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AOS 101. Atmospheric Forces. April 8/10. Vector. Vectors have a magnitude and a direction (e.g. winds) Can be broken down into components: |a| = magnitude of vector a. v. u. Vectors can be added:. A + B = C. B. Resultant vector. Components can also be added: A = 3 i + 1 j
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AOS 101 Atmospheric Forces April 8/10
Vector • Vectors have a magnitude and a direction (e.g. winds) • Can be broken down into components: • |a| = magnitude of vector a v u
Vectors can be added: A+B=C B Resultant vector Components can also be added: A = 3i + 1j B = 3i + 4j C = A + B = (3+3)i + (1+4)j = 6i +5j A
Newton’s Second Law • Forces and accelerations are also vectors having directions and magnitudes. • Newton’s second law: • An object will accelerate in the same direction as the force acts on it
However, several forces will typically act on an object simultaneously • Hence, an object will accelerate in the direction of the net force where Fnet = F1 + F2 + F3 + F4 + ..., the sum of all force vectors.
Zero Net Force • Sometimes all forces will completely cancel out and Fnet = 0 • In this situation, the forces are said to be balanced • If there is zero net force, there is zero acceleration meaning: • If the object is at rest, it will stay at rest • If the object is moving, it will continue to move at the same velocity.
BOOK Free Body Diagram • Draw vectors representing each force mg mg Fr BOOK mg mg
Four Forces in the Atmosphere • Pressure Gradient Force • Coriolis Force • Friction (surface) • Centrifugal (highly curved)
1. Pressure Gradient (PG) Force • Always points from high to low • Always perpendicular to pressure contours (isobars) LOW FPG P1 = 1000 hPa P2 = 1004 hPa HIGH
ρa = density of air ~ 1 kg/m3 • |P2 – P1| = difference in pressure (abs. value) • D = distance between observations • Larger pressure difference, shorter distance (i.e. isobars closer together) results in larger force
2. Coriolis (cor) Force • Apparent force due to earth’s rotation • Always perpendicular and to the right (in the N.H.) of the wind Fcor
|V| = magnitude of wind (in m/s) • f = 1.4 x 10-4 * sin(latitude) • Midlatitudes: f ~ 1.0 x 10-4 • An increase in wind speed results in a stronger force • In the absence of friction, will oppose PG force
Geostrophic Balence • PG and Coriolis forces balance: • How does this happen? • Wind will increase until magnitude of Coriolis force (fv) is the same as PG force.
Thus, balanced wind speed can be found by: • When geostrophically balenced, winds will be parallel to isobars, with low pressure to the left LOW FPG P1 = 1000 hPa P2 = 1004 hPa HIGH Fcor
3. Frictional (Fr) Force • Due to roughness of the earth’s surface • Only important within 1-2 km of the ground (planetary boundary layer) • Negligible in free atmosphere (above 2 km) • Always in the opposite direction of the wind FFr
LOW FPG P1 = 1000 hPa • At the ground, winds will not be parallel to isobars • Winds will cross isobars towards lower pressure FFr P2 = 1004 hPa Fcor HIGH
4. Centrifugal (cen) Force • Outward “force” due to inertia while curving • Always perpendicular to wind vector, outward from circle L Fcen
|V| = magnitude of wind (in m/s) • R = radius of circulation • Only important for strong winds (e.g. the jet stream) that are highly curved.
Two possibilities Fcen FPG Fcen Fcor Fcor FPG H L
Summary • Pressure Gradient • ALWAYS perpendicular to isobars • ALWAYS points from high to low pressure • Coriolis • ALWAYS perpendicular to wind vector • ALWAYS (in the NH) to the right of wind vector • Friction • ALWAYS in opposite direction of wind vector • Only important with 1-2 km of the ground • Centrifugal • ALWAYS points outward from circle, perpendicular to wind vector • Only important for strong winds and highly curved flows
Application to Weather Maps • Weather maps will typically be on an isobaric surface (constant pressure sfc.) • Height of the surface plotted instead of pressure • “height” features are same as “pressure” features • High height area is same as high pressure area • Low height area is same as low pressure area • PGF acts from high heights to low heights