Chapter 4: Fluids Flashcards

1
Q

fluids

A

ability to flow and conform to shapes in their containers

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

solids

A

do not flow and are rigid

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

density

A

ρ = m / V

m = mass
V = volume

unit: kg/m^3 or g / ml or kg / cm^3

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

weight if any volume of a given substance with known density can be calculated:

A

Fg = ρ V g

ρ = density
V = volume
g = gravity

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

specific gravity (SG)

A

SG = ρ / 1 g /cm^3

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

pressure

A

P = F / A

P = pressure
F = force
A = area

units: pascal (Pa) = 1 N/s^2

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

pressure units conversions

A

1.013x10^5 Pa = 760mmHg = 76o Torr = 1atm

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

how can we calculate the difference in prressure?

A

Fnet = PnetA
Fnet = (Poutside - Pinside) A

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

absolute (hydrostatic) pressure

A

total pressure that is exerted on an object that is submerged in a fluid

P = Po + ρ g z

P = absolute pressure
Po = ambient pressure (pressure at the surface)
ρ = density
g = gravity
z = depth of the object

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Gauge pressure

A

difference between the absolute pressure and the atmospheric pressure

Pgauge = P - Patm = (Po + ρgz) - Patm

note that when Po = Patm, then Pgauge = P - Po = ρgz

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

hydrostatic

A

Study of fluid at rest and the forces and pressure associated with standing fluids.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

pascal principle

A

Changing pressure will be transmitted undiminished to every portion of the fluid into the walls of the container.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

pascals equations

A

P = F1/A1 = F2/A2

F2 = F1 (A2/A1)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

volume of fuid displaced by piastal 1 will be the same volume of liquid displced by piston 2

A

V = A1d1 = A2d2

d2 =d1 (A1/A2)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

Archimedes’ priciple deals with buoyancy of objects when placed in a fluid

A

the mass of the fluid displaced exerts a force equal to its weight agaisnt the submerged object

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

buoyancy

A

Fbuoy = ρfluid Vfluid displaced g = ρfluid Vsubmerged g

One way to conceptualize the buoyance form is that it is the force of the liquid. Trying to return to the space from which it was displaced. That was trying to push the object up and out of the water.

14
Q

float VS sink

A

An object will float if its average density is less than the average density of the fluid it is immersed in. It will sink if its average density is greater than that of the fluid.

15
Q

cohesion

A

It occurs between molecules with the same properties. It is the attractive force that a molecule of liquid fuel stores other molecules of the same liquid. This established the incision in the plane of the surface of the water. When there is an indentation on the surface, then the cohesion could lead to a net upward force.

16
Q

adhesion

A

Force that a molecule of the liquid fuel stored the molecules of some other substance. When liquids are placed in containers and meniscus or curved surface in which the liquid curls up the side of the container. A small amount will form when the adhesive forces are graded in the cohesive forces.

17
Q

Surface tension.

A

Causes the liquid to form a thin but strong layer like a “skin” and the liquid surface.

17
Q

Backwards Meniscus.

A

Occurs when the cohesive forces are greater than the adhesive forces

18
Q

Laminar flow.

A

It is smooth and orderly. In his, often modelled as layers of fluid that flow parallel to each other.

18
Q

Poiseuille’s law.

A

Q = πr^4 ΔP / 8 η L

Q = flow rate
r = radius of the tube
ΔP = pressure gradient
η = viscosity
L = lenght of the pipe

Note that the relationship between the radius and pressure gradient is inverse exponential to the 4th power. Even a very slight change in the radius of a tube has significant effect on the pressure gradient.

19
Q

viscosity (η)

A

Increase viscosity of a fluid increases its viscous drag, which is a nonconservative form that is innocuous to irresistible. Low viscosity means they flow easily.

19
Q

flow rate is constant for a closed system and is independent of changes in cross=sectional area

A

Q = v1 A1 = v2 A2

Q = flow rate
v1 and v2 = linear speeds
A1 and A2 = areas

This is the continuity equation and it tells us the fluid will flow more quickly through narrow passages and move slowly through wider ones.

20
Q

streamlisnes

A

Indicates the pathway followed by tiny fluid elements as they move.

20
Q

turbulent flow

A

rough and disorderly. Eddies which are swirls of fluid in the downstream side of an obstacle.

21
Q

bernoulli’s equation

A

P1 + 1/2 ρ v1^2 + ρg h1 = P2 + 1/2 ρv2^{2} + ρg h2

ρ = fluid density
g = acceleration due to gravity
P_{1} = pressure at elevation 1
v_{1} = velocity at elevation 1
h_{1} = height of elevation 1
P_{2} = pressure at elevation 2
v_{2} = velocity at elevation 2
h_{2} = height at elevation 2

21
Q

Bernoulli’s equation explained

A

Expression of conservation of energy for a flowing fluid. This equation states that the sum of the static pressure in the dynamic pressure will be constant between any two points in a closed system.

22
Q

Venturi effect.

A

For a horizontal flow there is an inverse relationship between pressure and speed, and in a closed system there is a direct relationship between cross-sectional area and pressure exerted on the walls of the tube.

22
Q

Fluid in Physiology.

A

The circulatory system behaves as a closed system with non constant flow.

Resistance decreases as the total cross-sectional area increases. Arterial circulation is primarily motivated by the heart. Venous Circulation has three times the volume of arterial circulation and is motivated by the skeletal musculature and expansion of the heart. Inspiration and expiration create a pressure gradient not only for the respiratory system, but for the circulatory system as well.