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I'm not sure why they'd use mm H2O either. That said, it seems bizarre to use +PSI as you end up with negative numbers.I can't see using mm of water to measure pressures unless we're talking about very small pressures
So that's how they came up with ATA's... that makes sense.So to relate: 1 Atmosphere = 101325 Pa 1 Bar = 100,000 Pa and the German ATA (technical atmosphere absolute) is Kilograms per centimeter squared
so - 1 ATA = 98066.5 Pa
That's quite a lot of mercuryIn passing: one standard atmosphere will support a column of Mercury 760 mm tall thus 1 ATM = 760 mm of Hg.
That does make using water a bit strange...Since Mercury is 13.6 times denser than water 760 X 13.6 = 10336 mm or 10.336 meters
The problem is I'm not sure what calibrations were used at the time to create the figures. For example 14.70 is commonly seen, it seemed the RAF used 14.696. Technically 14.69595 can be used, but I'm not sure if they entered those numbers, and I'm figuring it might have a slight effect that wasn't in the actual documents.You can't find that yourself?
So, I'll just put 14.69595. Looking at the workbook, the numbers come out close enough.The first and second are rounded from the third.
The USSR seemed to use mmH2OHg. I'm not sure if this was absolute or gauge pressure.
I'm not sure why they'd use mm H2O either.
Yup, we did that experiment at school when I was 13.I can't see using mm of water to measure pressures unless we're talking about very small pressures, One Atmosphere of pressure will support a column of water roughly 33 feet tall (10.06m).
First of all POWER – defined as the RATE at which work is done and WORK is FORCE X DISTANCE.
**N.B.** The Force must be exerted against gravity so strangely enough simply holding a 20 pound weight stationary 4 feet above the floor does zero work! Holding a 20 pound weight at a constant 4 feet above the floor as you move laterally 20 feet also does zero work. Now raising the weight from the floor to a height of 4 feet does do work. 20lb X 4ft = 80 ft x lb of work
n physics, work is the product of force and displacement. A force is said to do work if, when acting, there is a movement of the point of application in the direction of the force.
For example, when a ball is held above the ground and then dropped, the work done on the ball as it falls is equal to the weight of the ball (a force) multiplied by the distance to the ground (a displacement). When the force {\displaystyle F}F is constant and the angle between the force and the displacement {\displaystyle s}s is θ, then the work done is given by W = Fs cos θ.
Work is a vector quantity, so if you spend a lot of energy moving the couch all around the lounge room only for it to end up in the same spot you've done no work.
You are correct and I stand corrected. I was thinking in terms of gravitational potential energy. To do work there must be a displacement in the direction of the force. Pushing all day against a building until you collapse does zero work and although Force was exerted there was no displacement and thus no work was doneThe Force does NOT have to be exerted against gravity.
Add the word "TOTAL" and we're in agreement pushing the couch and moving it does do work. Eastward displacement does positive work as does moving it northward. Westward movement and southward movements are negative displacements. If the couch returns to the same location the the vector sums will indeed total zeroyou've done no work.
It matters. If you apply a Force and that Force or component thereof produces a displacement in the direction of that force or component then you do work.it does not matter if it was moved sideways.