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Pressure Variation
#26
Posted 21 October 2015 - 04:59 AM
#27
Posted 21 October 2015 - 05:22 AM
The sketch is correct, apart from in the example I gave the length of the pipe was 100m
The average pressure in your sketched example, and my example (when the pipe is 100m long) increases as the pipe is moved from horizontal to vertical
How does the average pressure (and hence the total energy) increase as the pipe is moved from horizontal to vertical, if no energy is added to the system?
Or is it just that we are getting this extra pressure for free, where did this energy come from?
If pressure at the top of the pipe drops to 95 bar and the base pressure increases to 105 bar, then energy is conserved.
(If you redo your sketch/spreadsheet with the pipe being 100m long, you will more clearly see what I refer to)
Edited by jamese, 21 October 2015 - 05:54 AM.
#28
Posted 21 October 2015 - 06:04 AM
Again im saying you are not getting any free energy. You are rotating the pipe right? That adds the head. You can do a simple experiment. Take a 10m length pipe. Fill it with water in horizontal position and see the pressure at both ends. It will read atm pressure. Next you made the pipe vertical with water, the top end pressure will be atm and bottom pressure will be atm pr + rho x g x h. Do you agree this? Try to make a energy balance calc.
#29
Posted 21 October 2015 - 07:51 AM
According to you, after the pipe is rotated we have more pressure in the pipe than we had in horizontal situation.
Since the top end pressure is the same, and everything from this point downwards is then increased.
This equals more energy.
Edited by jamese, 21 October 2015 - 07:52 AM.
#30
Posted 21 October 2015 - 08:38 AM
#31
Posted 21 October 2015 - 09:17 AM
There is no work done to rotate the pipe, since the pipe rotates at the mid point the pipe is mass balanced.
#32
Posted 21 October 2015 - 11:10 AM
#33
Posted 21 October 2015 - 12:18 PM
The work required to raise it would only be a function of the inefficiency of the bearing it rotates on, which is external to the closed pipe system.
(whilst one end of the pipe raises, the other end drops)
(top end requires work to be raised, lower end does work whilst being lowered = no net work)
Edited by jamese, 21 October 2015 - 12:24 PM.
#34
Posted 22 October 2015 - 01:43 AM
#35
Posted 23 October 2015 - 03:47 AM
OK agreed on the torque.
But putting it another way, in the absence of resisting forces, ie drag and bearing friction (both which are external to the pipe);
If tiny force is instantaneously applied to the pipe (and then removed) the pipe will then start turning.
In the absence of any more force being applied the pipe will continue turning with no additional force applied.
In your scenario the total energy in the pipe varies dependent on its position?, why?
Edited by jamese, 23 October 2015 - 03:48 AM.
#36
Posted 25 October 2015 - 11:02 AM
Edited by samayaraj, 25 October 2015 - 11:08 AM.
#37
Posted 06 November 2015 - 06:20 AM
Dear Jamese,
Good Day.
Please see the spreadsheet in which I have drawn a diagram to illustrate my explanation and confirm if the diagram is in line with your expectations. It is way more easier visualizing it when we draw the diagram.
This answer is with respect to the initial spring shaped pipe you were talking about.
The structure of the spring and thus the system volume does not change. So the pressure at the top cannot
change unless you are accounting for realistic spring buckling (See Spreadsheet) in which case the pressure at the top changes just a wee bit due to pressure increase in fluid which is a consequence of decrease in overall system volume because of buckling. This buckling occurs because no Spring can be compressed without Buckling as it is impossible to do so. The buckling is what stores the elastic energy in the spring.
2. The pressure at the bottom changes due to the reduction in height of fluid above the datum and if you account for the Spring buckling as in the above case in order to be realistic, then that too. Because the pressure increase due to buckling is equally distributed at the top and the bottom.
3. As for the conclusion from your PhD friend, the pressure at the top of the spring only depends on the fluid above that cross section (assumed here as atmospheric air), and the spring buckling, so it cannot change in this case.
Please see the drawing in the Spreadsheet.
Regards,
Shantanu
Attached Files
Edited by shantanuk100, 18 November 2015 - 01:00 AM.
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