An opening of area 0.252 cm2 in an otherwise closed beverage keg is 40.1 cm below the level of the liquid (of density 1.01 g/cm3) in the keg. What is the speed of the liquid flowing through the opening if the gauge pressure in the air space above the liquid is (a) zero and (b)0.532 atm?
@IrishBoy123 can you help me?
toricelli
i know how to do in letter a however, in a letter b i can't seem to get the answer :(
ok so we may have to go back to Bernoulli, again from that Wiki page: \[gz+{p_{atm}\over\rho}={v^2 \over 2}+{p_{atm}\over\rho}\] but here we seem to have different pressures so \[gz+{p_{\color{red}{inside}}\over\rho}={v^2 \over 2}+{p_{atm}\over\rho}\] sove for v from there with a) \(p_{inside} = 0\) and b) \(p_{inside} = ????\) where ??? is (0.5* atmospheric pressure) in SI units
1 thing to be careful about it's gauge pressure so inside for a \(P = P_{atm}\) for b), i think you add a further 0.5 atm been a while
i think gauge pressure is the deviation from atmospheric pressure..
This question is kinda of confusing
I have the same problem also and seems can't get the answer
thank you guys for helping me :)
yes, ganesh, my recollection too, and i have had a check as well so for internal gauge = 0 you get \(gz+{p_{atm}\over\rho}={v^2 \over 2}+{p_{atm}\over\rho}\) \(\implies gz={v^2 \over 2}\) and hence Toricelli for the second where internal gauge = 0.532 you get \(gz+{1.532p_{atm}\over\rho}={v^2 \over 2}+{p_{atm}\over\rho}\) \(\implies gz+{0.532p_{atm}\over\rho}={v^2 \over 2}\) so you plug the numbers [SI uits] into a fuller Bernoulli equation to solve
oh i't not equal to zero :)) but the answer is the same as my a
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