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myv65 · 10-17-2002, 12:26 PM

There's been a few discussions lately about maximizing velocity within a water cooling system. I'd like to point out that it is a simple matter to calculate the absolute maximum velocity that a given pump can produce. This information is really of limited use, as we'll see shortly, but may prove interesting to some.

Pumps all have a dead-head pressure limit. This is the static pressure they'll generate when zero flow occurs. Static pressure and velocity are simply different forms of energy with the former representing potential and the latter representing dynamic.

Ignoring losses, you can equate head with velocity using the same equations for free-fall of an object. Namely that distance equals 1/2 * acceleration * time^2. If you have a pump that dead-heads at 1 meter, then you use the equation to solve for time. Time equals (distance * 2 / acceleration)^(1/2), so time equals (1 * 2 / 9.81)^(1/2) = 0.45 seconds. Velocity equals time * acceleration, so maximum theoretical velocity equals 0.45 * 9.81 = 4.42 meters/second.

Using dead head levels of 1.5 and 2 meters yields 5.42 and 6.26 meters/second.

OK, so what does this really mean? If you dead-head the pump and pop a hole at the same elevation as the pump outlet, you'll never see a velocity higher than the equations show. The actual velocity you would see is a function of the hole. Standard engineering charts define head loss for various types of orifice and entrace conditions. In general, you'll never get more than about 70% of the value shown by the equations above. More realistically, a number around 50% would be more accurate.

I said earlier this information is of limited use. These conditions exist only when a pump is dead-headed. As soon as you allow some flow, the maximum velocity you'll ever see begins to drop. For a given pump, you could run tests to determine the maximum obtainable velocity versus flowrate. It will vary with flowrate and obviously vary for different pumps. The only thing you can easily state with confidence is that a given pump will never exceed X.XX meters/second.

Just something to keep in mind as you try to balance flow restrictions/velocity increases with your particular pumps and an easy way to peg absolute limits that you can't physically attain.

10-17-2002, 12:26 PM	#1
myv65 Cooling Savant Join Date: May 2002 Location: home Posts: 365	Pumps and peak velocity There's been a few discussions lately about maximizing velocity within a water cooling system. I'd like to point out that it is a simple matter to calculate the absolute maximum velocity that a given pump can produce. This information is really of limited use, as we'll see shortly, but may prove interesting to some. Pumps all have a dead-head pressure limit. This is the static pressure they'll generate when zero flow occurs. Static pressure and velocity are simply different forms of energy with the former representing potential and the latter representing dynamic. Ignoring losses, you can equate head with velocity using the same equations for free-fall of an object. Namely that distance equals 1/2 * acceleration * time^2. If you have a pump that dead-heads at 1 meter, then you use the equation to solve for time. Time equals (distance * 2 / acceleration)^(1/2), so time equals (1 * 2 / 9.81)^(1/2) = 0.45 seconds. Velocity equals time * acceleration, so maximum theoretical velocity equals 0.45 * 9.81 = 4.42 meters/second. Using dead head levels of 1.5 and 2 meters yields 5.42 and 6.26 meters/second. OK, so what does this really mean? If you dead-head the pump and pop a hole at the same elevation as the pump outlet, you'll never see a velocity higher than the equations show. The actual velocity you would see is a function of the hole. Standard engineering charts define head loss for various types of orifice and entrace conditions. In general, you'll never get more than about 70% of the value shown by the equations above. More realistically, a number around 50% would be more accurate. I said earlier this information is of limited use. These conditions exist only when a pump is dead-headed. As soon as you allow some flow, the maximum velocity you'll ever see begins to drop. For a given pump, you could run tests to determine the maximum obtainable velocity versus flowrate. It will vary with flowrate and obviously vary for different pumps. The only thing you can easily state with confidence is that a given pump will never exceed X.XX meters/second. Just something to keep in mind as you try to balance flow restrictions/velocity increases with your particular pumps and an easy way to peg absolute limits that you can't physically attain.