precipitation systems in midlatitude Flashcards

1
Q

Precipitation may be classified as

A

convective and stratiform

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2
Q

Precipitation characterized by

A

turbulent vertical fluxes of heat and momentum

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3
Q

Precipitation characterized by turbulent vertical fluxes of heat and momentum such as

A

showers and thunderstorms are convective.

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4
Q

Convective precipitation regions are relatively …………….. and precipitation from them tend to be

A

Narrow intermittent and intense

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5
Q

Convective precipitation systems may be

A

hydrostatic (e.g., as in extratropical cyclones and frontal zones) or non-hydrostatic (e.g., showers and thunderstorms)

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6
Q

Stratiform Precipitation Systems these systems are characterized by

A

relatively gentle vertical fluxes of heat and momentum

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7
Q

Stratiform Precipitation Systems This type of precipitation is often found

A

poleward of warm fronts in a broad region of warm advection.

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8
Q

Stratiform precipitation systems are always

A

hydrostatic

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9
Q

Stratiform precipitation regions are relatively

A

wide, and precipitation from them tends to be steady.

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10
Q

Cumulus Convection:

A

Convection that results in the formation of cumulus clouds (or sometimes thunderstorms) with a flat base and rounded puffy top.

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11
Q

Convection refers primarily to atmospheric motions that

A

transfer heat, moisture and momentum in the vertical direction.

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12
Q

As the surface warms, it

A

heats the overlying air, which gradually becomes less dense than the surrounding air and begins to rise.

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13
Q

thermal

A

The bubble of relatively warm air that rises upward from the surface

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14
Q

Convective clouds (such as ………………..) are usually referred as

A

cumulonimbus deep, if their depth is a substantial fraction of the depth of the troposphere.

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15
Q

Deep cumulus convection may be “based” either in

A

the boundary layer or aloft.

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16
Q

A parcel of air that is warmer than its environment will

A

A parcel of air that is warmer than its environment will

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17
Q

As an unsaturated air parcel located near the surface rises, its temperature will

A

follow a dry adiabat

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18
Q

lifted condensation level (LCL)

A

Where the dry adiabat crosses the saturation mixing ratio line, the air becomes saturated and condensation commences.

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19
Q

when does level of free convection LFC occure

A

If there is no convective inhibition blocking the ascent of the rising air parcel, the lifted condensation level becomes the level of free convection, or LFC.

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20
Q

Level of Free Convection (LFC):

A

The height at which a lifted parcel of air would first become warmer (less dense) than the surrounding air.

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21
Q

As the parcel continues to rise, it follows a

A

moist adiabat

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22
Q

As the parcel continues to rise, it follows a moist adiabat. Once the parcel reaches the ……… and becomes …………………………………

A

LFC and becomes less dense than the surrounding air

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23
Q

Once the parcel reaches the LFC and becomes less dense than the surrounding air, it continues to

A

rise freely until it becomes as cool (as dense) as the surrounding air.

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24
Q

Once the parcel reaches the LFC and becomes less dense than the surrounding air, it continues to rise freely until it becomes as cool (as dense) as the surrounding air. This upper level is the

A

Equilibrium Level (EL).

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25
Q

CAPE stands for

A

Convective Available Potential Energy

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26
Q

An estimate of buoyant energy can be computed by

A

determining the temperature difference between the ascent path and the environment at all levels from the LFC up through the equilibrium level.

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27
Q

the positive area between two curves equals

A

When we sum up all of these temperature differences, we arrive at a number equal to

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28
Q

…………………………………………. is CAPE, which is given by:

A

The quantitative measure of this positive area

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29
Q

CAPE is measured in units of

A

J/kg

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30
Q

The environmental CAPE for convective storms is often in the range of

A

1000-2000 J/kg

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31
Q

The environmental CAPE for convective storms is often in the range of 1000-2000 J/kg. However, values higher than ……… sometimes occure

A

5000 J/kg

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32
Q

Wmax

A

Maximum Potential Speed of the Updraft

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33
Q

The maximum potential speed of the updraft (………………….), or Wmax, can be directly obtained from ………….. as shown by this equation:

A

maximum vertical velocity

CAPE

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34
Q

the wmax equation is derived from

A

from a simplification of the vertical momentum equation by ignoring mixing, water loading, and pressure effects

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35
Q

In reality, these simplifications mean that Wmax often

A

overestimates the actual updraft value by a factor of 2.

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36
Q

For example, using this equation, a relatively high CAPE of 2000 J/kg would indicate a Wmax of

A

63.2 m/s

37
Q

For example, using this equation, a relatively high CAPE of 2000 J/kg would indicate a Wmax of 63.2 m/s, or, allowing for the overestimate, a more probable

A

Wmax of 31.6 m/s, or about 65 knots.

38
Q

Capping inversion acts as a

A

lid

39
Q

Capping inversion acts as a lid, which can prevent

A

near-surface parcels from reaching their level of free convection (LFC).

40
Q

CIN can prevent

A

storms from forming, even with high instability aloft.

41
Q

In the presence of a capping inversion, some additional mechanism (………………………………………………) is required to initiate convection.

A

like heating, moistening and synoptic scale lifting

42
Q

convective inhibition (CIN)

A

The work needed to lift an air parcel from rest at the surface to the LFC

43
Q

convective inhibition (CIN) it is the

A

It is the negative of the area enclosed by the environmental temperature profile and the dry and moist adiabats connecting the surface to the LFC on skew-T.

44
Q

For CIN > …………………deep convection is unlikely to occur in the absence of external forcing

A

100 J kg-1

45
Q

For CIN > 100 J kg-1, deep convection is unlikely to occur in the absence of external forcing, such as might be provided by

A

daytime heating or the approach of a strong front.

46
Q

The basic building block of the convective systems is the

A

thunderstorm cell (or deep convection)

47
Q

Deep convection takes in to various forms of convective systems:

A

a. single convective cells (some thunderstorms) consisting of a single updraft and downdraft – form under conditions of weak vertical wind shear.
b. multi cell storms (e.g., squall lines) made up of organized groups or sequences of convective cells – that develop under conditions of strong vertical wind shear and
c. supercells with rotating updrafts formed from the multicell storms mesoscale convective systems (MCS) - bands or zones of clouds and precipitation on a scale of 100 km or larger in at least one direction that are generated by interacting convective cells.

48
Q

Both multi- and supercell storms are capable of producing

A

hail and strong winds

49
Q

Most damaging tornadoes are associated with

A

supercell storms

50
Q

The necessary conditions for the occurrence of deep convection are:

A
  • the existence of a conditionally unstable lapse rate Γw < Γ ≤ Γd
  • substantial boundary-layer moisture, and
  • low level convergence (or lifting) sufficient to release the instability.
51
Q

Convection feeds on

A

the potential energy inherent in the temperature and moisture stratification.

52
Q

The so-called convective available potential energy (CAPE), (in J kg-1) of a reference air parcel is given by:

A
53
Q

Tv and Tv​ stand for

A

virtual temp of the parcel and environment

54
Q

The reference air parcel used in computing the CAPE may be an air parcel at

A

the Earth’s surface

55
Q

The reference air parcel used in computing the CAPE may be an air parcel at the Earth’s surface or it may be chosen to be representative of the

A

mean temperature and humidity of the air within the boundary layer.

56
Q

The reference air parcel used in computing the CAPE may be

A

an air parcel at the Earth’s surface or it may be chosen to be representative of the mean temperature and humidity of the air within the boundary layer.

57
Q

Convective storms often form in an environment in which

A

the vertical wind shear vector (do V/do z) is dominated by the increase in scalar wind speed V with height.

58
Q

The strength of the shear affects the ……………………………… within the storm

A

vertical tilt of the updrafts and downdrafts

59
Q

The strength of the shear affects the vertical tilt of the updrafts and downdrafts within the storm:

A
  • weak shear favors a structure in which the downdraft ultimately isolates the updraft from its supply of low level moisture leading to the storm’s demise,
  • strong shear favors a tilted structure with a relationship between updraft and downdraft, resulting in more intense, longer lived storms capable of producing hail and strong winds
60
Q

Changes in wind direction with height also play an important role in the

A

dynamics of convective storms

61
Q

In the presence of vertical wind shear

A

air possesses vorticity that can be visualized as a rolling motion about a horizontal axis.

62
Q

explain the rotation of the convective systems

A

When boundary layer air is drawn into the updraft of a convective storm, the vorticity about a horizontal axis may be tilted so that it is transformed into vorticity about a vertical axis

63
Q

When boundary layer air is drawn into the updraft of a convective storm, the vorticity about a horizontal axis may be tilted so that it is transformed into vorticity about a vertical axis

Note how

A

ounterclockwise vorticity about the x axis (as viewed looking in the positive direction along the axis) is tilted into counterclockwise vorticity about the z axis, as viewed from above.

64
Q

In the presence of vertical wind shear, air possesses vorticity that can be visualized as a rolling motion about a horizontal axis.

This is a powerful mechanism for

A

imparting rotation to convective storms

65
Q

When the environmental vertical shear is relatively weak and only the CAPE is dynamically significant, ………….. occure

A

ordinary cells

66
Q

When the low level vertical shear is larger and the CAPE is not too small a …………………….. storm can form

A

multicell (succession of ordinary cells)

67
Q

If CAPE is high and the vertical shear is strong,

A

a supercell forms

68
Q

Since storm behavior is a function of

A

both shear and updraft strength

69
Q

Since storm behavior is a function of both shear and updraft strength, and maximum updraft strength is a function of

A

CAPE

70
Q
A
71
Q

Since storm behavior is a function of both shear and updraft strength, and maximum updraft strength is a function of CAPE, it is useful to consider an

A

empirical quantity, the bulk Richardson’s number (R).

72
Q

The bulk Richardson’s number is

A

ratio of CAPE to a quantity proportional to the square of the mean vertical shear integrated over height (S2) as an indicator of storm type

73
Q

what is (R)’s formula

A
74
Q

u6000 and u500​ are

A

the pressure-weighted mean-vector wind speeds in the

lowest 6 km and 500 m, respectively.

75
Q

Observational and numerical work suggests that ordinary cells form exclusively when R is

A

greater than 30-40

76
Q

When R is …………………….., supercells or long-lived multicell storms develop.

A

smaller (<40)

77
Q

If R is ………………, while both ………………………………, less severe long-lived cells are possible.

A

less than 30-40

the CAPE and the vertical shear are small

78
Q

Thunderstorms (single cell storms)

These are

A

the small isolated cumulonimbus clouds produced by local convection in an unstable airmass rather than by fronts or instability lines.

79
Q

Thunderstorms (single cell storms)

These systems generally develop

A

just one main precipitation shower (a single cell storm), and the pressure field is entirely determined by buoyancy of the warm updraft.

80
Q

Thunderstorms (single cell storms)

Only about ………of the water vapor ………………….in the updraft actually reaches the ground in the form of precipitation.

A

20%

condensed

81
Q

Thunderstorms (single cell storms)

Only about 20% of the water vapor condensed in the updraft actually reaches the ground in the form of precipitation.

The remainder

A

evaporates either in the downdraft or into the ambient air.

82
Q

self-destruct mechanism:

A

The single-cell thunderstorm is short lived and rarely produces destructive winds or hail because it contains a built in self-destruct mechanism namely, the downdraft circulation.

83
Q

In the absence of vertical wind shear, the precipitation produced in

A

the downdraft destroys the buoyant updrafts that feed it.

84
Q

Multicell storms are characterized by

A

a succession of cells, each evolving through its own cycle as in a single cell storm and promoting the development of new cells.

85
Q

A prominent feature of many convective storms is the gust front, where

A

warm, moist boundary-layer air is lifted by the leading edge of the evaporatively cooled air diverging from the base of the downdraft.

86
Q

New cells tend to form along the

A

advancing gust front

87
Q

New cells tend to form along the advancing gust front, sustaining​ ………………. while

A

the multicell storm

older cells die out as they fall behind the gust front and become surrounded by cooler, denser downdraft air.

88
Q

From the perspective of a ground-based observer, the passage of this storm would be marked by

A

thickening high overcast, followed by the approach of a much lower, darker cloud base, followed by an abrupt wind shift and temperature drop that marks the arrival of the gust front.

89
Q

Multicell storms

Heavy precipitation would not begin until

A

a few minutes after the passage of the gust front and might include hail.