1.
·
First Law:
An
object at rest will remain at rest, or remains moving in a straight
line,
unless acted upon by a force(s).
·
Second Law:
Acceleration of an object is proportional to the net force
applied.
Force is proportional to
acceleration
F prop. a
Force equals mass x acceleration
F = m x a
·
Note that if an object is
changing direction (e.g.,
wind blowing around a low pressure system) then:
·
A force must be acting on
it
·
It must be accelerating
2.
Four Forces
Affecting the Winds
·
Pressure gradient force (PGF)
(pg. 150)
·
See
Fig. 6.9, 6.10, 6.11
·
Coriolis force (effect) (pg. 151)
·
Arises
from fact that earth is a
rotating frame of reference, not stationary (Fig. 6.13, 6.14, 6.15)
·
To
be significant, the air must be
MOVING; it must NOT be on the equator (0°
latitude);
and it must be LARGE SCALE.
·
CF
changes wind direction, not wind
speed
·
Net
result: winds deflected to the
RIGHT in the N.H.
·
For
a cool Coriolis
video
click here.
·
Centripetal force (derived from: center +
towards) found where wind circulates around a Low or High.
It must exist because wind flowing around a
curve (e.g., L or H) is accelerating (
·
Frictional force reduces wind speed due
to
surface roughness such as mountains, forests, etc. (see section 4,
below)
3.
Upper Level
Winds (here FF = 0 and can be
ignored)
·
Wind speed and direction
is due to balance of PGF
(towards L), CF (to right of flow direction) and centripetal force
(towards
center of rotation (see Fig. 6.17, “Net” is due to centripetal force).
·
Geostrophic wind =
straight line motion, parallel to
contour lines
·
Net
result of PGF and CF is a flow that
is parallel to contours, NOT from high-to-low pressure, as one might
have
expected.
·
Low
is on the left.
·
The
stronger the PGF (steeper gradient)
the stronger the wind (Fig. 6.16)
·
Rule
of thumb – surface wind speed =
50% of 500 mb wind speed
·
Gradient wind = curved
path around low/high pressure
centers in upper atmosphere
·
Cyclonic
flow = counterclockwise around
a Low (in N.H.) (Fig. 6.17)
·
Anticyclonic
flow = clockwise around a
High (in N.H.) (Fig. 6.17)
·
Plotting upper level
winds on constant pressure
charts (Fig. 6.18; Figure 2, pg. 149; see also any 500
mb map)
·
Contour
lines on all upper level charts
represent altitude in decimeters (dm) and are spaced every 6 dm. 1 dm = 10 m.
Normal altitudes on a 500 mb chart are about 500 dm (= 5km).
·
Lowest
altitudes correspond to coldest
air and so are found in the north on the map (e.g.,
·
Troughs
= cooler air = mid-latitude
cyclones (pg. 148)
·
Ridges
= warmer air = anticyclones (pg.
148)
·
Meridional
flow = roughly N-S flow
pattern (along the meridian lines)
·
Zonal
flow = roughly E-W flow pattern
(across time zones)
4.
Surface Winds
(now FF must be included)
·
Friction force slows the wind in the
“boundary
layer” (Fig. 6.19).
·
Therefore,
CF (which is proportional to
wind speed) gets weaker.
·
If
CF gets weaker then PGF begins to
dominate and draws air across contour lines and into a Low (or pushes
it away
from a High).
·
Surface
winds cross contours at an
angle of about 30°
and so they “fill in” a Low or they “empty” a High (Fig. 6.20).
·
Contour
lines on all surface
level
charts represent altitude in millibars (mb), and are spaced every 4
mb.
·
Normal
altitudes on a surface chart are
about 1000 mb, and are all corrected to the mean sea-level pressure
(MSLP) (pg.
147, Figure 6.7).
5.
Vertical Winds
·
Convergence and
divergence (Fig. 6.21)
6.
Pressure
Measurement (pg. 144)
·
Standard atmospheric
pressure at sea level = 1013.25
mb (U.S. Standard Atmosphere, pg. 437); typical ranges from about 1050
mb to
880 mb (Figure 6.3)
·
Mercury barometer (Fig.
6.4)
·
Aneroid barometer (Fig.
6.5, 6.6, ASOS)
7.
Wind
Measurement (pg. 160)
·
Wind speed – anemometer
·
Wind direction – wind
vane. Always name a wind after its origin
(e.g.,
sea breeze originates from the sea; North wind originates from the
North).
·
Rawinsonde
(pressure, wind speed, wind direction with altitude; the skew-T diagram)
·
ASOS
(Figure 6.26)
·
Doppler
radar (from WSR 88-D radars, so-called NEXRAD) in cloudy air (pg.
136).