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                                                                                               11.3 Precipitation  363
                                         of cyclonic disturbances over the North American continent as well as the rotary or cyclonic
                                         motion of horizontal air currents converging at points of low pressure.
                                             In the continuous planetary circulation of the atmosphere between equator and poles,
                                         warm, moisture-laden, tropical air masses travel poleward, are cooled, and precipitate
                                         their moisture along the way. Ultimately, they are transformed into cold, dry, polar air. A
                                         return movement drives polar air masses toward the equator, and heavy precipitation
                                         results when tropical and polar air masses collide. The light, warm, tropical air cools and
                                         precipitates its moisture as it is forced up and over the heavy polar air. Collisions between
                                         tropical and polar air masses normally account for the protracted general rainfalls and
                                         accompanying floods of the central and eastern United States. When, for unknown rea-
                                         sons, polar air does not return toward the equator in the usual manner, serious droughts
                                         can occur.
                                             The Bjerkness cyclone model shown in Fig. 11.2 identifies the movements of warm
                                         and cold air masses in the usual type of cyclonic storm. Precipitation is indicated on the
                                         plan by shading. The cross-sections suggest the manner in which warm air is forced up-
                                         ward by cold air. At the cold front, the colder air wedges itself below the mass of warm air
                                         and usually advances southward and eastward in the Northern Hemisphere. At the warm
                                         front, the warm air is forced to climb over the retreating wedge of cold air and usually ad-
                                         vances northward and eastward in the Northern Hemisphere. When there is little or no
                                         movement at the boundary of the air masses, the front is called stationary. When the cold
                                         front overtakes the warm front and lifts all the warmer air above the surface, the front is
                                         said to be occluded.

                                                                          Warm air

                                                        Cold air                            Cold air






                                                  A                                                     A

                                                                                             Cold air
                                                   Cold air




                                                                    Warm air  Warm front
                                                  B                                                     B
                                                          Cold front





                                                                     Warm air
                                             Cold air                                                    6 miles



                                                          40    125               200      300 miles
                                             Figure 11.2 Bjerkness Cyclone Model
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