out drills that make the difference obvious.
An amperage chart gets you in the ballpark, but the arc and the finished bead are the real instructors. Learning to read symptoms and change exactly one variable at a time is what turns a guess into a repeatable setup.
A rod that continually sticks to the plate or stubs out before it can establish an arc almost always signals amperage that’s too low. The electrode can’t melt fast enough to keep pace, so the tip fuses to the workpiece the instant you touch down. An excessively long arc and a damp electrode produce the same symptom – moisture in the flux conducts poorly and drags the arc down.
Raise the amperage in small steps of 5–10 amps, shorten your arc length, and dry or replace suspect rods before touching the dial again.
Blowing holes through sheet is the classic sign of excessive amperage or an electrode that’s simply too large for the thickness. A 1/8-inch E6013 that runs beautifully on 3/16-inch plate will cut straight through 16-gauge. Drop to a smaller diameter, cut amps, and either increase travel speed or try a series of tack welds to manage heat. Sheet work rewards patience over power.
A crackling, unstable arc that showers spatter points to amperage that’s too high, or travel that’s too slow for the heat being poured in. Back the amps down a notch, verify your polarity and current setup matches the electrode spec, and pick up the travel speed. If spatter persists after that, the electrode may be damp or the wrong type for the current.
Undercut – those grooves melted into the base metal along the edges of the bead – usually means too much amperage or travel that’s too slow, letting the arc wash out the sidewalls. A travel angle that leans too far in one direction makes it worse. Reduce heat slightly, hold a consistent 10–15° drag angle, and let the puddle fill the edges before moving on.
A high, rounded bead sitting on top of the plate without biting in is a cold weld. The arc never penetrated the sidewalls. Increase amperage, tighten arc length, and slow down just enough for the toes to wet in. This is where deliberate practice on scrap plate makes all the difference – you feel the puddle open up as the amps come up.
Gas holes in the bead are usually a technique or moisture problem rather than an amperage one. Long arcs, dirty metal, damp electrodes, and excessive travel speed all trap gas. Clean the joint, shorten the arc, and store low-hydrogen rods properly.
Note: Low-hydrogen electrodes such as E7018 must be stored and handled correctly. Moisture pickup degrades weld quality and can cause porosity, so keep them in a holding oven or sealed container and use fresh rods when quality matters.
When the arc wanders or snaps toward one side, you’re likely fighting arc blow – a magnetic deflection problem associated with DC welding. Common fixes: switch to AC, move the work lead (ground) clamp to a different position, shorten the arc, or reduce amperage. Changing your work lead connection point often settles it instantly.
Changing two things at once makes it impossible to know which fix worked. Keep a notebook of amperage, electrode, thickness, and polarity – this turns guesswork into a personal chart. For thicker material where heat management and interpass control matter more, industry guidance such as the AWS D1.1 structural welding code is worth consulting.
Finally, don’t overlook the rod itself. Miller’s guidance on common stick electrodes echoes what every seasoned welder knows: most “amperage problems” are really arc length, travel, or storage problems wearing an amperage costume.
Mild steel plate is the training ground, but real jobs throw you curves. The settings that worked on 1/4-inch flat stock will fail on 18-gauge sheet, 2-inch plate, or a stainless pipe joint. Here’s how to adapt.
Below about 1/8 inch, stick welding turns into a heat-management exercise. Drop to a 3/32 or 5/64-inch electrode, run the low end of its range (often 40–70 amps), and travel fast to keep the arc from lingering. Where your machine and electrode allow it, DCEN (electrode negative) puts more heat into the rod and less into the work, which reduces burn-through.
Two shop tricks help. First, clamp a copper backing bar behind the joint — copper pulls heat away and supports the molten puddle. Second, use short, quick stringers instead of a weaving motion; a weave dumps far more heat per inch. If you’re comparing current types, our guide to DCEN, DCEP, and AC explains why polarity changes the heat balance. For anything under 16 gauge, MIG or TIG usually beats stick because the arc simply carries too much heat for reliable results.
On heavy sections, amperage alone won’t fuse the root. You need beveling, multiple passes, and controlled heat between them. AWS D1.1 Table 5.8 sets minimum preheat and interpass temperatures based on base metal thickness and material group; thicker steel and higher-carbon grades demand more preheat to slow cooling and prevent cracking.
Interpass temperature matters as much as preheat. Let the joint cool too far and you risk cold laps; let it climb too high and you lose mechanical properties. Some alloys also require post-weld heat treatment. Increase amperage modestly for fill passes once the root is sound, and stagger your stops so heat doesn’t build up in one spot. Measure interpass temperature with a contact thermometer or temperature crayon rather than guessing. For heavy, high-deposition work, automated processes like robotic submerged arc welding take over where manual stick becomes impractical.
Quick Note: Always check the applicable code or a qualified WPS before welding thick or critical sections. Table 5.8 is a starting point, not a substitute for your procedure.
Stainless conducts heat poorly and expands more than carbon steel, so it warps and “sugars” easily. Use matching specialty electrodes (E308L, E316L) at roughly 10–15% lower amperage than the same diameter in mild steel, keep a tight arc, and minimize travel width. Lower heat also limits sensitization — chromium carbide precipitation that hurts corrosion resistance. Our welding practice guide covers drills that build this finesse.
Cast iron cracks when it cools fast. Use nickel-based electrodes (ENi-Cl or ENiFe-Cl), preheat the part to 400–600°F where practical, and run short stringer beads with a peening pass to relieve stress. Keep amps moderate and let the part cool slowly — never quench it. A common choice is a 3/32 or 1/8-inch nickel rod run at the low-middle of its range; the goal is fusion, not speed.
Pipe welding splits the amperage decision by pass. Root passes commonly use E6010 or E6011 for their deep, forceful penetration and ability to burn through fit-up gaps. Fill and cap passes switch to low-hydrogen E7018 for strength and a smoother bead. Wall thickness drives amperage: thicker walls tolerate and need more current, while thin-wall root passes run cool to avoid blow-through. A handy rule: the root sets penetration, the fill builds strength, and the cap controls appearance — tune amps for each, not once for the whole joint.
Galvanized, painted, or contaminated metal releases toxic fumes when the arc hits it. OSHA 1910.252 requires adequate ventilation to keep exposures below permissible limits. Grind coatings off first, weld outdoors or with local exhaust, and wear proper PPE. See our protective eyewear guide for the full setup.
By now the pattern should feel familiar: amperage and metal thickness are not two separate settings you guess at — they are one conversation between your machine, your rod, and the steel in front of you. Instead of memorizing numbers, give yourself a process you can run on every job, every time.
Quick Note: The charts and rules of thumb throughout this guide are starting points, not verdicts. Amperage is a range, not a single magic number — your machine’s calibration, your arc length, and your travel speed all shift where the “right” setting actually lives.
That last point is the real skill. Reading the puddle — watching how it wets out at the toes, whether it wets in or crowns up, how fast it freezes — tells you more than any dial. If the puddle fights you, climbs, or freezes the rod, drop about 5 amps. If it spreads flat and sinks, or the arc wanders, you are running hot. Your eyes and ears are the final gauge.
The welders who set amps instinctively got there the boring way: deliberate practice on scrap coupons. Grab offcuts, keep a log of rod, polarity, and amps, and weld the same joint repeatedly while changing one variable at a time. That is one of the fastest ways to build a feel for correct amperage and travel speed, and it costs almost nothing but time.
When you want to go deeper, the surrounding fundamentals reward study. Polarity logic carries straight across processes, so how DCEN, DCEP, and AC behave in TIG sharpens your stick decisions, and flux-core polarity shows the same principles at work in wire feeding. If your shop uses multiple processes, our guides on gasless flux-cored welding and automated submerged arc show where heat control gets handed to a controller.
Note: No setting matters if you skip the basics. Wear proper PPE — helmet, gloves, and approved eye protection — work with adequate ventilation per OSHA requirements, and inspect every weld after it cools. Slag pockets, undercut, and lack of fusion hide in plain sight; grinding a test bead open is the honest way to confirm penetration.
Start low, test on scrap, adjust in small steps, and trust the puddle. Do that consistently and the 20-amp gap between a frozen rod and a burn-through stops being a gamble — it becomes a decision you make on purpose.
For 1/8-inch steel, a 3/32-inch E6013 at roughly 40-90 A or a 1/8-inch electrode at roughly 75-130 A is a good starting point. Use E6013 for the cleanest, most controlled arc on thinner stock. Start low and bump up in small steps until the toe lines wet in cleanly.
Yes, generally. Thicker steel acts as a larger heat sink, so you need more current to reach fusion temperature and achieve penetration. The fix is often to move to a larger electrode that can carry more amps rather than simply cranking the dial on a small rod.
Too much amperage overheats the electrode, causes the flux to burn off unevenly, produces heavy spatter, undercut, and burn-through on thin material. It also increases the risk of a widened heat-affected zone. Dial back in 5-amp steps and test on scrap.
E7018 typically runs on DCEP with a 3/32-inch rod around 65-110 A, a 1/8-inch rod around 90-160 A, and a 5/32-inch rod around 130-220 A. E7018 is a low-hydrogen electrode used for structural work, so proper storage matters as much as the setting.
No. E6010 is a DCEP-only electrode and will not run on AC. If your machine is AC-only, use E6011, which is the AC-capable alternative with a similar deep-digging arc for root passes and dirty steel.
A sticking rod usually means the amperage is too low, the arc length is too short, or the electrode has absorbed moisture. Raise the amperage slightly, hold a short but consistent arc, and store electrodes properly, especially low-hydrogen types.
A common starting point is about 15 percent below your flat-position setting. Out-of-position work needs less heat so the puddle stays controlled and does not sag. Test the change on scrap before running a finished joint.
As a rule of thumb, match the electrode diameter to the metal thickness for thin material, then step up to bigger rods as thickness increases. Thin sheet gets 3/32-inch rods, 1/8 to 1/4 inch steel gets 1/8-inch rods, and 1/4 inch and up often uses 5/32-inch or larger electrodes.
DCEP concentrates heat in the base metal for deeper penetration, while DCEN melts off the electrode faster with shallower penetration. Because penetration and bead shape change with polarity, you should re-tune amperage whenever you switch polarity, even at the same thickness.