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This is a pretty out there question... really.
ΔP = -½ρΔ(v²) < 0 (because v_final > v_initial)
- This is proof we lost "pressure" (or kinetic energy that is NOT translational) to translational kinetic energy which does not exert any pressure.
explain this again...?
This is a pretty out there question... really.
ΔP = -½ρΔ(v²😉 < 0 (because v_final > v_initial)
- This is proof we lost "pressure" (or kinetic energy that is NOT translational) to translational kinetic energy which does not exert any pressure.
explain this again...?
This is using bernoulis equation and saying that it equals to zero for that point. We have, therefore, the final equation: Δpressure = -1/2density * Δvelocity^2.
Derived from: ΔP+ dgΔy(which is = 0 since no change in height) + 1/2dΔv^2 = 0
ΔP + 1/2dΔv^2 = 0. For simplicity's sake, we're taking out the 1/2 and density
ΔP +Δv = 0. Subtract the v to get ΔP = -ΔV. We know that we get an increase in velocity, which means a positive Δ, which makes the ΔP a negative increase, which means the pressure decreases.
I don't know how that correlates to KE = 3/2RT, though.
Couldn't you just use PV = nRT? Pressure decreases and therefore the temperature decreases since volume remains?
Actually, I'm an idiot. Temperaute is average kinetic energy of a particle. It all comes together!![]()
The 'v' in Bernoulli's equation (which is invaluable for fluids in motion) is the velocity, not the volume 🙂ΔP + 1/2dΔv^2 = 0. For simplicity's sake, we're taking out the 1/2 and density
ΔP +Δv = 0. Subtract the v to get ΔP = -ΔV. We know that we get an increase in velocity, which means a positive Δ, which makes the ΔP a negative increase, which means the pressure decreases.
I don't know how that correlates to KE = 3/2RT, though.
Couldn't you just use PV = nRT?
This is a pretty out there question... really.
ΔP = -½ρΔ(v²) < 0 (because v_final > v_initial)
- This is proof we lost "pressure" (or kinetic energy that is NOT translational) to translational kinetic energy which does not exert any pressure.
explain this again...?
That statement above says that because the velocity increased, the pressure decreased.
There are two types of kinetic energy that I'm familiar with: 1) the kinetic energy of a molecule associated with its high speed random motion (which is also associated with its pressure and thermal energy), and 2) the translational kinetic energy of a large moving body (i.e. a fluid mass flowing in one direction).
Pressure decreasing will cause a reduction in type 1 kinetic energy.
Since KE = 3/2 RT, KE is proportional to T, so if KE goes down, T must go down.
And, its important to note that you cannot use PV=nRT here because PV=nRT is the "ideal gas" law and we're working with ideal fluids in motion.
What personally gets me is that if you take some water and run it through a very long tubing it will increase in energy. But, I think that's from friction increasing its internal energy, so in the case where there is no friction, I guess that wouldn't happen and we'd get the result I described.
No, I know that. God, if I don't know that by now, I've been getting remarkably lucky on questions.The 'v' in Bernoulli's equation (which is invaluable for fluids in motion) is the velocity, not the volume 🙂

This is a pretty out there question... really.
Okay, so, when this fluid in motion speeds up it loses pressure because it loses its "random motion" kinetic energy to a translational kinetic energy. Random motion kinetic energy is the one related to temperature.
So, we can look at it this way:
ΔP + ρgΔy + ½ρΔ(v²) = 0 ; rewritten in terms of the energy values being conserved here and nothing there is no ρgΔy (no change in gravitational potential energy of the fluid):
ΔP = -½ρΔ(v²) < 0 (because v_final > v_initial)
- This is proof we lost "pressure" (or kinetic energy that is NOT translational) to translational kinetic energy which does not exert any pressure.
Their explanation calls on KE = 3/2 RT, so we can rewrite this as ΔKE = 3/2 RΔT
ΔT = 2/3ΔKE this tells us that since ΔKE < 0, that ΔT< 0, so the temperature had to go down.
This is according to their explanation; personally, I would have thought that temperature would have increased -- but maybe it wouldn't in the absence of friction?
Best summation EVER👍Yeah, you've got it. I know, it's one of those "concept" Qs that's so typically EK... probably beyond scope of MCAT, but you never know.
I don't remember what page this was on, but EK gave the example of running through this area with bees chasing you... ring a bell? Anyway, their whole point is that there are two different types of velocity:
"Random" motion which is just like Brownian motion (I think of it as just vibrating molecules), and "translational" motion which is actual displacement in the direction of your motion. So random motion is responsible for temp, and translational motion is what we usually associate with KE.
Then it's just a matter of energy conservation: higher temperature fluid uses up more of its energy on "random" motion, so less of it is freed to actually move forward as a collective entity (as opposed to random motions of individual molecules). A lower temperature fluid uses up less of its energy just vibrating around, so has more energy available to it to move forward as a collective entity.
Anyway, that's how I think about it... sounds like you've got a good handle on it now, but it helped me just to type that out again.. heh.
BUT, on audio osmosis disc 3 track 12 (fluids in motion) Jordan says, "when the molecules of a fluid move faster, the fluid gets hotter."
You need to listen to the rest of the track (it's only 75 seconds long!). Jon explains the difference between random translational motion which creates temperature, and uniform translational motion which does not.