FRTN65
Exercise 7
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2022 HT/Autumn
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Exercise 7

  • Due No Due Date
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7.1 Dimensionless variables - Water hammer pressure peak when closing a valve
A pressure peak LaTeX: pp can often be heard when closing a valve abruptly, stopping a fluid flow in a pipe.  We can  therefore assume it depends on propagation of pressure waves in the fluid, i.e. the speed  of sound LaTeX: v_{sound}vsound of the fluid (340m/s for air, about 4-5 times faster in water). Our intuition might also say that it depends on the density LaTeX: \rhoρ LaTeX: [kg/m^3][kg/m3]of the fluid and the fluid velocity LaTeX: vv [m/s] before closing the valve.
Find two  dimensionless combinations LaTeX: \Pi_1Π1 and LaTeX: \Pi_2Π2 of LaTeX: pp,LaTeX: v_{sound}vsound,LaTeX: \rhoρ,LaTeX: vv. Can you from this guess the expression for the maximum LaTeX: pp (which is obtained when the closing of the valve is infinitely fast) as a function of the other 3 variables ?
Check your result against the Joukowski formula, described in https://www.youtube.com/watch?v=GfCCsdHKrF8 Links to an external site.
7.2 Dimensionless variables - Resistance when moving through air or water
a) Construct the dimension matrix A of size 3*7 when we consider the variables
Drag force LaTeX: FF [N], Viscosity LaTeX: \muμ [kg/(m s)], Speed of pressure waves in fluid LaTeX: v_{sound}vsound [m/s],  gravitational constant LaTeX: gg[m/s^2] speed of object LaTeX: vv [m/s], characteristic length of object LaTeX: dd [m], fluid density LaTeX: \rhoρ[kg/m^3].
b) Show that you can construct the four dimensionless quantities mentioned in the book,
Pressure coefficient=LaTeX: P_c = \frac{F}{\rho v^2d^2}Pc=Fρv2d2, Reynolds number = LaTeX: R_e = \frac{\rho vd}{\mu}Re=ρvdμ, Mach number = LaTeX: M_m = \frac{v}{v_{sound}}Mm=vvsound,  Froude number= LaTeX: \tilde F_r = \frac{v^2}{gd}˜Fr=v2gd
(literature usually defines "Froude number LaTeX: F_rFr" as the square root  of this expression...)
Note: The typical form of the function P_c=f(R_e) for the drag force of a sphere inside a fluid (for situations where M_m and F_r will not influence the result) can be found on wikipedia here: https://en.wikipedia.org/wiki/Drag_coefficient Links to an external site.

7.3 Flow in a Tube and Reynolds numbers

 

a) At roughly what water flow rate v [m/s] would the water in your garden hose be laminar? Say diameter d=0.01 meter, and say R_e<1000.

b) What is approximately the Reynolds number when you use the water hose ?
c) Same question when you drink water through a straw ?
d) What about when you breathe air through a straw ?
Hint: You might find these links useful
http://www.pressure-drop.com/Online-Calculator/index.html Links to an external site.
Googling gives that max exhale pressure is around 50mbar (female) about double for men. Links to an external site.
Water at room temperature has (dynamic) viscosity around LaTeX: \mu = 0.001 \textrm{ Pa s}μ=0.001 Pa s. (Air has  about 20 times lower dynamic viscosity).

https://www.omnicalculator.com/physics/water-viscosity Links to an external site.

https://www.simscale.com/docs/simwiki/numerics-background/what-is-the-reynolds-number/ Links to an external site.
7.4 Energy intuition
Moving 100kg 1meter vertically requires 1kJoule = 1000Ws = 1000Nm. We also have 1kWh = 3.6MJoule.
Order the energy of the following according to size, and guess roughly how many kJ they correspond to
  • Heating 1kg water 100 degrees
  • Melting 1kg ice (0degree ice -> 0 degree water)
  • Standard 9V battery
  • Energy in 2mF capacitor charged to 230V
  • 1000kg car moving at 50km/h
  • 1 liter of car petrol
  • 1kg chocolate used as food LaTeX: \sim∼ 5000kcal
  • Your daily electric energy consumption
  • A fully charged Tesla electric car
  • Daily consumption of food
  • 1 second usage of ESS

Also construct some rules of of thumb for heat energy:

  • For water, how many meters upwards movement does the energy in a 1 degree temperature increase correspond to ?
  • How many meters up of a 100kg body does daily consumption of food correspond to ?
7.5 About Pressure
SI Units: 1 Pa = 1N/m^2 and 1atm LaTeX: \approx≈1bar LaTeX: \approx≈ normal air pressure LaTeX: \approx≈ 10m water columnLaTeX: \approx≈LaTeX: 10^5105Pa
Find out (Google) What is the typical water pressure at your home? Is it smaller, larger, or about the same as the air pressure in a bike tire? Roughly what pressure can you generate by your lungs? What is approximately the pressure difference inside a balloon compared to surrounding. What is the pressure under your foot if you stand on one leg ?
 
* 7.6 Froude number
A rule of thumb for sailing boats is that a longer boat can sail faster and that speed LaTeX: v_{hull}vhull is proportional to
LaTeX: \sqrt{L}√L. Have a look at https://en.wikipedia.org/wiki/Hull_speed Links to an external site. and formulate the
expression LaTeX: v_{hull}={\sqrt {L_{WL}\cdot g \over 2\pi }}vhull=√LWL⋅g2π as a condition on the Froude number. What is the intuitive explanation to this limit speed ?
Some bonus material:
https://www.youtube.com/watch?v=vcZOk5jZtMA Links to an external site.
7.7 Hydralic jump phenomenon
sink.png
Does the Froude number F_r=1 roughly predict the radius LaTeX: rr for where the hydraulic jump occurs in the water in your water sink at home? Here LaTeX: dd would be the (low)  water depth [m] in the supercritical flow region near the center, and LaTeX: v\left(r\right)v(r)  its (radially outwards) water speed [m/s]. Use that flow rate Q at radius LaTeX: rrwould be LaTeX: Q = d 2\pi r v(r)Q=d2πrv(r) [LaTeX: m^3/sm3/s] and guesstimate Q, d, r
Some related material:
https://www.youtube.com/watch?v=7tjf8HWiR3Y Links to an external site.
https://www.youtube.com/watch?v=UPQz2lwnk9k Links to an external site.
Interesting note: A recent analysis  indicates that the situation is more complicated here, than what was earlier believed: https://www.thechemicalengineer.com/news/circular-hydraulic-jump-not-caused-by-gravity/ Links to an external site.

Bonus: watch the rest of https://www.youtube.com/watch?v=g1Ld8D2bnJM&t=115s  Links to an external site.and https://www.youtube.com/watch?v=KSylo01n5FY Links to an external site.

 

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Week 8