3/32 E7018 Amperage: Settings, Polarity & How to Run It
My first E7018 rod went about as badly as a weld can go without catching fire. I was…
READ ARTICLE →It is a feeling every welder knows. You strike the arc on a piece of mild steel, expecting a smooth bead, but all you get is a sputter, the rod sticks to the plate, or you burn straight through your sheet metal. For those running E6013, this frustration almost always comes back to one dial: amperage. While technique matters, no amount of steady hands can compensate for a setting that is too hot or too cold for the rod in use.
Part of the reason this setting is so unforgiving is that E6013 is one of the most versatile electrodes on the market. Classified under AWS A5.1/A5.1M as a high-titania (rutile) potassium covered electrode for shielded metal arc welding (SMAW), it carries the familiar code. The ’60’ means a minimum 60,000 psi (414 MPa) tensile strength, the ‘1’ means all-position, and the ‘3’ means a rutile potassium coating suitable for AC, DCEP, or DCEN. This flexibility is rare, as many electrodes are far more limited in polarity.
Quick Note: Unlike E6010, which is restricted to DCEP, E6013 can run on AC, DCEP, or DCEN with ease. Its potassium compounds allow it to run on AC at low amperages and low open-circuit voltages, making it especially friendly to small hobby inverters and old transformer buzz boxes.
This wide compatibility is a blessing, but it also creates a trap. With such a broad usable range, it is tempting to guess a number and start welding. The reality is that E6013 has an unusually wide amperage window, but it still has a distinct sweet spot for each rod diameter. Straying too far from that range will affect nearly every aspect of the arc and the final bead.
Amperage is not just about “how hot” the arc is, but about the balance of the weld itself. When set correctly, it keeps the arc stable and predictable. When it is off, the effects are immediate. A few key outcomes include:
These tradeoffs are why many welders cross-reference their settings with a known baseline. For example, if you have used the E7018 amperage guide, you will notice E6013 often tolerates a slightly different range, especially on AC. Understanding those differences saves rods, time, and frustration.
The goal of this article is to take the guesswork out of those numbers. Over the coming sections, we will cover charts by diameter, thickness and joint type, polarity effects, position-based tweaks, and troubleshooting. We will also compare E6013 to other electrodes to show when it shines. Most importantly, we will focus on finding its sweet spot, because for this electrode, amperage truly is the setting that makes or breaks the weld.
Amperage is the volume of electrical current flowing through the arc, and it is the throttle on your machine. Turn it up and you dump more heat into the joint every second. Turn it down and the puddle goes cold. That single number drives four things at once: penetration depth, rod melt-off rate, deposition rate, and how cleanly the bead wets into the base metal.
Current creates intense resistance heating at the arc, and that heat does the actual melting. Push more amps through the same rod and the arc bores deeper into the steel. Back the amps off and it rides high on the surface. Because E6013’s rutile coating burns into a soft, quiet arc, it delivers shallow-to-medium penetration — the lowest of the common mild steel stick electrodes — which is exactly why it is the go-to for thin sheet and cosmetic beads. It tolerates one of the widest amperage windows of any stick rod, but it still rewards precision inside that window. That is the whole reason a 3/32 in rod can run clean anywhere from roughly 70 to 120 amps.
Where does bead wetting come in? When the puddle is hot enough, surface tension drops and molten filler flows out to feather into the plate edges, giving those smooth, concave toes you see in textbook welds. Run cold and the filler humps up, leaving a crowned bead sitting on top with edges that never fuse. Run hot and the puddle turns watery, sagging and undercutting the sides.
Set the amps too low and the rod cannot sustain a stable molten pool. The electrode sticks, the arc stutters, and you get cold lap and lack of fusion, where filler sits on top of the steel instead of fusing into it. That kind of defect often shows up later as an overlap welding defect that needs grinding out and repairing.
Set the amps too high and the opposite happens: burn-through on thin material, undercut along the toes, heavy spatter, a harsh popping arc, and a rod that glows red-hot and starts shedding its coating. On sheet metal, the difference between a clean weld and a blown hole can be 10 or 15 amps.
Quick Note: If you can hear a steady bacon-frying crackle and the rod melts evenly, the amperage is close. Sticking means go up. Spatter and undercut mean go down.
Amperage never acts alone. Voltage controls arc length — the physical gap between rod tip and puddle — and travel speed controls how long the arc stays in one spot. Typical E6013 arc voltage windows run roughly 18.5 to 25 volts depending on diameter, per manufacturer data sheets. Weld too slowly and even moderate amps pile up excess heat; weld too fast and you starve the joint of fusion. The three settings must move together, and polarity shifts the whole equation because DCEP concentrates more heat in the workpiece while DCEN sends it into the rod. Shortening the arc raises current and heat at the same setting, which is why dragging the rod close mimics a bump in amperage.
Higher amps also melt the rod faster. Pinnacle Alloys data shows E6013 deposition climbing from about 1.35 lb/hr at 70 A (3/32 in) to 4.22 lb/hr at 190 A (3/16 in) on AC. That extra metal has to go somewhere, so travel speed must rise to match or the bead turns into a fat, lumpy pile. This burn-off behavior is why operators chasing production on thick plate compare stick to high-deposition processes like submerged arc. For out-of-position work, manufacturers recommend cutting amps about 15% below the flat setting so gravity does not beat the puddle. If you are used to wire-feed welding, remember stick gives you far less leeway to correct a bad heat setting on the fly.
Rod diameter is the biggest single lever you pull on E6013 amperage. A thicker rod carries more metal, needs more heat to melt it, and therefore burns hotter. That relationship is the whole chart in a sentence: smaller rod, lower amps, thinner material. Yet the ranges are narrow enough to be genuinely useful. Get within 10 A of the target and the rod usually behaves.
Here is a practical starting table for the seven most common E6013 sizes. Use the “start here” column the first time you strike an arc, then fine-tune it to your machine and material.
| Rod Diameter | Amperage Range | Good Starting Point | Typical Use |
|---|---|---|---|
| 1/16 in | 20–45 A | ~30 A | Sheet metal, thin gauge, tacking |
| 5/64 in | 25–60 A | ~40 A | Light sheet, delicate work |
| 3/32 in | 40–90 A | ~65 A | Sheet, vertical-up, general light work |
| 1/8 in | 80–130 A | ~105 A | The all-rounder for 1/8 to 1/4 in plate |
| 5/32 in | 105–190 A | ~145 A | Heavier flat and horizontal work |
| 3/16 in | 150–230 A | ~190 A | Thick plate, flat position |
| 1/4 in | 200–300 A | ~240 A | Heavy sections, high-deposition flat work |
A rod’s cross-section determines how much current it can carry. A thin 1/16 in rod has little metal to melt, so it burns back fast if you push too many amps — that is how you blow holes in sheet. A fat 1/4 in rod is the opposite: run it cold and the arc stutters, the slag freezes ahead of the puddle, and penetration stalls. Amps must match the mass of metal you are melting, and the rod’s diameter is a direct proxy for that mass. The AWS A5.1 specification lists standard E6013 sizes from 1/16 in all the way to 5/16 in, which means a 1/4 in or larger rod needs a machine that can genuinely deliver 200+ A.
The quick rule of thumb is to match rod diameter to material thickness. A 3/32 in rod suits roughly 1/16 to 1/8 in steel, a 1/8 in rod covers 1/8 to 1/4 in, and a 5/32 in rod takes over above 1/4 in.
Most of your E6013 welding will fall into three sizes:
Quick Note: 3/32 in is where most beginners should start. At 40–90 A it is forgiving on thin steel, runs clean vertical-up, and rarely burns through. Begin near 65 A, watch the puddle, and nudge from there. If the rod sticks, add 5 A; if it burns through, drop 5 A.
Quick Note: 1/8 in E6013 is the benchmark. Manufacturers cluster it around 80–130 A, so a 105 A start lands you safely mid-window on 3/16 to 1/4 in plate. It also handles gaps and dirty steel better than most rods, which is why it is the default in repair shops.
No two datasheets are identical. HYW lists 1/8 in E6013 at 80–140 A, while Washington Alloy caps the same size at 80–130 A. Pinnacle and Toko sit in between. The chemistry and coating formulation differ slightly from maker to maker, so the usable window shifts with each product. Treat any chart, including this one, as a starting reference rather than gospel. The data sheet on your rod package is the final authority for that exact electrode. Even within a single brand, a change in coating batch or how the rods were stored can nudge the sweet spot, so always verify on scrap before you commit to a joint.
Once you have a starting amperage, resist big jumps. Adjust in 5–10 A increments and re-test on scrap of the same thickness. A 10 A change is often the difference between a smooth, crackling arc and one that sticks or sputters. Match the chart to your machine’s real output, too: if a 1/4 in rod calls for 240 A but your welder tops out at 200 A, either step down a rod size or upgrade to a machine and leads rated for the job.
While rod diameter is a solid starting point, it is only half of the equation. To dial in E6013 amperage, you need to account for the thickness of your base metal, the joint you are welding, and the quality of your fit-up. These factors will raise or lower your ideal range far more than most beginners expect.
The thinner the metal, the less heat it can take before it warps, distorts, or burns through. For thin sheet metal in the 16-20 gauge range, a 3/32 or 1/16 in E6013 rod at low amperage is your best bet. For 16-gauge sheet, a 1/16 in rod at roughly 25-35 A on DCEN prevents burn-through. This low range works because E6013’s shallow penetration means it sits on top of the metal rather than burning through, making it ideal for sheet, auto body panels, and thin-wall tubing.
As thickness increases, so does the need for heat. For 1/8 to 3/16 in plate, an 1/8 in E6013 rod typically runs 100-115 A as a sweet spot. For quarter-inch and thicker plate, 5/32 or 3/16 in rods are far more practical, and they will require a higher amperage to achieve proper fusion. Keep in mind that E6013 is not a substitute for E7018 on structural work because its deposit is not low-hydrogen and its penetration is limited. For heavy structural joints, a low-hydrogen option like 3/16 E7018 is a more appropriate choice.
Quick Note: Thin metal acts as a heat sink in reverse. Instead of pulling heat away, it absorbs very little, so a small bump in amps can go from a clean bead to a hole in seconds.
Not every joint requires the same amount of filler or penetration. A tight butt joint with no gap will need slightly more amps than you may think to fuse both edges, but an open root will need lower amps to avoid blowing through. Beveling thick plate increases the surface area for fusion, but it also allows you to use a smaller rod and a controlled amperage rather than cranking it up.
Fillet welds behave differently from groove welds. A T-fillet or a lap weld joint spreads heat across two pieces of metal, which can act as a small heat sink. For these joints, you may be able to run near the middle of your range, but fit-up will be the deciding factor. If the pieces are lapped tightly with no gap, heat builds up faster, so a slight reduction in amps can prevent excess buildup. On the other hand, a loose fit-up will rob you of fusion and tempt you to overcompensate.
One of the most common errors to watch for with these joints is excess metal spilling over the edge. This is known as overlap, and it is one of the hallmarks of poor technique. To learn how to spot and prevent it, check out our guide on the overlap welding defect.
Heat sinking is one of the most practical concepts for E6013. Thin, small parts dissipate heat slowly, so you need lower amps and faster travel to avoid distortion and burn-through. Thick, large plates pull heat away rapidly, so you will need more amps to achieve fusion at a reasonable travel speed. Clamping, jigs, or welding near a previous pass can all change how much heat your workpiece holds.
For any setup, use these rules of thumb as a baseline: 16-20 gauge with 1/16 or 3/32 in rod at the lowest safe amps, 1/8 to 3/16 in plate with 1/8 in rod around 100-115 A, and quarter-inch or thicker with 5/32 to 3/16 in rod at the upper end of its range. From there, let the arc be your guide. A steady, crackling arc with minimal sticking is far more telling than any number alone.
Note: When in doubt, drop your amperage by five and increase your travel speed slightly. For E6013 on thin metal, this adjustment will save you from more burn-through than any other tweak.
Here’s the good news about E6013: it will run on just about any current you can throw at it. According to AWS A5.1, this is one of the most polarity-flexible mild steel electrodes made. You can run it on AC, DCEP (electrode positive), and DCEN (electrode negative). But “it runs” and “it runs the way you want it to” are two very different things.
Polarity changes where the heat goes. That single idea explains everything in this section.
On DCEP, the electrode is positive. Electrons stream from the work to the rod, and since most of the arc’s heat is generated where the electrons land, that heat piles up on the electrode tip. You get a hotter rod, faster melt-off, and a deeper, more biting weld pool.
DCEP generally produces deeper penetration than DCEN, which makes it the default choice for thicker sections, root passes, and joints where you need the arc to dig in and fuse the edges. The tradeoff is heat. Because the rod runs hotter at the same amperage, you’ll often back the dial down a few amps on DCEP, or run faster before the workpiece gets away from you.
Quick Note: Polarity doesn’t shrink the amperage window — 1/8 in E6013 still runs roughly 90 to 130 amps on any current. What changes is how hard that amperage bites. Set amps to match the behavior, not the number.
Flip the leads and you flip the story. On DCEN the work is negative, most of the heat concentrates in the base metal, and the electrode stays cooler. Melt-off slows down, the arc feels softer, and penetration gets shallow — about as shallow as E6013 ever gets.
That’s a feature, not a flaw. On very thin stock, DCEN is how you avoid blowing a hole through the panel. It gives you more control over a wandering pool and lets you weld sheet metal with an electrode that would otherwise be too aggressive. This electrode-negative reasoning shows up across other processes too; if you want to know how polarity shifts heat in tungsten arcs, our guide on AC or DC for TIG welding steel walks through the same physics from the other direction.
AC sits between the two extremes. The current alternates, so the arc spends half its time with the electrode positive and half with it negative. The result is penetration that lands somewhere in the middle of DCEP and DCEN, with a balanced feel that’s forgiving on fit-up.
AC has two practical perks. First, it’s the great equalizer for transformer and AC-only machines — the old buzz boxes in countless garages run 6013 brilliantly. Second, AC’s inherent cleaning action helps the arc cope with rusty, painted, or otherwise contaminated surfaces. According to ESAB University, that self-cleaning behavior is a big part of why AC is so forgiving. It also helps rein in arc blow, the magnetic wandering that plagues DC work near corners and heavy tacks.
If you’re weighing which current to run on carbon steel, the logic parallels what happens when you pick polarity for a wire process — our breakdown of polarity for flux core welding covers DCEN versus DCEP in the same heat-balancing terms.
| Current | Penetration | Best For | Amps at a Given Rod |
|---|---|---|---|
| DCEP | Deepest | Thick sections, root passes, digging in | Same range; rod runs hotter, so ease down if needed |
| AC | Medium | AC-only machines, dirty steel, arc blow | Same range; balanced behavior |
| DCEN | Shallowest | Thin sheet, control, less burn-through | Same range; rod runs cooler, may push slightly higher |
The takeaway is simple. Your amperage chart doesn’t change with polarity — your expectation does. Deep, biting arc? DCEP. Gentle, controlled arc on thin metal? DCEN. A forgiving middle path on an old AC machine? AC. Read the puddle, trust the penetration you’re seeing, and nudge the amps to fit the current you chose.
Next, we’ll take that same logic and tilt the workpiece, because flat, vertical, and overhead all shift where the amps want to land.
Position matters more than most welders expect because gravity never takes a break. In flat work, gravity is on your side. The molten puddle sits in the joint where you put it, and you can pour heat into the arc without worrying about metal running away. Tip the workbench vertical, flip the part overhead, and that same puddle turns into a dripping hazard. The amps that ran beautifully on the bench will now sag, undercut, and leave you with a cold, lumpy bead that looks nothing like your flat passes.
The fix is simple in principle: back off your amperage out of position. Manufacturers such as Pinnacle Alloys recommend decreasing amperage by about 15% for out-of-position welding. Think of it as buying yourself reaction time. Lower heat means a slower-freezing puddle, and a slower puddle is one you can actually steer. A hotter puddle freezes fast but runs fast, and you get less time to read it before the metal drops out of the joint.
E6013 uses a rutile potassium coating, and that coating is the whole trick. It produces a fast-freezing slag that sets up almost immediately behind the arc, building a shelf that helps support the puddle in vertical and overhead work. This is why E6013 is rated for flat, horizontal, vertical, and overhead positions in AWS A5.1, the same spec that governs 6013 classification. Switch to a low-hydrogen or cellulose rod, and that support disappears, which is why those electrodes need their own out-of-position rules.
Quick Note: “All-position rated” does not mean “equally good in every position.” E6013 genuinely shines flat and horizontal. Vertical and overhead are possible, but they demand lower amps and tighter control.
Here is a concrete example using 1/8 inch rod. Flat, that electrode happily runs 95–115 A. Turned vertical-up, most welders drop to roughly 70–86 A to keep the puddle from sagging through the joint. That is the 15% haircut in action, and it is a good mental starting point for every diameter. Remember that smaller rods shift the entire range downward, so 3/32 inch 6013 might top out near 90 A flat and sit closer to 65 A vertical-up.
| Position | 1/8 in rod (approx.) | Puddle behavior |
|---|---|---|
| Flat | 95–115 A | Wide, fluid, high deposition |
| Horizontal | 90–105 A | Controllable, watch the top toe |
| Vertical-up | 70–86 A | Fast-freezing, needs low heat |
| Overhead | 70–90 A | Drips easily, keep it moving |
Amperage is only half the story. Your angle and travel style shift too, and ignoring that half of the equation means even perfect amps will fight you:
In every out-of-position pass, keep your electrode manipulation small. Big weaves build a puddle you cannot freeze in time, and that is when E6013 bites back. If you are moving between processes on a bigger fabrication, a quick refresher on DCEN vs DCEP polarity for flux core helps you translate these position habits to other rods.
Start about 15% below your flat setting, watch the puddle, and dial in from there. Position sets the ceiling on your amps, and E6013 rewards you for respecting it.
Your ears and eyes tell you more about E6013 amperage than any chart ever will. Once you recognize what “right” sounds and looks like, dialing in the machine becomes second nature. Here’s how to read the signals and adjust with confidence.
A steady bacon-frying sound means your amperage is close. That even sizzle is the arc transferring metal smoothly, drop after drop. Run a bead and close your eyes for a second — your ears will learn the correct pitch faster than you’d think.
Quick Note: E6013 should be dragged with a short arc. It does not need and does not want a whipping motion — that style belongs to electrodes like E6010. Keep a constant short arc and let the amps do the work.
Sound gets you close; the bead confirms it. Compare what you see to this quick diagnostic.
| Symptom | Likely Cause | Fix |
|---|---|---|
| Bead crowned and ropey | Too cold | Add 5–10 A |
| Bead flat, washed-out, with undercut | Too hot | Reduce 5–10 A |
| Excess spatter, rough irregular arc | Wrong polarity or amperage | Check polarity, then adjust |
| Poor wetting at the toes | Not enough current | Add ~10 A |
A healthy 6013 puddle is fluid and wets the edges in a smooth, slightly convex shape. If it sits up like a ball of solder, it’s starved for heat. When the puddle piles up and won’t wet into the toes, reach for the dial — add about 10 A — rather than slowing your travel speed. Slowing down just makes a cold, tall bead. Excess spatter plus a rough, irregular arc often points to the wrong polarity or amperage, per ESAB University. Polarity is a frequent culprit; our guide to DCEN vs DCEP polarity explains how swapping leads reshapes the arc.
Move in 5–10 A increments. Big jumps overshoot, and you’ll chase the setting all afternoon. Change one variable at a time and run a test bead on scrap before touching your actual workpiece. Keep a scrap plate at the same thickness as your job; that’s the only honest test.
Amperage never works alone. A long arc raises voltage, widens the puddle, and spatters more — so shorten it before you blame the amps. As a rule, keep the arc as short as the rod allows without sticking; longer arcs lose heat and control. Travel speed does the same balancing act: too fast gives a thin, cold, high-crowned bead; too slow overheats and burns through thin steel. Get the arc short and the speed steady first, then fine-tune current.
At the top of the amperage range, your machine works hardest. Push a 90 A-rated welder to its ceiling on a long bead and the thermal overload may trip mid-weld. A 60% duty cycle at 90 A means roughly six minutes welding followed by four minutes cooling; exceeding that shortens machine life and can sag your voltage. Check your manual, and don’t mistake a hot machine’s drop in output for a settings problem.
The visual instincts you build reading a 6013 puddle transfer straight to other processes. Learning to spot a crowned, cold bead versus a flat, washed-out one is the same skill you use judging fusion and profile on wire welds — see our guide to good and bad MIG welds for the visual checklist.
Fine-tuning isn’t guessing. Sound, bead shape, spatter, and wetting give you four honest signals. Read them, adjust in small steps, and E6013 becomes one of the most forgiving electrodes in your shop.
Most bad 6013 welds trace back to a handful of setup errors, and nearly all of them are fixable in under a minute. Here are the ones that show up again and again, with the symptom you’ll see and the fix that cures it.
Symptom: The rod sticks to the plate, the arc keeps extinguishing, and the puddle sits on top of the metal instead of biting in. The bead looks tall, ropey, and crowned, with cold lap at the edges and zero fusion underneath.
Fix: Sticking and frequent arc extinction are classic signs of amperage that is too low for the rod diameter. Bump the amps up in 5-amp steps until the arc starts smoothly and the puddle wets out at the toes. If you’re already near the top of the range for that rod, switch to a smaller diameter instead of forcing more current through it. Give each change a few inches of bead before judging it, since E6013 stabilizes as the rod warms.
Symptom: Burn-through on thin sheet, deep undercut along the edges, a crater that sags at the end of the bead, and spatter flying everywhere.
Fix: Burn-through, undercut, and excessive spatter indicate amperage that is too high or travel that is too slow. Drop the amps first, then tighten your travel speed and shorten the arc. On light gauge, stepping down one rod size is often cleaner than dialing down a fat rod to the ragged edge of its range. Watch the toes closely: if they’re washing away or the edges look eaten back, you’re still running hot.
Symptom: The amps look perfect on paper, but the arc runs harsh or weak no matter how you adjust, penetration is inconsistent, and the bead never quite behaves.
Fix: A machine set to the right number on the wrong polarity still produces a bad weld — polarity must match the electrode. E6013 runs well on both AC and DC, but each mode shifts how the arc feels, so remember to re-tune rather than reusing your DC numbers. If you’re unsure which lead goes where, brush up on how polarity in stick welding is wired before you blame the rod.
Symptom: Flat welds look great, but the moment you go vertical or overhead the puddle falls out, sags, or runs ahead of the arc.
Fix: Gravity is working against you, so reduce amperage roughly 10 to 15 percent for vertical-up and overhead work. A slightly colder, tighter arc keeps the puddle manageable without sacrificing fusion. You’ll usually also want a shorter arc and a faster, more deliberate travel to stay ahead of the heat.
Symptom: Spatter, arc wander, and a rough, undercut bead that won’t settle down despite reasonable settings.
Fix: Keep the arc length roughly equal to the rod’s core diameter. Too long a gap wastes heat, widens the arc, and encourages undercut. Also check your rods: damp electrodes or a damaged flux coating can mimic the symptoms of a wrong amperage setting, so store them dry and discard chipped ones. And make sure rod size actually suits the metal — a 1/8 in rod on 18-gauge sheet will burn through no matter how carefully you tune. A clean, dry rod and a snug stinger connection go a long way toward a stable arc.
Quick Note: Your machine’s readout can lie. Amperage displays drift with age and heat, so a $40 clamp meter around the stinger lead often reveals a real output that’s 15 to 20 percent off the dial. Verify before you chase ghosts.
For a useful calibration reference across electrode types, compare our 3/16 E7018 amperage guide, where the amp windows behave very differently. And whatever you’re tuning, protect your eyes while you dial the arc in — see our guide to protective eyewear for welding before the next bead.
E6013 is the friendly rod in the drawer, but it is not always the right one. Swap it for a cellulosic or low-hydrogen electrode and the amperage window shifts, the polarity rules tighten, and your whole setup needs a second look. Here is how the numbers actually compare.
The table below shows typical general-purpose ranges. Confirm the exact figures against your manufacturer’s data before you commit.
| Electrode | 3/32 in | 1/8 in | 5/32 in |
|---|---|---|---|
| E6013 (rutile) | 40–90 A | 80–140 A | 110–190 A |
| E6011 (cellulosic) | 40–85 A | 80–130 A | 130–180 A |
| E7014 (iron-powder rutile) | 80–125 A | 110–160 A | 140–210 A |
| E7018 (low-hydrogen) | 70–100 A | 90–150 A | 140–210 A |
For a 1/8 in rod, E6010 runs about 75–130 A on DC+ only, E6013 about 80–140 A on AC or DC either polarity, and E7018 about 90–150 A on AC or DC+, per manufacturer product data. E7018 needs a little more current than E6013 at the same size, and its polarity options are narrower. That is the low-hydrogen coating at work, and that narrow window is exactly why E7018 rewards a disciplined setup.
Polarity is the other variable that moves with the rod. E6013 is forgiving: AC, DCEP, and DCEN all run, which is why beginners love it. E7018 runs on AC or DCEP but not DCEN, and E6011 works on AC or DCEP. Get this wrong and you lose penetration and arc stability. The fundamentals are covered well in ESAB’s guide to polarity in stick welding.
Deposition rate climbs with amperage for all four rods, but E7014 and E7018 are engineered to use that extra current productively. Pushing E6013 too hard simply burns the coating, which is why rod selection and amperage selection go hand in hand.
Reach for E6011 when you need deep penetration into dirty, rusty, or poorly fit steel that you cannot fully clean. Choose E7018 when code or structural strength demands a low-hydrogen deposit; the extra amperage and oven storage are part of that trade-off. Step up to E7014 when you want more metal down per hour in flat or horizontal work. When in doubt, match the rod to the job: clean thin steel favors E6013, dirty or open-root work favors E6011, and structural welds favor E7018.
Deciding between stick and wire? It helps to know how the other processes compare. Our guide on whether flux core is the same as MIG explains the difference, and the MIG wire selection guide covers filler choices for wire-fed work.
Settings shift with size for every rod, so pull up a dedicated chart when you move to larger electrodes, like 3/16 E7018 amperage.
Quick Note: These ranges are starting points. Arc behavior also depends on polarity, position, and joint fit-up, so dial in from a test coupon and verify current against the relevant AWS A5.1/A5.1M spec.
Setting E6013 amps is not a one-time decision. It is a habit you build every time you lay a bead. The welders who get consistent, strong results are not the ones who memorized a single magic number. They are the ones who dial in, watch the arc, listen to the puddle, and adjust as conditions change. Small adjustments beat big swings every time.
Quick Note: A minimum 200 A machine output is needed to properly run a 1/4 in E6013 electrode. If your welder tops out lower, step down to a smaller rod rather than fighting the machine.
Amperage discipline means nothing if you get hurt. Stick welding throws sparks, spatter, intense UV, and metal fume. Always wear a proper helmet with correct shade, plus protective eyewear underneath for chipping slag. Leather gloves, jacket, and sleeves are standard, not optional, because hot spatter finds every gap. Never strike an arc with bare skin exposed or your sleeves rolled up.
Ventilation is just as important as eye protection. Welding fume exposure is a well-documented NIOSH and OSHA concern, so weld with airflow or local exhaust and wear respiratory protection when needed. Two standards anchor all of this: ANSI Z49.1 (Safety in Welding, Cutting, and Allied Processes) and OSHA 1910.252, which together define the requirements for PPE, ventilation, and fire prevention.
Never weld near flammable material without a fire watch and a charged extinguisher within reach. Confirm that extinguisher is rated for the fire class you might face before you strike the first arc. Get that environment right from day one using a solid welding facilities setup guide.
| Rod Diameter | Typical Amps | Polarity | Best Position | Steel Thickness |
|---|---|---|---|---|
| 1/16 in | 20–40 A | AC / DCEP | Flat, Horizontal | Up to 1/16 in |
| 3/32 in | 40–90 A | AC / DCEP | All positions | 1/16–1/8 in |
| 1/8 in | 75–125 A | AC / DCEP | Flat, Horizontal | 1/8–3/16 in |
| 5/32 in | 110–160 A | AC / DCEP | Flat, Horizontal | 3/16–1/4 in |
| 3/16 in | 140–190 A | AC / DCEP | Flat | 1/4 in and up |
| 1/4 in | 200–250 A | AC / DCEP | Flat | Heavy plate |
E6013 earns its reputation as the best beginner rod precisely because it is forgiving. It restarts easily, runs on AC or DC, and tolerates messy technique. But forgiving is not the same as automatic. Apply the same discipline to amperage that you would to any other rod, and good enough becomes genuinely strong. Treat the numbers above as a starting point, not a cage, and let the arc tell you the rest.
A 1/8 in (3.2 mm) E6013 rod typically runs 80-130 A. A good starting point for 1/8 to 3/16 in plate is about 100-105 A on AC or DCEP, dropping to roughly 85 A for vertical-up work. Always fine-tune in 5-10 A increments based on the arc sound and bead profile.
Yes. E6013 is rated for AC, DCEP, and DCEN, making it one of the most polarity-flexible mild steel electrodes. DCEP gives deeper penetration, DCEN gives the least penetration for thin stock, and AC is the most compatible with older transformer machines.
A 3/32 in E6013 rod runs roughly 40-90 A, with about 65-70 A a common starting point. It is the go-to size for sheet metal, vertical-up, and overhead work where a small, controllable puddle is needed.
Sticking is almost always a sign of amperage that is too low for the rod diameter, or a dirty or damp rod. Increase the amperage in small increments and use a short arc. If it still sticks, try a smaller rod or check that your machine is set to the correct polarity.
Yes. Manufacturers generally recommend reducing amperage by about 10-15% for out-of-position work. For example, an 1/8 in rod at 100 A flat may run closer to 85 A vertical-up so gravity does not pull the puddle out of the joint.
E6013 is generally not used for code-critical structural work. Its deposit is not low-hydrogen and its penetration is shallow. Structural applications typically call for E7018 or similar low-hydrogen electrodes, so check your WPS and applicable code before substituting.
A 1/4 in E6013 rod needs a minimum of roughly 200 A and can run up to about 300 A in the flat and horizontal positions. That means you need a welding machine capable of at least 200 A output to run this diameter properly.
Yes. Amperage directly controls heat input and therefore penetration depth. E6013 already has shallow-to-medium penetration, so running too cold produces cold lap and lack of fusion, while running too hot causes burn-through and undercut. Polarity also shifts penetration at the same amperage.