stewartcs
Science Advisor
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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