Week 5 (Intro and Static Pressure 1) Flashcards

Introduction to Fluid Mechanics and Static Pressure

1
Q

What’s a fluid?

A

Anything that continuously deforms under a shear stress (applied on it’s surface)

Anything that flows
Any liquid or gas

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2
Q

How is fluid mechanics relevant to biomedical engineering?

A

Cardiovascular system
Diagnostic tests
Reproduction
Some diseases (e.g sickle cell, gestational diabetes)

Fluid mechanics is relevant to all parts of engineering

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3
Q

Fluids have many properties, the 2 we are concerned about are:

A

Density
Viscosity

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4
Q

Viscosity

A

Measure how difficult it is to make it flow

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5
Q

How does pressure act in fluids

A

In all directions
Tries to squash or crush submerged things
Always acts perpendicular (normal to surface)

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6
Q

We generally got flow from high to low pressure, but pressure exists even when….

A

Fluid is not moving (static pressure)

Need to build structures to withstand

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7
Q

What causes pressure?

A
  • In a solid, weight solid above
  • In a fluid, weight fluid above
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8
Q

How do you derive the equation 𝑝= 𝜌𝑔ℎ

A

Consider the weight of fluid above him

*Take a cylinder with area, A
𝐹 = 𝑚𝑔

  • What is mass of the cylinder? (Density x Volume) 𝑚 = 𝜌𝑉 = 𝜌𝐴ℎ
    𝐹 = 𝜌𝐴ℎ𝑔
  • Pressure is Force/Area 𝑝 =𝐹 /𝐴 =𝜌𝐴ℎ𝑔 /𝐴 = 𝜌𝑔ℎ
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9
Q

the pressure equation for in a liquid isn’t dependent on what variable?

A

𝑝 =𝐹 / 𝐴 =𝜌𝐴ℎ𝑔 / 𝐴 = 𝜌𝑔ℎ

  • Doesn’t depend on area!
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10
Q

Pressure depends on:

A

Pressure = Fluid Density ×
Accel. due
to Gravity × Depth

𝑝 = 𝜌𝑔ℎ

  • Doesn’t depend on area or shape!
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11
Q

What if more than one layer of fluid? E.g. oil on water

A

we can simply add up the pressures
* Total weight of fluid above

F = total mass x g
total mass = mass of water + mass of oil

p = F / A

using mass = density x volume (i.e A x h)

You get
p = rho1.g.h1 + rho2.g.h2

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12
Q

what measures atmospheric pressure?

A
  • Barometer measures atmospheric pressure
  • Mercury exposed to atmospheric pressure and a vacuum
  • Impossible to make a perfect vacuum - Pressure in ‘vacuum’ is ‘vapour pressure’ (very close to zero)
  • Difference in height is due to atmospheric pressure
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13
Q

How do you calc atmospheric pressure using a barometer?

A

h, is the height from the bottom surface of the mercury from the barometer to the beginning of the vacuum

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14
Q

In a barometer, why use Mercury and not water, to measure atmospheric pressure?

A
  • How high would column of water be? ∆𝒑 = 𝝆𝒈𝒉
    𝒉 = 𝒑 / 𝝆𝒈
    𝒉 = 10.3m
  • Very high!

Alternatively the density of mercury is much higher.

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15
Q

Including atmospheric pressure

  • Was our earlier calculation wrong? Do we need to think about atmospheric pressure too?

Just treat atmosphere as another
layer of fluid

Final Equation:

A

pressure = p (atm) + rho1.g.h1 + rho2.g.h2

Therefore whenever you solve a problem you need to always take into account atmospheric pressure (add it on).

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16
Q

What is the net pressure for the example of a leaky kettle?

A

What is the pressure driving the fluid out?
P out = Patm + rho.g.h

P in= P out

net pressure: P = P out - P in = rho.g.h

Atmospheric pressure cancels out anyway!

17
Q

Gauge Pressure

A

We ignore atmospheric pressure – we measure the difference between pressure inside the kettle and outside it

Therefore if we use the gauge pressure don’t need to recalculate for e.g La Paz or anywhere!

  • Similar to how we use degrees Celsius instead of Kelvin
  • Except we can choose our ‘zero point’ depending on the context
  • Gauge pressure doesn’t have to be measured with respect to atmosphere.
  • For example
  • Inside an aeroplane, you might measure with respect to cabin pressure instead of atmosphere
  • Inside the lungs, you might measure with respect to minimum pressure during a breath
18
Q

‘Absolute pressure’ includes…

A

the atmospheric pressure

19
Q

What if we want to measure gauge pressure in an engine?

Could hook engine up to a barometer . . . But this measures absolute pressure
(i.e. it includes atmospheric pressure)

What if we used two barometers – one for engine and one for atmospheric?

There is a simpler way:

Can we find 𝒑(𝒆𝒏𝒈𝒊𝒏𝒆)?

A

Use a manometer, through the use of a U-bend

Fluid heights are different, because they feel different pressures

𝒑(𝒆𝒏𝒈𝒊𝒏𝒆) = 𝜌𝑔Δℎ
note, this is for gauge pressure

where delta h, is the height difference between the 2 meniscus.

absolute pressure = atmospheric pressure + rho.g.delta h (gauge pressure).

Absolute pressure can be measured using a barometer

Gauge pressure for an engine by using a manometer

20
Q

What causes static pressure?

A

caused by the weight of fluid above

21
Q

Why is static pressure important?

A
  • Induces forces on submerged structures
22
Q

Tank of water – what is the force
experienced by the bottom surface?

A
  • Absolute pressure on the bottom surface
    includes 𝜌𝑔ℎ (due to water) and
    atmospheric pressure
  • But atmospheric pressure also acts
    upwards – so can cancel out
  • Only consider gauge pressure

Force = pressure × Area
Fy = p.A = rho.g.h.A

23
Q

Tank of water

  • What about horizontal force (𝐹x)
A
  • Pressure now varies with depth
  • Take average pressure

Fx = mean p . A

Same as taking the pressure at the mid-depth (depth = h/2)

24
Q

How to calculate using differential calculus (summary)

A
  • Can also calculate forces by looking at force on infinitesimal
    element of the wall and integrating
25
Q

Slightly more complicated example – inclined plate

What are vertical and horizonal forces on
the inclined plate?

A

The pressure always acts perpendicular
to the surface, so the force will have
horizontal and vertical components.

  • Start by getting the magnitude of the total
    force, F

Again we start by averaging the pressures

Average pressure = (Pa (surface) + Pb (bottom container)) / 2

Pa = 0
Pb = rho.g.h

F = average pressure . A

F = rho.g.h/2.A

What is the area?
𝐴 = 𝐿𝑤
(𝑤 is the direction coming out of the page) ℎ = 𝐿 cos 𝜃

F = average pressure . A = rho.g.h/2.(h/cos 𝜃.w)

F = rho.g.(w.h^2/2cos 𝜃)

Break down in horizontal and vertical components:

Fy = F.sin 𝜃

Fx = F.cos 𝜃

This method works well for simple cases, but sometimes we will need to be a more general approach (e.g. a curved wall, or getting moments instead of forces)

26
Q

A more complex method:

This method works well for simple cases, but sometimes we will need to be a more general
approach (e.g. a curved wall, or getting moments instead of forces)

  • Let’s look at the pressure and forces on a
    single element of the wall
  • 𝑧 is measured along the direction of the wall
A
  • Pressure on the fluid element is
    𝑑𝐹 = 𝑝.𝑑A

Pressure at point z is
𝑝 = 𝜌𝑔ℎ

Where the depth is ℎ = 𝑧.cos 𝜃

Area of element is 𝑑𝐴 = 𝑤.𝑑z

So we get
𝑑𝐹 = 𝜌.𝑔.𝑧. cos 𝜃. 𝑤.𝑑z

We can find the total force, 𝐹, by integration:

F = Integral dF = Integral from L to 0 (𝜌𝑔𝑧 cos 𝜃 𝑤𝑑z)

F = 𝜌.𝑔. cos 𝜃. w. integral from L to 0 (z.dz)

F = 𝜌.𝑔. cos 𝜃. w. [z^2/z] from L to 0

F = 𝜌.𝑔. cos 𝜃. w. (L^2/2)

Remember that
ℎ = 𝐿 cos 𝜃 substitute

F = rho.g.(w.h^2/2cos 𝜃)

Same as we got with previous method!