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It is relevant to calculate the heat induced by the pump, or more specifically, the heat induced by the flow restrictions. As Since87 demonstrated, it can be easily calculated. |
Flow restrictions shouldn't add to much if any. Unless it's a very strong head pump or the restrictions are so great it causes pump cavatation.
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I do agree that your not measuring cooling power, rather the power used from the pump's output. |
Submerged Liquid Jet Impingement Heat Transfer(SLJIH)
The only submerged jet data with which I have played are presented http://widget.ecn.purdue.edu/~eclweb/jet_benchmark/ in the "Heat Transfer Results as Excel spreadsheet". I do not offer a graph because of "Any unauthorised use, copying or mirroring strictly prohibited ". However the graphs show the Heat Tranfer profile changes with conditions. However I do ,naively, consider the "plateau profile" of the "3.1mm ID" results maybe the ones applicable to to flat bottomed wbs.Additonally in "fantasy calculations" I equate the "h" of the plateau to that calculated by Flomerics at r= ~2.5D. Yes, it is "stretching it a bit" but ...................... |
Murray13 is right here.
This is where you want to look at your pump's PQ curve. If you were running under the peak efficiency, then a higher restriction would yield better results, because you would then have more total power applied by the pump. I found out something interesting the other day, while looking up orifice plates for LiquidRules: there are two kinds of restrictions out there; those that provide a recoverable pressurre drop (venturi) and those that don't (orifice plate). Jet inpingement produces a non-recoverable pressure drop. What that means is that although the fluid is flowing at a higher speed, it is permitted to enter an open area, in which it will turbulate: this speed cannot be recovered, it is simply a result of the opening. In a venturi, the speed is (essentially) recoverable. (Venturi is like a couple of funnels connected together at the small end). |
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Well, at least I got a good chuckle on a Saturday morning. Thanks. ;) |
I'm glad I could liven up your morning:D
I just mentionned it, because I hadn't seen it anywhere, and because I never looked at it that way before. It was specifically about recoverable vs non-recoverable pressure drops. The friction losses are an add-on (where it applies). It might not be relevant to anything, but it's there... It also relates to Radius, as I'm looking at trying to implement a jet (or jets), but my solutions always seem to end up into (mostly) recoverable PDs.:shrug: |
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I like to try a Iwaki (that the name?) with a nice head that uses about the same amount watts. When I tried the faucet trick that had about 50 psi and the same constant water temp as ambient air , the gains were great with a 1C difference between idle and load. Total 5C delta. Finding a pump like that without putting it's heat into the water to negate the gains is probably impossible. |
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I have no interest to use multiple jets. Over a wider area of heat it's great. To cool an area the size of a cpu die all is needed is one single impingement. Once one tries to use multiple jets so close together, it effects the wall flow and possibly the stagnation area. |
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Some rough sums: http://www.jr001b4751.pwp.blueyonder.co.uk/NozVel.jpg Based on Billa Data extracted from GIF* by Inspection and using : http://www.jr001b4751.pwp.blueyonder.co.uk/NozPQ.jpg * http://www.thermal-management-testin...vs.%20flow.gif |
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I've got a Little Giant 2-MDQ-SC, that has a max head of 14.6 feet. The problem I'm encountering is a dead flow spot in the block. I'm aiming for a jet, but of course because of the unusual inlet geometry, I have to tune it all just right, to maximize what my pump can do. I ran some tests with my pump, where I cap the outlet with caps with different size openings. I was originally shooting for 3/16. Right now, I'm looking at 1/4. I also tried a 3/8 test. None of my tests were conclusive. Part of the reason is the calculation (missing measurement?) of the pressure drop. I also suspect that the pump is behaving erraticly, because it has a design limitation (i.e. it doesn't do 0 head), or maybe I'm just completely wrong and nothing has anything to do with anything...:shrug: See LiquidRulez thread for a bit more info. |
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a (repeat) gift for the 3432 count poster this is how pump 'data' is commonly presented (w/o a curve) http://thermal-management-testing.co...60~%20data.jpg but if you think BACK to the pump characteristics link in pHaestus' article, you might recall a discussion of pump (impeller) efficiency do you know what that means ? here is more complete data for the same Hydor pumps (but 50~) http://thermal-management-testing.com/hydor.jpg do observe how the min-max ratio changes as the pump size increases getting a clue yet ? Thank you Bruce at Cooltechnica for the pumps |
"Other ways of shooting a liquid"
BB2k posted the above line and I would like to expand on it. In some experimental data I ran across there was indeed a difference in the results of jet impingement on a flat plate by changing the shape of the nozzles (circular being among the worst). Another variable to the equation. Anyone feel like googling? |
google ? google ?
who dat ? whey dey at man ? what I wanna know is . . . . |
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EDIT: The shape also effects the spreading rate and turbulance levels. |
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Here's a link courtesy of myv65 that was imformitive for me about pumps.
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Have found trying to estimate dP in different ID nozzles beyond me. Will leave the "evasion" posted - graphs quite pretty(and maybe informative Quote:
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I've had that dP kindly calculated for me (see details in Radius thread). I can share this formulae with you (or try to post it here, PM me).
Calculations were based on fluid properties, flow rate, and nozzle size. Results include dP (and speed?). I was also kindly reminded to look into hypersonic (or was it supersonic) flow speeds... (I was assuming 4 gpm:rolleyes: ). |
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I simply used a bucket of water at the inlet. Granted that there was a 1 foot rise, but I honestly expected the water to shoot up 15 feet, not 10. I have to revisit that test sometime, and see how I can get it right :rolleyes:. I know that my previous calculations were wrong. |
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Here's some links. An impingement database but you have to pay. Why? So I can't link to any information. http://www.eevl.ac.uk/jet/index.htm Various links I collected. http://www.electronics-cooling.com/h...01_may_a2.html http://home.icpf.cas.cz/vejrazka/web...ew_booklet.pdf http://web.cvut.cz/cp1250/fme/k212/p...ta/h06%5Ea.htm http://www.stanford.edu/~xzm/Research/Reno2003.pdf http://widget.ecn.purdue.edu/~eclweb/jet_benchmark/ http://fcl6.kaist.ac.kr/people/phd/pts/article.pdf http://216.239.57.100/search?q=cache...n&ie=UTF-8</a> Calc to calculate heat transfer of impingement. No idea how accurate it is. http://www.coolingzone.com/Content/D...as/fcalc10.htm Then there is the libraries but you have to pay for each copy of an article. Their more informative than these links. What ever happened to free imformation via the internet for the people? |
Ben.
Thanks for the offer.For the moment, further dP sums are not on my agenda so will give a miss. SysCrusher. Thanks. 50% are new to me. As you are aware, I have used and abused the the Flomerics calculator for both Cathar's WW* and the Switech462**. I do get reasonable( my opinion) , if accidental, agreement with Billa's test data. * http://forum.oc-forums.com/vb/showth...hreadid=161563 ** http://forum.oc-forums.com/vb/showth...hreadid=161124 |
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You can NOT decrease the diameter of the opening with the same pressure. |
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http://micromachine.stanford.edu/~lian/jetcooler.html |
Here is a cut and paste from a publication. The author is in the paste so it should be alright to post it here.
Quote "Article number: 1321 Title: Effect of nozzle geometry on impingement heat transfer distribution from jet arrays Author: Owens,R.D. and Liburdy,J.A. Year: USA, 6-8 August, Vol. 1, ASME HTD 303, 3-10 Abstract: Heat transfer distributions were determined for flat surfaces using three different 3 x 3 jet-impingement arrays. Each array used a different jet orifice cross sectional geometry, either circles, triangles, or ellipses. For each geometry, the jet-to-jet spacing divided by the hydraulic diameter, was three. Five flow rates were tested with Reynolds numbers ranging from 268 to 1557. For each flow rate, the four jet array height-to-jet spacings (H/D) of 2, 3, 4, and 5 were tested. All of the parameters presented, such as the Reynolds and Nusselt numbers, were based on the orifice hydraulic diameter. In order to determine the heat transfer distributions for each condition tested, thermochromic liquid crystals were used as part of a transient heating test method. In the majority of the tests, the ellipse array performed the best, with the triangular orifice close behind. Also, of the three orifice geometries, the ellipse had the lowest pressure drop. The heat transfer improvement was especially predominant at low Reynolds number. Publication: Proc. 30th 1995 National Heat Transfer Conf., Portland," End quote Click to jet impingement database search engine I'll dig some more. I recall reading a strange phenomena with the ellipse. It (the jet profile) will invert itself on the impingement surface at the right conditions for a benefit in heat transfer. |
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I found my other source of "confusion". When designing/calculating a nozzle within a pipe, the formulaes used assume that the distance passed the nozzle is at a minimum of 10d. So I now conclude (incorrectly?) that the pressure drop in a jet inpingement configuration is composed of 2 things: a)pressure drop across the nozzle b) pressure drop caused by the jet striking the baseplate. Now is there actually a pressure drop from [b], or is this configuration merely affecting the nozzle's performance, throwing off any calculations? If there is a pressure drop, is it calculable? |
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