Hi Metarinka!
Very first of all, please forgive me the great delay in my response it is as I said once. Quite much to do at the moment and thus as being the inverse opposite, quite less time for this wonderful forum! By the way, it appears unbelievable but a few days or even a few weeks not attending the forum means one is missing hundreds of posts. Wow... this is truly tremendous!
Thank you Metarinka for your excellent reply and the detailed and valuable information contained in it! Please let me try to state two or three words on even your response since I mean you have described some very interesting items deserving to be discussed further.
As one of the first of those please let me come back on what you have attached as my quote and dealing with the assumption of that the travel speed under tri-mix should be presumed to be higher compared with Ar/CO2. You know this assumption was made by me under having considered the statements coming from Ed Craig who - I hope my memory serves me right - has mentioned that helium runs "hotter" that argon under similar conditions. Even this was what made me a bit concerned, so to speak. Since from my humble standpoint it is dangerous to compare both gases - even used as arc welding shielding gases - 1:1 due to their quite different physical properties they are showing within the arc plasma. This means when comparing both shielding gases under similar parameter set ups one will obtain results as I have tried to describe them by having stated the examples with the approximate similar wire feed speed of 9 m/min. Even this however, is nonetheless one of the benefits of the tri-mix, or high helium containing shielding gases in general. Due to the greater performance obtainable by using these shielding gases one may obtain particular benefits as even higher welding speed, improved droplet detachment characteristics or wetting behavior. So what happened when you have tested the shielding gases was - at least in my interpretation - even the proof for this assumption. Due to you have firstly chosen similar conditions - based on the parameter set up for tri-mix (quote: "Several welds were performed under Tri-mix at settings comfortable to the welder") - for both shielding gases, you could not use even these parameters to be used for the Ar/CO2 mix. And honestly I would have been surprised if you would have been able to use them in a 1:1 ratio. And just a short input once again. Statements as e.g. "Helium runs hotter than argon under similar conditions" may awake - at least from my point of view - even the assumption that the welder has just to switch the shielding gases from argon to helium, remain at the same parameters and may run the bead faster since even helium provides more "heat" over the unit time. But this is definitely not the case, as you have recognized and given your welder the chance to freely and experienced adjust the parameters and other variables /quote/
"Penetration, travel speed, shielding gas flow rate and machine parameters were all open variables the welder was free to manipulate in order to achieve a similar quality bead..."
/unquote/.
And even these set-ups were the result of his adjustments:
Tri-mix:
21V
220 WFS
98-2:
27V
375 WFS
And this is the evidence for that no similar conditions can be chosen for both shielding gases, which is however the risk of being assumed when listening to statements as "helium runs hotter than...". Of course runs helium "hotter" than argon but nonetheless it is necessary to change some very important conditions for obtaining approximately similar results. To use different words. Helium provides a higher arc performance with similar conditions where I have to clarify that - at least for me - the only real "constant" in GMAW is the wire feed speed. Even this is - so my assumption - what your welder has experienced when switching to Ar/CO2 and using the similar parameters as been used for tri-mix. And of course it won't work to reduce the welding speed to obtain a similar heat input into the base metal, since there must be an imbalance to be observed between the energy input in general and due to the stronger bead reinforcement you would probably have obtained by decreasing the travel speed you have not obtained an increase in the melting efficiency itself. In other words. One can of course reduce the travel speed to try to obtain a similar "heat input" when using Ar/CO2 but this is just a theoretical approach and the real results will most likely deviate from the theoretical assumptions by showing unacceptable bead appearances. As one of the most influencing factors I believe is the quite different heat conductivity of both shielding gases to be seen. Argon has a lower heat conductivity across the plasma's radial cross section shows thus a "hot" core and a temperature drop across the radius resulting in the well-known finger type penetration profile. Helium whereas shows a higher heat conductivity under showing simultaneously a diffuse arc plasma but having an even more homogenous temperature distribution. However, it requires a higher arc voltage leading under similar wire feed speeds to a higher arc performance hence higher melting efficiency and hence higher welding speed under the assumption to obtain a similar depth of penetration.
Thus again to obtain similar welding results with particular respect to productivity your welder had of course to change the parameter set up which results in those values as been stated by you.
This again makes it entirely understandable what you have stated subsequent to that, namely /quote/:
"Travel speed under 98-2 would actually be higher (although obviously not by a theoretical factor of 2) when trying to maintain an equal bead appearance under a "colder" less penetrative arc (due to shielding gases)." /unquote/.
It appears understandable that a wire feed speed of 375 inches/minute (9.525 m/min) when using Ar/2CO2 compared with a wire feed speed of 220 inches/minute (5.588 m/min) requires a higher welding speed since you have admittedly adjusted the arc performance by increasing the voltage times the current (wire feed speed) but of course you have changed the constant wire feed speed on the other hand and to deposit thus a higher burn off rate - to obtain similar bead shapes - it requires a higher travel speed. This makes sense and does of course lead my assumption that the welding speed under tri-mix was assumed to be higher to be incorrect. But - as I tried to describe - I have assumed the welding speed to be higher under using tri-mix based on the general statement that helium runs "hotter " than argon under similar conditions which I interpreted have included similar welding parameters.
Coming now to your "BIG DETOUR" :-)
Well, what should I say..?
Most interesting what your observations and the explanations for these are. First of all I would like to treat the observation for increased voltage - set by the welder - does require an appropriate increase in wire feed speed to avoid burn back and some other problems. When I am interpreting these observations correctly then you have proved hereby the volt ampere relationship between both crucial values in GMAW. When using a conventional power supply - I am sorry for not knowing the correct English term - what means that I can choose both voltage and wire feed speed independently (i.e. no modern power source providing "synergic" characteristics) one from the other then I mean one could obtain even what you have found by having set the voltage as a main value and adjusting the wire feed speed and proportional to this the current for finding the correct operating point as being the optimal matching point between both values. However, besides this operating point there is a more or less wide range possible depending to the characteristics of the power supply itself and limiting the field where even the parameters can be varied in between. In Germany we call this "Arbeitsbereich" or translated "working range".
In respect to your statement /quote/:
" In my experience the prime welding variable for GMAW is voltage, on constant voltage machines V is related to heat input..." /unquote/
please let me say the following.
I must repeat myself when saying that "heat input" is my personal hobby. Even this makes it so hard for me to say what "heat input" in the most objective sense of the word really is. This, since it is most intricate to define it exactly in general due to the extraordinary amount of variables relating to this issue. What does this mean now..? Well, let me assume that the voltage is the main variable for affecting the heat input and I assume further that the voltage is approximately proportional to the arc length. Then I assume to set a particular range of parameters i.e. voltage and wire feed speed or current, respectively. The result of the electrical efficiency of the arc is thus voltage times current. Now I assume that I have to calculate the "heat input". This is being accomplished by setting the electrical arc efficiency over the travel speed. This is a theoretical approach as well-known. However, even by the moment the arc is ignited the conditions related to the welding process may vary dependent to the particular instantaneous conditions as to be found as a reaction between the solid (base metal) and its specific properties and the arc. The performance from the arc is relating again by having a specific arc length (set by the voltage) and current (set by the wire feed speed). When now obtaining a particular product being set by voltage times current I must consider as well the appropriate length of the wire extension which does stand for an important amount of resistance to be integrated into the product which has been calculated by voltage and current. When now increasing the voltage by holding the wire feed speed or current respectively, constant, one increases the arc length and hereby decreases the wire extension length. This means that one decreases the resistance cohering to even the wire extension but increases the arc resistance which might compensate again the resistance losses of the wire extension. In other words, one might assume that the product remains the same as the wire feed speed remains the same. However the heat input might drop due to greater energy losses by radiation and the penetration profile might change as the cathode spot changes with respect to its unit area. This again means I am transferring an approximate similar product of arc energy (reduced by the increased radiation losses) over a greater area which yields a wider bead having a shallower depth of penetration. Hmmm...
Coming instead to an approach to welding speed and arc or welding performance, respectively. This is being expressed by the term "melting rate" (MR) and can be stated as:
MR = alpha * I + beta * l * I² / a
I is the current, l is the electrical wire extension and a is the cross sectional area of the wire. Alpha and beta are constants. Whereas the first term represents the arc heating effect and the second term represents the resistive heating of the electrode. Wire feed speed - which depends to the current chosen and this again is chosen in relation to the wall thickness of the parts to be welded - is - as I said once - for me the only constant in GMAW since the wire being fed has to be molten and to be deposited onto the workpiece over a particular unit of time. In order to obtain proper bead shapes and penetration profiles one has - proportionally to the wire feed speed which determines the melting rate - to choose an appropriate welding speed. This however is determined again by a maximum melting efficiency what means finally that I cannot increase the welding speed infinitely by increasing the melting rate - or the welding performance - infinitely. In other words, and this is what makes the subject so complex, each base - filler material combination suited under a particular shielding gas composition, under particular peripheral conditions will obtain particular values for welding speed, bead appearance, "heat input", etc. etc. An experienced welder - as you have mentioned - recognizes these conditions instinctively and adjusts the exterior and interior parameters to even obtain a proper result under varying conditions. However, so far that I remind correctly, the relation between welding speed and melting efficiency has been investigated by ROSENTHAL very first time. He has stated that there is s strong coherence between the welding speed and the melting efficiency which is based on the thermomechanical properties of the base material, in particular its heat conductivity. This means that the less time the material has to conduct a particular amount of thermal energy into the adjacent areas the higher the melting efficiency is. In other words, when considering a constant arc performance and changing the parameter travel speed one can presume a higher melting efficiency the higher the travel speed is. Even due to the increasing imbalance between the thermal energy transferred from the arc to melt the base material and the time the thermal energy or the heat source (arc) respectively, can interact with the solid matter.
To come to an end slowly and dealing with two little points thus.
Firstly the "colder" shielding gas.
I have tried to understand what the meaning of "colder " shielding gas might be. Does this mean that pure CO2 is the colder shielding gas when being compared with Ar/15CO2? Normally CO2 provides even great benefits for increasing the depth of penetration due to dissociation and recombination processes delivering additional thermal energy to improve fusion depth and "heat input". Even though I do not really know if this is the right comparison but CO2 reminds me personally always on helium since both shielding gases require higher voltages for GMAW purposes. Both again yields higher arc powers and thus higher heat inputs compared with "colder" shielding gases like argon. Although, and this has been excellently explained by you, CO2 has the restriction of not being able to be used in a spray arc mode. Nonetheless, in Germany we have standardized the so called "Langlichtbogen" (translated best as "Long Arc") which does work as particular arc mode under pure CO2 at ranges the regular Spry Arc does work under high Argon containing shielding gases. It has a high performance obtains deep penetration but is not short circuit free and yields spatter. One particular characteristic is that it burns underneath the base materials surface quasi as a "buried" arc.
Secondly let me say a word to the shielding gas flow rates, you have kindly stated. As I have assumed that the flow rate for the use of tri-mix should have been higher, the opposite was the case /quote/:
"However under the tests the welder actually increased flow rate under 98-2 as opposed to tri-mix. This was his reaction in trying to counter the increased oxidation. I believe flow rate was around 22 CFH for tri-mix and 28-30CFH for 98-2..." /unquote/.
I have conversed (into liters per minute) the flow rates - under the assumption that CFH = Cubic Feet per Hour - as been stated above and have received:
· 22 CFH ~ 622.97 l/h ~ 10.38 l/min.
· 28 CFH ~ 792.87 l/h ~ 13.21 l/min.
· 30 CFH ~ 849.50 l/h ~ 14.15 l/min.
Hmmm... to be honest with you Metarinka - by the way, may I perhaps call you Joel? - and please this is just a guess. I mean that in particular the values for the tri-mix might be a little too low under the consideration of a significantly reduced shielding gas density. The values for the Ar/2CO2 whereas are - at least from my humble point of view not that high actually when using the rule of thumb: wire diameter x 10 ~ flow rate - but of course not knowing what the diameter of your filler was.
So... and now coming really to an end, it's ~ 1.45 a.m. here. It was great to read your outstanding interesting explanations and it's truly a joy to discuss this with you.
And I thank the good Lord as I thank my beloved wife for having granted me the time finally once again for being allowed to visit this great forum. However, the weekend comes and I am at home this weekend... Perhaps I'll find some additional time to read some of the hundreds of posts been sent in the meantime since I've been here last time.
Last but not least, Metarinka, you have stated /quote/:
"In fact with a large enough sample size (the number of welders at my facility) I was able to establish a formula using statistical methods to calculate travel speed for a voltage with about 90% confidence, of course due to the parameter range there is a always going to be variation in weld parameters while still maintaining acceptable bead appearance. If requested I can dig up and attach this information." /unquote/.
This sounds extremely interesting! Would you be so kind and provide this information? That were truly great!
Once again thank you for your very knowledgeable and most interesting reply and my very best regards,
Stephan