Hydrodynamik I & II Flashcards

1
Q

Definition of a fluid

A

A fluid deforms continuously, no matter whether the stress is large or small. That means that the constituent parts do not have the same velocity.

Fluids are liquids or gases

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2
Q

What are ideal fluids?

A
  • have no viscosity
  • no regards to molecules colliding with each other
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3
Q

Definition of newtonian fluids.

A

is a fluid in which the viscous stresses arising from its flow, at every point, are linearly correlated to the local strain rate—the rate of change of its deformation over time

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4
Q

Definition of viscosity.

A

RESISTANCE TO FLOW.

is a measure of its resistance to deformation at a given rate.

  • for a liquid - the kinematic viscosity decreases with higher temperature
  • for a gas - the kinematic viscosity increases with higher temperature
  • it expresses interaction between fluid layers that can transfer momentum between them.

Viscous critical force:

F crit= η^2/ ρ

  • if Fs>Fcrit = NICHT visköse Medium –> Turbulente Strömung
  • if Fs laminare Strömung
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5
Q

Definition of viscous force bzw. Scherkraft.

A

fs = −η (v ⋅ A )/d

A: size of the plates

v: speed
d: distane between plates

η : viscosity of the medium

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6
Q

What is the newtons law of viscosity?

A

–>definition of shear stress, the stress on a surface in y- direction due to flow in x-direction

—> dvx/dy : Shear rate (const= newtonian fluid) it is just a gradient of velocity in a flowing material.

Viscosity = const —> Newtonian fluid

n = f (dVx/dy) –> depends on rate of deformation–> NON newtonian fluid

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7
Q

Explain the diferent plots of shear stress / shear rate, and what meaning do they have to the fluid dynamics.

A

….

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8
Q

Explain the no slip condition and boundary layer flow in the two plates experiment.

A

Experiment: two layers and in between a fluid. The upper layer in moving while the other is static. The fluid is moving on the x axis, whereas the shear force is applied in the opposite direction. A flow profile is created, where the smaller the h (distance between the plates) the linear the correspondace.

  • the fluid at boundaries move at same velocity as boundary. Meaning: vx (y=0) = 0 ; vx (y=h) = v.
  • je näher an der bewegliche Platte, desto schneller die Bewegung der visköse Fluid ist.
  • Für ganz kleine h –> lineare Anstieg, also vx (y)= vy/h

Boundary layer:

the distance z = dL when v = 0.99 v . But, dL gets larger with increasing distance from the leading edge of the plate. With increasing thickness of the layer, it becomes unstable which leads to turbulence. This transition is accompanied by a sudden increasing friction and thickness of the boundary layer (dL ≤dT)

*

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9
Q

definition of laminar flow

A

Laminarefluß ist der parallele Fluss von Partikeln. Es kommt zustande, wenn die Viskosität groß ist und die Strömmung dadurch bestimmt wird.

  • The velocity profile resembels a deck of cards. No cross-currents perpendicular to the direction of flow.
  • The velocity of flow varies from zero at the walls to a maximum along the cross-sectional centre of the vessel.
  • At lower velocities.
  • Re > 10^4 transition from laminar –> turbulent flow
  • Fs = viskose kritische Kraft =
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10
Q

What is the viscous critical force and what does it measures?

A

Viscous critical force:

F crit= η^2/ ρ

  • if Fs>Fcrit = NICHT visköse Medium –> Turbulente Strömung
  • if Fs<fcrit> laminare Strömung</fcrit>
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11
Q

What is the Reynolds number? helps predict flow patterns in different fluid flow situations. At low Reynolds numbers, flows tend to be dominated by laminar (sheet-like) flow, while at high Reynolds numbers flows tend to be turbulent

A

The Reynolds number is the ratio of inertial forces to viscous forces within a fluid which is subjected to relative internal movement due to different fluid velocities.

  • helps predict flow patterns in different fluid flow situations. At low Reynolds numbers, flows tend to be dominated by laminar (sheet-like) flow, while at high Reynolds numbers flows tend to be turbulent
  • aminar flow occurs at low Reynolds numbers, where viscous forces are dominant, and is characterized by smooth, constant fluid motion

Re = ρuL /μ = uL/v

where:

ρ is the density of the fluid (SI units: kg/m3)

u is the flow speed (m/s)

L is a characteristic linear dimension (m)

μ is the dynamic viscosity of the fluid (Pa·s or N·s/m2 or kg/(m·s))

v is the kinematic viscosity of the fluid (m2/s)

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12
Q

Relation between Re , F crit, & laminar/turbulent flow.

A
  1. Re small = laminar flow –> Fs < Fcrit => viscous medium
  2. Re big = turbulent flow –> Fs > Fcrit => not viscous medium

–> Pt : point of transition from laminar to turbulent flow mit zunehmender Länge und Geschwindigkeit. ( Re= 10^4 = 2000)

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13
Q

define kinematic viscosity.

A
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14
Q

define shear strain

A
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15
Q

Explain Stockes Law

in a falling sphere viscosimeter;

A
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16
Q

Wann stoppt ein Bakterium, wenn es aufhört aktiv zu schwimmen?

A
17
Q

What distance is it E. coli still swimming after it stops beating the flagellum?

A
18
Q

How much POWER is needed to push a bacteria forward?

A
19
Q

Erklären Sie den Fluss durch Kapillaren als Fluss durch Konzentrichen Röhren dargestellt wird.

A

–> The inner cyclinders move faster than the outer ones

  1. the central cylinder has a driving force. F= π* r^2 * pressure difference.
  2. there is also a frictional force, Ff= (2πrl)*η* (-dv / dr) , the laste term is the shear rate. => Ff changes with the radius
  3. Fd = Ff at steady movement => π* r^2 * pressure difference = (2πrl)*η* (-dv / dr)
  4. Through integration–> velocity profile. v(r) = - (dif. p/ 2πlη) * (1/2*r^2 +C)
  5. At no slip condition: r= R & v(r) =0 –> goes to zero.
  6. v(r) = - (dif. p/ 2πlη) * (R^2 -r^2) => PARABOLIC FUNTION

=> vmax is at the center, where r=0, and the flow has the largest distance from the surface.

20
Q

What is volume flow (Jv) and what is its relation with the Hagen-Poiseuille equation?

A

Beschriebt die laminare Strömung eines homogenen Newtonsche Fluids durch ein Rohr in abhängigkeit von Eigenschaften vom Fluid und Rohr.

  • incompressible fluids
  • laminar flow

–> Blood flow!

  • der Fluss in den Kapillaren hängt von der 4te Potenz von R ab
  • Bei einer Innendurchmesser Verdopplung –> hohen Fluss bzw. hohen Druck
  • pressure increase –> Jv will increase
  • if the viscosity of blood increases –> Jv will decrease
21
Q

Explain the following Begriffe and its consequeances in fluid dynamics.

  1. Arteriosclerosis
  2. Stenosis
  3. Aneuryms
A
  1. Arteriosclerosis: Thickening of the walls of the arteries and more rigidyty in them. –> for the same flow the blood pressure must increase
  2. Stenosis: narrowing of the arteries –> in arties radius are decreased so is the volume flow rate, which leads to low blood pressure.
  3. Aneurym: blowing out of the arteries, wall thickness –> turbulent flow
22
Q

Properties of blood in fluid dynamics

A
  1. non- newtonian fluid, which means that the viscosity represents a function of the shear rate or of the dv/dh. (fluid)
  2. Viscosity is reduced at higher flow pressure
  3. The increase of η at low flow speed is caused by aggregation of the erythrocytes into rouleaux (“Geldrollenbildung”)
  4. Viscosity increases with the haematocrit, 50% more –>2*η
  5. Blood Cells are strongly deformed in narrow capillaries.
  6. In large vessels the RBCs concentrate in the centre of the vessel, where the shear is minimal => flattering og the flow parabola
  7. Capillary diameter is not constant and the velocity profile is only slowly adapting.
  8. Pressure of blood is PULSED. –> partially compensated by elastic blood vessels.
  9. VISCOELASTIC ( due to RBCs), η alters as a function of time after a change in stress.
  10. Pulse speed: function of DENSITY (ρ) not viscosity. –> Moens-Kortevef equation
  11. Branching points are critical for maintaining laminar flow.
  • low bifurcation angles - laminar flow, bigger angles turbulence.
  • The Pt bzw. critical Re. depends on the angle α , Re higher for a high angle.
23
Q

What is the Farheus-Lindqvist Effect?

A

describes how the viscosity of a fluid, in this case blood, changes with the diameter of the tube it travels through. In particular there is a ‘decrease in viscosity as the tube’s diameter decreases

–>This is because erythrocytes move over to the centre of the vessel, leaving only plasma near the wall of the vessel.

24
Q

How does a sudden narrowing of a vessel affects the velocity profile?

A

–> narrowing of the parabolic profile in order to maintain laminar flow

25
Q

What is the pulsed speed and which equation describes it?

A

is the velocity at which the blood pressure pulse propagates through the circulatory system, usually an artery or a combined length of arteries. PWV is used clinically as a measure of arterial stiffness.

26
Q

Explain the picture.

A

Um noch laminare Strömungen innerhalb des Blutflusses zu haben, ist es wichtig kleine Verweigungen und demzufolge kleine Winkel, um LAMINARE Strömungen aufrechzuerhalten.

Kritische Reynoldszahl ( ab 2000 gibt es Turbulenzen) ist von den Branching points winkel abhängig.

27
Q

How does the flagellar propulsion ( in 1-2µm: bacteria, archaea) work?

A
  1. Rotary motor turn the flagella relative to the body with the frequency ω.
  2. Torque (Drehmoment)is generated by rotation and it is opposed by viscous drag, due to counter-rotation of the cell body
  3. Thrust (Vorstoß) generated by the flagellum is balanced by drag, due to translation of the body.

= the Bacterium rotates in CW motion with a spcf. frequency.

28
Q

What are the components of the drag in bacterial propulsion ?

A

FΩ = Reibung im Schwimmrichtung

FΩ´ = Reibungskraft entgegen der Drehrichtung -> WOBLING

  1. FΩ & FΩ´ = TORQUE- Drehmoment
  2. Fv and Fv´ = THRUST- Vorstoß

–> Wenn sich FΩ & FΩ´ nicht während der Rotation balancieren ensteht CONICAL WOBLING.

29
Q

Which modes of flagellar beating exist in eukaryotes?

A
  1. UNDULATION MODE
  • Flagelattes and mammalia sperm
  • no helix, rotation –> Reibung beim Vorstoß
  • flagellare Welle nach rechts, dann erfolgt eine Bewegung nach links.
  1. BREAT STROKE MODE
  • aka. Power recovery stroke
  • Vorward ( power) =/= Back (recovery) stroke –> Netto Kraftbewegung nach VORNE
  • Power stroke = forward movement
  • Recovery stroke = brings flagellum in start position
30
Q

What is the geometric cluth model?

A
  • molecular mechanism how bending of the cilia or flagella