HABYTIME MINI LECTURE 26: QUADRANTING A JET STREAK
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
METEOROLOGIST JEFF HABY
A jet streak is a region of high speed wind within the jet stream (subtropical jet stream / polar jet stream). The best charts to analyze
jet streaks within the jet stream are the 300-mb chart in the winter and the 200-mb chart in the summer. The jet core is the segment of
the highest speed wind within a jet streak. This is typically toward the center of the jet streak. The diagram below shows a drawing
of a jet streak with a jet core of 140 knot winds at the center. The jet core occurs where the pressure gradient force is highest. Where
the height contours are closest together is generally where the highest wind speeds will be located. The diagram below shows heights
contours and the position of the jet core where the height contours are closest together. A few wind vectors near the jet core are
also drawn in to show the direction of the wind through the jet streak.
Weather forecasters will quadrant a jet streak in the following two ways below. The jet streak is divided into 4 sections with the middle
of the jet streak being where the strongest wind is located. The entire jet streak does not move as fast as the winds that are flowing
through the jet streak. For example, the entire jet streak may be moving at 25 knots while the maximum jet streak winds are 120 knots. Thus,
wind moves through the jet streak. The 4 sectors of a jet streak given below are the left rear quadrant, the right rear quadrant, the left
front quadrant and the right front quadrant. A jet streak can also be divided into two regions called the entrance sector and the exit
sector. Wind enters the jet streak within the entrance sector (which are the left and right rear quadrants) and exits within the exit
sector (which are the left and right front quadrants).
The purpose of quadranting a jet streak is to find where the regions of lifting and sinking air are located. Upper level divergence
contributes to lifting air while upper level convergence contributes to sinking air. When reading about “upper level divergence” in
a forecast discussion, jet streak divergence is one contributing factor to upper level divergence and thus rising air. Rising air
enhances precipitation chances and storm chances. The regions of upper level divergence (rising air) are in the Right Rear quadrant
and the Left Front quadrant while the regions of upper level convergence (sinking air) are in the Left Rear and Right Front quadrant. The
diagram below shows the quadrants of a jet streak and a path that a parcel of air can take as it moves through the jet streak. Notice
the parcel of air shifts from the RR and into the LR quadrant before shifting from the LF and into the RF quadrant. The significance
of this will be explained next since this is what causes the divergence and convergence quadrants within a jet streak.
A parcel of air enters the jet streak in the entrance sector at position 1 for example in the diagram below. As the parcel moves toward
the jet core, the parcel is accelerating due to the higher pressure gradient. The Pressure Gradient Force (PGF) acts very quickly on
the parcel of air but the Coriolis (f) acts slowly. Thus, the PGF overpowers the Coriolis force and the parcel deviates more in the
direction of the PGF (position 2). A longer vector of PGF at position 2 as compared to the Coriolis is used to indicate the PGF is
stronger than the Coriolis. Between position 2 and position 3, the Coriolis is coming into adjustment with the PGF and the parcel
deviation of motion stops. However, when the parcel starts coming out of the jet core at position 3 and the wind speeds slow (and
thus PGF weakens and the parcel decelerates), the PGF rapidly reduces while the Coriolis is slow to adjust. The temporarily stronger
Coriolis causes the parcel to deviate toward the direction of the stronger Coriolis (at position 4). The Coriolis adjustment completes
between position 4 and position 5. At position 5, the parcel is once again in balance between the PGF and Coriolis forces. In the right
rear quadrant (from position 1 to 2), there is an evacuation of mass as more air mass piles into the left rear quadrant. This deficit
of air helps pull up air from below (thus rising air in right rear quadrant). In the left front quadrant (from position 3 to 4), there
is also an evacuation of mass more air mass piles into the right front quadrant. This deficit of air helps pull up air from below
(thus rising air in the left front quadrant).
|
|
|