Chapter 1 Flashcards

1
Q

Circulation and vorticity are

A

the two primary measures of rotation in a fluid

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2
Q

Circulation is a

A
  • scalar integral quantity
  • macroscopic measure of rotation for a finite area of the fluid
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3
Q

Vorticity is a

A
  • vector field
  • microscopic measure of the rotation at any point in the fluid
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4
Q

draw an example of circulation and vorticity

A
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5
Q

What is the difference between macroscopic and microscopic

A
  • Macroscopic:
    • Large scale
    • rotation of entire fluid –> circulation
  • Microscopic:
    • Very Small
    • How individual particles rotate “any point within the fluid”
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6
Q

barotropic fluid

A

characterised by the absence of horizontal temperature gradients completely.

No horizontal gradient –> temperature is constant “Isotherm”

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7
Q

A barotropic fluid is one in which

A

the surfaces of constant pressure (p1, p2 …) and constant density (or specific volume) are parallel.

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8
Q

Specific volume (a):

A

volume of a unit mass of air

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9
Q

density (p):

A

mass/volume = 1/volume

specific volume = 1/p (when p constant volume is constant)

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10
Q

In a barotropic fluid, …………………..is a function of ………………and……………………………………………………

A

density

pressure only

density is constant along a constant pressure surface.

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11
Q

P1 ​stands for

A

Isotere (specific volume)

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12
Q

a1​ stands for

A

Pressure uniform

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13
Q

ideal gas law:

A
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14
Q

From ideal gas law:

A

If P is constant p is constant –> constant ratio = constant

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15
Q

The law implies that

A

for a barotropic atmosphere, temperature is constant on a constant pressure surface.

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16
Q

for a barotropic atmosphere, temperature is constant on a constant pressure surface.

Therefore, in a barotropic fluid,

A

surfaces of constant pressure, constant density and constant temperature all are parallel.

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17
Q

Summary of barotropic fluid

A

No change in temperature and pressure –> no circulation due to these factors but circulation may develop due to other factors

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18
Q

baroclinic fluid

A

characterized by the presence of horizontal temperature variations.

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19
Q

A baroclinic fluid is characterized by the presence of horizontal temperature variations.

In such a fluid,

A

density is not a function of pressure alone and density variations occur due to horizontal temperature variations. Ex: Land and sea breeze.

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20
Q

Explain the figure

A

the isobars slope upwards towards the warm, while the isosteres slope upward over the cold.

Therefore, in a baroclinic fluid, the surfaces of constant pressure and constant specific volume intersect each other, forming quadrilaterals known as ‘solenoids’.

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21
Q

Fig. also shows that the solenoids give

A

rise to direct circulation (warm air rises and cold air sinks).

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22
Q

circulation is a

A

scalar quantity

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23
Q

Circulation

A

expresses the macroscopic rotational tendency of a finite area of a fluid.

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24
Q

The circulation, C, around a given closed curve in a fluid is

A

the integral around the curve of the components of the velocities along the curve

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25
Circulation equation:
26
Draw a figure that better represent the circulation equation
27
C, a measure of
the rotation of the fluid
28
C, a measure of the rotation of the fluid is:
* positive (C \> 0) for cyclonic circulation and * negative (C \< 0) for anticyclonic circulation
29
Circulation has dimensions
30
If dx, dy, dz are components of ......, then
dl
31
Circulation around a closed loop is, simply the
integral of the tangential velocities around the loop.
32
* Circulation around a closed loop is, simply the integral of the tangential velocities around the loop. * Hence, the mean tangential velocity around
the loop can be obtained from circulation (C) as follows: where r is the radius of the circular loop
33
The Circulation theorem It gives an
expression for the individual rate of change of the circulation, over a closed chain of fluid particles.
34
what are the terms in the following circulation theorem
35
What is the simplified version of the solenoidal term
36
Coriolis term
37
What does F represents in the Coriolis term
represents the area enclosed by the projection of the chosen closed circuit on the equatorial plane.
38
The coriolis term states that if a material surface
expands in time or displaced polewards its projection onto the equatorial plane increases (dF/dt \>0)
39
What is the simplified version of the circulation theorem
40
In a barotropic fluid, since density is a function of pressure only, we can write the solenoidal term as:
41
Therefore, for a barotropic fluid, the circulation theorem becomes:
42
When a material surface ............................... or .................................
expands in time or displaced polewards c decreases --\> cyclonic circulation decreases. anticyclonic circulation increases
43
Since in a baroclinic fluid, density is not a function of pressure alone, \_\_\_\_\_\_\_\_\_\_\_\_Therefore, for a baroclinic fluid, the circulation theorem can be written as:
/o (a)(dp)not equal to 0
44
Sea breeze
* During the day the land is heated while the water surface remains relatively cool. * The isosteric surfaces slope downwards towards the warmer land as depicted, causing the wind to blow from the sea toward the land.
45
land breeze
* During night, the opposite situation occurs. * The land surface cools off and the water remains relatively warm so that the wind blows from the land toward the sea.
46
On the small spatial scales of land–sea breezes the rotational (coriolis) effect of the earth
may be disregarded.
47
On the small spatial scales of land–sea breezes the rotational (coriolis) effect of the earth may be disregarded. The observed circulation pattern is then due to
the solenoidal effect
48
The observed circulation pattern is then solely due to the solenoidal effect and the circulation theorem can be written as:
49
a counter clockwise (cyclonic) circulation will be developed with
rising motion over warmer land and sinking motion over colder ocean.
50
the two primary measures of rotation in a fluid
Circulation and vorticity
51
* scalar integral quantity * macroscopic measure of rotation for a finite area of the fluid
Circulation
52
* vector field * microscopic measure of the rotation at any point in the fluid
Vorticity
53
A resembles
Circulation
54
B resembles
Vorticity
55
characterised by the absence of horizontal temperature gradients completely
barotropic fluid
56
the surfaces of constant pressure (p1, p2 ...) and constant density (or specific volume) are parallel in
A barotropic fluid
57
volume of a unit mass of air
Specific volume (a)
58
characterized by the presence of horizontal temperature variations.
baroclinic fluid
59
expresses the macroscopic rotational tendency of a finite area of a fluid.
Circulation
60
the integral around the curve of the components of the velocities along the curve
The circulation, C,
61
integral of the tangential velocities around the loop.
Circulation around a closed loop
62
expression for the individual rate of change of the circulation, over a closed chain of fluid particles.
The circulation theorem
63
represents the area enclosed by the projection of the chosen closed circuit on the equatorial plane
What does F represents in the Coriolis term
64
* During the day the land is heated while the water surface remains relatively cool. * The isosteric surfaces slope downwards towards the warmer land as depicted, causing the wind to blow from the sea toward the land.
Sea breeze
65
* During night, the opposite situation occurs. * The land surface cools off and the water remains relatively warm so that the wind blows from the land toward the sea.
land breeze