Confused about water/compressed air

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A fire protection technician is confused about why the pressure reading in a fire hydrant barrel exceeds the expected 150 psi when filled with water, despite the air inside being at atmospheric pressure. The discussion reveals that the gauge measures pressure relative to atmospheric pressure (psig), and the increased reading may be due to hydrostatic head effects from the hydrant's elevation. Participants explain that in static conditions, air pressure should equal water pressure at the same level, but the elastic nature of gases can lead to higher readings during filling. The technician seeks a formula to calculate the pressure increase based on variables like water volume, psi, and temperatures. The conversation highlights the importance of understanding pressure dynamics in fire hydrant systems to prevent potential damage or safety hazards.
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This is my first post in this forum. First and foremost, big thanks to anyone who takes time out to help me with this. I work for a fire protection company; one thing i service is fire hydrants.

I recently discovered this and do not understand why this is happening:
A hydrant contains only air in its barrel at atmospheric pressure. When the hydrant valve is opened and the 150psi water source begins to fill the hydrant, the air in the hydrant is compressed. (Note: the hydrant is not discharging water, only filling the air occupied barrel between the valve and top section.) This is to be expected. However, when a gauge is placed on the top section to measure the pressure in the barrel I expected to find the gauge reading 150psi - the water source pressure. Instead the pressure was much higher. Anyone know why or know of a formula to calculate this? Thanks for any info in advance!
 
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matt81turner said:
This is my first post in this forum. First and foremost, big thanks to anyone who takes time out to help me with this. I work for a fire protection company; one thing i service is fire hydrants.

I recently discovered this and do not understand why this is happening:
A hydrant contains only air in its barrel at atmospheric pressure. When the hydrant valve is opened and the 150psi water source begins to fill the hydrant, the air in the hydrant is compressed. (Note: the hydrant is not discharging water, only filling the air occupied barrel between the valve and top section.) This is to be expected. However, when a gauge is placed on the top section to measure the pressure in the barrel I expected to find the gauge reading 150psi - the water source pressure. Instead the pressure was much higher. Anyone know why or know of a formula to calculate this? Thanks for any info in advance!

Sounds like a bad gauge...unless the air pressure that exists before you open the valve is a lot higher than the 150 psi of the water...but that would mean your water pressure is also now higher...

CS
 
Your gauge wouldn't be measuring in psia would it?
 
The gauge is calibrated and measures PSI/kpa. Forgive me, I am not familiar with the difference between psig and psia. The air in the barrel is at atmospheric pressure and temperature as well. When I contacted the hydrant manufacturer I was told this was normal and would occur every time. Now I am scratching my head. The only other variable that I think may be relevant is the water source temperature is going to be lower than atmospheric air temperature.
 
matt81turner said:
The gauge is calibrated and measures PSI/kpa. Forgive me, I am not familiar with the difference between psig and psia. The air in the barrel is at atmospheric pressure and temperature as well. When I contacted the hydrant manufacturer I was told this was normal and would occur every time. Now I am scratching my head. The only other variable that I think may be relevant is the water source temperature is going to be lower than atmospheric air temperature.

PSIG is referenced to atmosphere, so atmospheric pressure would read 0 psig whereas it would read about 14.73 psia if the gauge where absolute.

So you are saying that you have a space in the hydrant that is at atomspheric pressure, and then suddenly it is filled with water at a pressure of 150 psi...correct?

The only thing I can think of is that there is a hydrostatic head effect that you are not accounting for somewhere.

CS

EDIT: We're talking about a fire hydrant that's outside on the curb right?
 
stewartcs said:
PSIG is referenced to atmosphere, so atmospheric pressure would read 0 psig whereas it would read about 14.73 psia if the gauge where absolute.

So you are saying that you have a space in the hydrant that is at atomspheric pressure, and then suddenly it is filled with water at a pressure of 150 psi...correct?

The only thing I can think of is that there is a hydrostatic head effect that you are not accounting for somewhere.

CS

EDIT: We're talking about a fire hydrant that's outside on the curb right?

Yes. OK, the gauge is PSIG - not absolute. It reads zero at atmospheric pressure. Right, it's a hydrant like outside at the curb. It's what's called a traffic model. The valve is 5' below grade and above this valve the vertical barrel and top section are dry until this valve is opened.
 
matt81turner said:
Yes. OK, the gauge is PSIG - not absolute. It reads zero at atmospheric pressure. Right, it's a hydrant like outside at the curb. It's what's called a traffic model. The valve is 5' below grade and above this valve the vertical barrel and top section are dry until this valve is opened.

Where is the system pressure of 150 psig measured from? Is it just behind the valve before the space containing atmospheric pressure, or is it measured at some other elevation?

CS
 
The water source pressure is measured at a different location with a calibrated psig gauge at aproximately identical elevation. Hope this helps.
 
matt81turner said:
The water source pressure is measured at a different location with a calibrated psig gauge at aproximately identical elevation. Hope this helps.

Sounds like there is an elevation change that you are experiencing (e.g. you have some extra head pressure due to the hydrant being at a lower elevation than where the system pressure is being measured from).

How high is the pressure above the 150 psig system pressure?

CS
 
  • #10
Not exactly sure how much higher the pressure reading is. My boss recorded them isn't available right now. I greatly appreciate your time and will think about this more and report back tomorrow.
 
  • #11
matt81turner said:
Not exactly sure how much higher the pressure reading is. My boss recorded them isn't available right now. I greatly appreciate your time and will think about this more and report back tomorrow.

No problem...Good luck.

CS
 
  • #12
Unlike liquids, gasses are somewhat elastic. That's why your car has vacuum hoses attached to the intake manifold; as the piston is being drawn down with the intake valve open, a partial vacuum is set up, limiting the amount of air that's available for the stratified charge.
What happens on the exhaust cycle is similar to what's happening in the fire hydrant: as the piston travels upward, exhaust gases are sent through the exhaust valve; however, a region of high-pressure combustion gases is set up that are under much more pressure than the ambient air. Likewise, the water in the hydrant is exerting a tremendous force on the air that you're measuring, and due to air's elastic nature, will be under a pressure that's significantly higher than just 150 psig.
 
  • #13
Thanks guys. I like to think of myself as a pretty intelligent person, but physics doesn't take long to make my brain hurt. I appreciate the insight. Now, if I could just come up with a formula that takes the variables (water volume and psi, ambient air volume and the temperatures) so that I can calculate the rise in pressure that will occur in the barrel. See, the problem stems from this: The water source pressure (approx 150psi) is below the hydrant's rated pressure, but the pressure we are recording once the barrel is filled with water and the ambient air is compressed is higher than what the hydrant is rated for. This, as you may have guessed, can cause hydrant and other property damage and even injury or death as these hydrants we service are in industrial plants.
 
  • #14
Neo_Anderson said:
Unlike liquids, gasses are somewhat elastic. That's why your car has vacuum hoses attached to the intake manifold; as the piston is being drawn down with the intake valve open, a partial vacuum is set up, limiting the amount of air that's available for the stratified charge.
What happens on the exhaust cycle is similar to what's happening in the fire hydrant: as the piston travels upward, exhaust gases are sent through the exhaust valve; however, a region of high-pressure combustion gases is set up that are under much more pressure than the ambient air. Likewise, the water in the hydrant is exerting a tremendous force on the air that you're measuring, and due to air's elastic nature, will be under a pressure that's significantly higher than just 150 psig.


If you are talking about the static condition, the pressure in the air cannot be different from the pressure in the water (at the same level) or the water level would change accordingly. The fact that the air is springy is not relevant. Think of a mechanical analogy: the tension in a (rigid) wire will be exactly the same as in a spring that it pulls against.

There is a relevant difference, however, and that is in the enormous amount of energy stored in compressed air compared with the very small amount of energy stored in an almost incompressible fluid like water. This is because you do much more work in compressing a large volume of air into a small volume in order to raise the pressure significantly - the work done is pressure change times volume. Your air assisted brakes use this energy. There is virtually no change in the water volume so very little energy involved.
 
  • #15
Neo_Anderson said:
Unlike liquids, gasses are somewhat elastic. That's why your car has vacuum hoses attached to the intake manifold; as the piston is being drawn down with the intake valve open, a partial vacuum is set up, limiting the amount of air that's available for the stratified charge.
What happens on the exhaust cycle is similar to what's happening in the fire hydrant: as the piston travels upward, exhaust gases are sent through the exhaust valve; however, a region of high-pressure combustion gases is set up that are under much more pressure than the ambient air. Likewise, the water in the hydrant is exerting a tremendous force on the air that you're measuring, and due to air's elastic nature, will be under a pressure that's significantly higher than just 150 psig.

This is not what is happening here. If the air is exposed to the fluid and it is in static equilibrium, the air pressure must equal the water pressure. Nothing more to it than that.

CS
 
  • #16
matt81turner said:
Thanks guys. I like to think of myself as a pretty intelligent person, but physics doesn't take long to make my brain hurt. I appreciate the insight. Now, if I could just come up with a formula that takes the variables (water volume and psi, ambient air volume and the temperatures) so that I can calculate the rise in pressure that will occur in the barrel. See, the problem stems from this: The water source pressure (approx 150psi) is below the hydrant's rated pressure, but the pressure we are recording once the barrel is filled with water and the ambient air is compressed is higher than what the hydrant is rated for. This, as you may have guessed, can cause hydrant and other property damage and even injury or death as these hydrants we service are in industrial plants.

Since this is a static system, you only need to know the pressure at one elevation (the 150 psig at whatever elevation), and the elevation change to the fire hydrant. The new pressure will be 150 +/- head pressure due to the elevation change. If the hydrant is lower than the referenced elevation (the point where the 150 psig is measured from) the head added will be positive. I suspect this is the case.

It would be helpful if you knew could find out how high the pressure is at the hydrant to get some idea of the elevation changed.

CS
 
  • #17
sophiecentaur said:
If you are talking about the static condition, the pressure in the air cannot be different from the pressure in the water (at the same level)
I think this is the key point.

To the OP: is the increased pressure a transient thing where it spikes up and then settles down to the 150 psi, or is it static even after you wait for a while.
 
  • #18
stewartcs said:
This is not what is happening here. If the air is exposed to the fluid and it is in static equilibrium, the air pressure must equal the water pressure. Nothing more to it than that.

CS

I'd expect a post like this from someone with just a couple of posts, but a Science Advisor getting it wrong?

Consider a closed, gaseous cavity that's halfway filled with water. Insert a pressure gauge in the middle of the cavity that's taking a reading of the gas, and another pressure gauge in the middle of the water that's taking a reading of that water.
Now, evacuate the gas from the cavity. The gauge that's measuring the gas should read 0 psi, and the gauge that's reading the water should read something other than 0 psi. In fact, the more water that's being measured, the higher the reading of the water gauge. The different reading is due to the gravitational field being exerted on the water which has the effect of increasing the water pressure. Thus, in the static condition, we have the two gauges reading different results.

Apply the same anology to the situation where air is being pumped into the cavity: After the air is pumped in, the gauge situated in the gas will read a very high reading (the gas, after all, is now far more pressurized than the air outside the cavity), and will exert an increase of force on the water that's in the cavity. Since the water does not compress (whereas the gas does compress), the gauge that's in the middle of the water does not change in its reading. Sure, the pressure that's being exerted on the cavity walls itself will be constant (even at the water-cavity interface), but in the center of the water the pressure will not change.

Please correct me if I'm wrong.
 
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  • #19
Neo_Anderson said:
I'd expect a post like this from someone with just a couple of posts, but a Science Advisor getting it wrong?

Consider a closed, gaseous cavity that's halfway filled with water. Insert a pressure gauge in the middle of the cavity that's taking a reading of the gas, and another pressure gauge in the middle of the water that's taking a reading of that water.
Now, evacuate the gas from the cavity. The gauge that's measuring the gas should read 0 psi, and the gauge that's reading the water should read something other than 0 psi. In fact, the more water that's being measured, the higher the reading of the water gauge. The different reading is due to the gravitational field being exerted on the water which has the effect of increasing the water pressure. Thus, in the static condition, we have the two gauges reading different results.

Apply the same anology to the situation where air is being pumped into the cavity: After the air is pumped in, the gauge situated in the gas will read a very high reading (the gas, after all, is now far more pressurized than the air outside the cavity), and will exert an increase of force on the water that's in the cavity. Since the water does not compress (whereas the gas does compress), the gauge that's in the middle of the water does not change in its reading. Sure, the pressure that's being exerted on the cavity walls itself will be constant (even at the water-cavity interface), but in the center of the water the pressure will not change.

Please correct me if I'm wrong.

The part you are missing is that the water has a constant pressure of 150 psig sitting behind a valve. On the other side of the valve there is a cavity with nothing but air in it at atmospheric pressure (which is 0 psig). As soon as the valve is opened, the air will be compressed by the water until it is in equilibrium with the water. In order for it to be in equilibrium with the water, the gas pressure MUST equal the water pressure. Hence, it can only be a maximum of whatever the water pressure is right behind the valve (assumed to be 150 psig based on the OP).

If you still have trouble understanding that, try to imagine a cylinder separated by a piston with water on one side and air on the other with the piston initially locked mechanically (both at 0 psig initially). Now pressurize the water to 150 psig and unlock the piston. What will happen to the air side?

Well, it will be compressed due to the unbalanced force on the piston by the water (F = PA). Since the area of the piston is the same on either side, the force is a function of the pressure only. Since the air pressure is initially 0, and the water is now 150 psig, a greater force is applied to the water side...hence the piston will move such that it compresses the air until the air pressure is equal to that of the water pressure, which will be 150 psig in this example.

CS
 
  • #20
It would seem that you are wrong (if I have understood what you are saying - in particular, I assume what you mean by "the middle of the water" means just below the surface).
The pressure just above and just below the surface of the water must be precisely the same. How could it not be? The respective moduli of the two fluids is irrelevant. If there were a difference in pressure then there would be a resultant force and things would move to change the situation.

stewartcs seems to be right
 
  • #21
DaleSpam said:
I think this is the key point.

To the OP: is the increased pressure a transient thing where it spikes up and then settles down to the 150 psi, or is it static even after you wait for a while.

I don't think his gauge would respond to a pressure transient such as a water hammer effect (I think that's where you are going with this).

Most transient pressures are dissipated within a few seconds anyway, although their pressure increase can be very high.

The only time I've been able to see a pressure transient from a water hammer effect is though electronic instrumentation, and not a gauge. Of course that doesn't mean it couldn't happen!

CS
 
  • #22
CS
It's the very devil to get the precise picture of the situation right so we are all discussing the same thing.
If your water container is rigid and sealed (ideal), when you let the piston go, the water will expand a miniscule amount - until its pressure is the same as that of the air.
If it is constantly topped up from outside, then the piston will move until the air pressure is 150psig. Are we talking constant pressure or constant mass? That is the question.
 
  • #23
sophiecentaur said:
CS
It's the very devil to get the precise picture of the situation right so we are all discussing the same thing.
If your water container is rigid and sealed (ideal), when you let the piston go, the water will expand a miniscule amount - until its pressure is the same as that of the air.
If it is constantly topped up from outside, then the piston will move until the air pressure is 150psig. Are we talking constant pressure or constant mass? That is the question.

I stated that the water pressure is constant which is what is known from the OP. This is a real world system. The system pressure is maintained constant at 150 psig.

CS
 
  • #24
So "rtfop" thoroughly then?
Mea culpa Magister.
 
  • #25
Could there potentially be a back-check valve, perhaps maintaining a "hammer" pressure effect at the head?
 
  • #26
There's no need to do a thought experiement to determine if it's a static condition or not, the OP stated that it is. The only questions are left are the details of the rest of the system.

When he says "industrial plant" I'm assuming it has it's own firewater system. The system should be designed/required to maintain a minimum pressure while supplying a certain number number of hydrants. We'd simply have to find out the control scheme to determine what the supply pressure is supposed to be.

Is 150 psig at the pump discharge? If the system is designed to control at 150 psig, then where is the sensing point in relation to this hydrant?

If we don't get any more info, I'll see what I can dig up as far as standards/requirements (chemical plant).
 
  • #27
Thanks, I will get on that asap.
 
  • #28
sophiecentaur said:
It would seem that you are wrong (if I have understood what you are saying - in particular, I assume what you mean by "the middle of the water" means just below the surface).
The pressure just above and just below the surface of the water must be precisely the same. How could it not be? The respective moduli of the two fluids is irrelevant. If there were a difference in pressure then there would be a resultant force and things would move to change the situation.

stewartcs seems to be right

You guys, this isn't rocket science for cryin' out loud!

Look. Consider a "J"-shaped cavity. Consider that the vertical part of the "J" is quite long in relation to the curved part of the "J". The curved part of the "J" has a 1 foot vertical section after the bend. The entire apparatus is, say, 20 feet long and 12 inches in diameter. It's closed on the curved end and has an opening at the top--or vertical--end.
Now add 20 gallons of water to the "J". What will happen? Yep! That's right--the water will almost fill the whole "J", but will leave a pocket of air at the end of the curved part of the "J" (remember, there's a 1-foot vertical section right after the bend). What's the air pressure in this little region? Far greater than the pressure that's being exerted by the water at the top of the vertical part of the "J"!

Thus we have unequal pressures between one end and the other end, which is the precise discrepancy the OP was bringing to the thread body.
 
  • #29
S_Happens said:
I'll see what I can dig up as far as standards/requirements (chemical plant).

Don't bother. We all should know by now that the unequal air psig measurements are due to the effect of gravity on the water in the watermain, and that the sheer weight of the water on the air pressure that's being measured is the reason for the PSI discrepancy.
 
  • #30
Every ~2.3 feet in elevation difference equals 1 psi. You might have a slope of 1-2%, 1-2 feet per 100 feet of horizontal difference, and it would appear level. Or etc.

But the air pressure at the hydrant is exactly equal to the water pressure at the hydrant. It's the other location and hydrant that are likely different. Or the gauge is giving a bad reading.
Neo_Anderson said:
Now, evacuate the gas from the cavity. The gauge that's measuring the gas should read 0 psi, and the gauge that's reading the water should read something other than 0 psi. In fact, the more water that's being measured, the higher the reading of the water gauge.

Impossible. Water or water vapor will fill the vacuum until the pressures are equalize. Just like when you suck on a straw you reduce the pressure in your mouth. You can't have two different pressures next to each other without causing some flow. This really is a simple situation. Once the water stops moving the air and water are at the same pressure no matter what.
 
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  • #31
Neo_Anderson said:
You guys, this isn't rocket science for cryin' out loud!

Look. Consider a "J"-shaped cavity. Consider that the vertical part of the "J" is quite long in relation to the curved part of the "J". The curved part of the "J" has a 1 foot vertical section after the bend. The entire apparatus is, say, 20 feet long and 12 inches in diameter. It's closed on the curved end and has an opening at the top--or vertical--end.
Now add 20 gallons of water to the "J". What will happen? Yep! That's right--the water will almost fill the whole "J", but will leave a pocket of air at the end of the curved part of the "J" (remember, there's a 1-foot vertical section right after the bend). What's the air pressure in this little region? Far greater than the pressure that's being exerted by the water at the top of the vertical part of the "J"!

Thus we have unequal pressures between one end and the other end, which is the precise discrepancy the OP was bringing to the thread body.

Of course the pressure at the top of the J will be less, it's open to atmosphere and the hydrostatic head from the elevation change is causing the air pressure to be high since it's trapped at the bottom...that's what's been said all along...i.e. the increase in pressure is probably attributed an elevation difference. You need to read the other posts more thoroughly. The elevation change was the first thing I proposed as the cause for the increased pressure. Hence me asking where the 150 psig was measured from.

The air pressure at the air/water interface is exactly the same...which is the crux of the problem. So, if he is reading 150 psig right at the valve, and then the valve is opened, the air pressure in the chamber will equalize to 150 psig. Period.

If the pressure read from another location at a higher elevation, then he'll have to add in the elevation head.

You're right, it's not rocket science, so stop trying to make it to be.

CS
 
  • #32
Neo_Anderson said:
...Likewise, the water in the hydrant is exerting a tremendous force on the air that you're measuring, and due to air's elastic nature, will be under a pressure that's significantly higher than just 150 psig.

This is ridiculous. The "air's elastic nature" (i.e. compressibility) has nothing to do with the air pressure being higher in a static fluid. If two fluids are in static equilibrium together, their pressures are exactly the same at the interface (i.e. same elevation). I refer you again to the example given above about the cylinder/piston.

CS
 
  • #33
You guys manage to get so cross with each other! Why?
I wouldn't mind betting that most of you would actually agree with each other about the basic Physics - it's just that you're not communicating the problem i.e writing what you actually mean and reading what's actually written. TX and RX need to be in sync.
Getting ratty doesn't help the Science one jot nor tittle.
 
  • #34
Neo_Anderson said:
Don't bother. We all should know by now that the unequal air psig measurements are due to the effect of gravity on the water in the watermain, and that the sheer weight of the water on the air pressure that's being measured is the reason for the PSI discrepancy.

I'm well aware of "head" pressure (so is pretty much everyone else in this thread, but you haven't seemed to notice). I'm not talking about flipping through some basic intro to physics book to figure out the magic of manometers. I'm talking about checking OSHA standards and anything else applicable to firewater systems to get any details, because we've been supplied almost nothing.

I asked where the 150 psig supply pressure was being read as well, and how it's being maintained. Even ignoring the fact that the OP doesn't know for certain that the supply is 150 psig, we can be almost certain that there isn't a gauge to read the pressure at the isolation for the hydrant. The systems (dry barrel like the OP is talking about) are setup where the hydrant has an underground isolation valve (two isolations really in case the hydrant needs to be worked on) connecting it to an underground header. The only question is to find out how the header pressure is maintained. The norm for industrial plants is to have their own firewater pumps that pull from a canal/river/large body of water. If this is the case then it might not be elevation change that we need to be concerned with.

I'm sure everyone participating already knew all this as they plow hatred first into this discussion.

It's obviously a simple situation that can be handled without thought experiments, confusion, and frustration.
 
  • #35
It seems obvious to me that your query is, actually, totally specific. The quoted pressure can only apply at the level where it is measured and you'd have to find out which level this is done on the supply. Unless you are drawing a significant flow of water then the head, locally, will differ just by the height difference. The presence of air is pretty much a red herring unless there is a significant height of trapped air. If there is, then the 'dry' pressure will be higher than the 'wet' pressure because air is much less dense. This is unlikely except when the system is first installed because who is going to bother to pump out water from a rising main?

If the gauge is giving a reading which does not agree with the above calculations then it has to be faulty. But this isn't a Physics question; it's surely one for the installer of the system or equipment or the recommendations of the local fire authority / insurance company. Also, if it's a safety of life consideration, I wouldn't rely on the potential BS you can read on a Forum (Mine included)!
 
  • #36
stewartcs said:
This is ridiculous. The "air's elastic nature" (i.e. compressibility) has nothing to do with the air pressure being higher in a static fluid. If two fluids are in static equilibrium together, their pressures are exactly the same at the interface (i.e. same elevation). I refer you again to the example given above about the cylinder/piston.

CS

We're not talking about two [different?] fluids, we're talking about a fluid and a gas in a solid, hollow structure.
The only way the OP could have gotten a very high psig reaading is if the gravitational pull on the liquid caused the high psig reading (every time he measures these things).
It's impossible to proffer an alternate explination unless there are water pumps or other hidden variables involved.
 
  • #37
A gas IS a fluid. So is a liquid.
They will both FLOW - i.e. they are fluid.
 
  • #38
Neo_Anderson said:
We're not talking about two [different?] fluids, we're talking about a fluid and a gas in a solid, hollow structure.
The only way the OP could have gotten a very high psig reaading is if the gravitational pull on the liquid caused the high psig reading (every time he measures these things).
It's impossible to proffer an alternate explination unless there are water pumps or other hidden variables involved.

I'm well aware of what we are talking about.

Yes there are two different fluids. As Sophie has already pointed out, air is a fluid that is in a gas phase.

The gravitational pull that you are referring to is, again, the hydrostatic pressure due to an elevation change. This explanation (elevation change) has been stated over and over and over again in this post as the probable cause.

CS
 
  • #39
This is simple. As has been pointed out, a system at equilibrium must have the same pressure at all points regardless of the media, i.e. air or water, and discounting pressure changes due to elevation. When the valve is first opened, the pressure of the air (at ~0 PSIG, presumably) will increase rapidly up to the pressure at the inlet of the valve. The gauge is at the TOP of the hydrant. Therefore, the highest pressure (due to velocity of the air) is seen at this point, resulting in an artificially high reading. The same would be seen if the hydrant was open to the atmosphere, because the air (or water) has to make a 900 bend at the location of the gauge, transferring kinetic energy to the gauge. This is also one way in which "water hammer" occurs due to the difference in flow rate of compressed air relative to water. (No, water hammer doesn't depend only on a bend, or on air in the pipes.) The inertial energy of the water rushing into the cavity results in a momentary pressure spike before the system reaches equilibrium (that is, stops flowing).

I'm sure that's what you're seeing here. After the sysem reaches equilibrium, the pressure will stabilize. But, it may be less than your source pressure due to pressure drop through the pipes and valves, assuming you have continuous flow. Of course, elevation does affect the pressure and you need to consider that as well.

Sorry it took so long to respond, I'm new here and just saw this thread!
 
  • #40
OK guys. I think I have finally gotten close to figuring this out with the combined gas law.
(P1V1)/T1 = (P2V2)/T2
P is pressure measured in atmospheres
V is volume measured in liters (does this have to be in liters?)
T is temperature in Kelvins

1 variables are initial state (when hydrant is in closed position)
2 variables are end state (after hydrant is opened and filled with water)

It's my understanding that if I can determine the values for P1, V1, T1, T2, and V2 I will be able to solve for P2.
I appreciate all the theories and feedback. Anyone think I am on the right track?
 
  • #41
Of course, when using this formula we are assuming that any other variables such as elevation change are not a factor. With that in mind, anyone see a problem with using this formula?
 
  • #42
Having read all of this stuff again I think we are probably just discussing a transient effect.
Unless there is some detail that has been left out of the original description. What is the timescale for all this to occur? If it's brief, then JohnEJ's idea of 'overshoot' of the mass of water sounds a good one. It would be a damped resonance effect of mass against spring, where the loss is so high than you only get less than one half cycle. If the pressure excess lasts for longer, then it could be explained by initial heating of the body of air as the water rushes in - if there is a non-return valve 'upstream' then the pressure could remain high, until the air cools down to ambient again.
 
  • #43
The elapsed time of this happening is a couple of minutes max. We are going to conduct this test again with a higher gauge since the previous one read 0-300psi and pegged when the water filled the hydrant. There is a check valve upstream at the fire pump hundreds of feet away. (the fire pump is not running during our testing) I didn't originally mention this because we do not believe it to be a factor.
 
  • #44
Hundreds of feet wouldn't make a lot of difference to an incompressible fluid in rigid pipes so JohnEJ's resonance mechanism could well explain the initial rise in pressure being maintained. A couple of minutes timescale makes me think in terms of some thermal effect - or a leak which let's air through but not water and gradually let's the pressure return to the normal water pressure.
 
  • #45
matt81turner said:
OK guys. I think I have finally gotten close to figuring this out with the combined gas law.
(P1V1)/T1 = (P2V2)/T2
P is pressure measured in atmospheres
V is volume measured in liters (does this have to be in liters?)
T is temperature in Kelvins

1 variables are initial state (when hydrant is in closed position)
2 variables are end state (after hydrant is opened and filled with water)

It's my understanding that if I can determine the values for P1, V1, T1, T2, and V2 I will be able to solve for P2.
I appreciate all the theories and feedback. Anyone think I am on the right track?

The equation should be dimensional correct. You could use cubic meters for volume (m^3), but you'll have to use Pascals (N/m^2) for pressure.

I don't think you're on the right track with this though.

CS
 
  • #46
matt81turner said:
The elapsed time of this happening is a couple of minutes max. We are going to conduct this test again with a higher gauge since the previous one read 0-300psi and pegged when the water filled the hydrant. There is a check valve upstream at the fire pump hundreds of feet away. (the fire pump is not running during our testing) I didn't originally mention this because we do not believe it to be a factor.

The timing is critical to answering you question. This is one of possibilities that was presented initially (i.e. water hammer/transient effect).

If the pressure reading is stabilized and you still have a high reading, it's not transient...

If it last only a few seconds (depending on the way the piping is set up with the check valve upstream) then it is most likely transient...However, like I said before, you're probably not going to see the transient on an analogue gauge.

CS
 
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