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The Coriolis Force QMUL Interview 7th July 2016 Introduction You all know Newton’s 2nd law, F = ma, but this is only valid in this form in an inertial frame of reference Inertial frame = at rest or in uniform motion In a non-inertial frame, such as a rotating body, it needs to be modified by introducing so-called fictitious or apparent forces Non-inertial = accelerating w.r.t inertial frame ^ | = ma Feff = |F – mω2r ^ur – 2mωvsinθu θ Fcentrifugal FCoriolis You’re all familiar with the first term: the centrifugal force Objects in a rotating frame feel an outwards push, perp. to axis This push has no physical origin but is a consequence of inertia 2 Coriolis force The Coriolis force is another apparent force that only acts when objects are moving in a rotating frame Appears to deviate objects to right (left) for anti-clockwise (clockwise) rotation E.g. a ball thrown on a roundabout In inertial frame ball travels straight In rotating frame introduce Coriolis force to explain deviation ω Coriolis force = 2mωvsinθu^ θ Only acts on objects moving in rotating frame Points perpendicular to velocity, v, & ω vectors Proportional to velocity perpendicular to axis FCoriolis v ω 3 Coriolis force The Coriolis force is another apparent force that only acts when objects are moving in a rotating frame Appears to deviate objects to right (left) for anti-clockwise (clockwise) rotation Inertial frame E.g. a ball thrown on a roundabout In inertial frame ball travels straight In rotating frame introduce Coriolis force to explain deviation Coriolis force = 2mωvsinθu^ θ Rotating frame Only acts on objects moving in rotating frame Points perpendicular to velocity, v, & ω vectors Proportional to velocity perpendicular to axis 4 Coriolis effect on Earth In N hemisphere, earth rotates anti-clockwise Object going E (in to paper) has a larger rotational velocity Horizontal component of the centrifugal (CF) and gravity (g) forces balance for object at rest ω gh Increases horizontal component of CF deviated S (to right) due to net Coriolis force ω CFv gh CFv CF CF g gv CFh g gv CFh Coriolis Force Zero at equator where CF is vertical and max at poles where it is horizontal 5 Coriolis effect on Earth In N hemisphere, earth rotates anti-clockwise Object going W (out of paper) has a smaller rotational velocity Horizontal component of the centrifugal (CF) and gravity (g) forces balance for object at rest ω gh Decreases horizontal component of CF deviated N (to right) due to net Coriolis force ω CFv gh CFv CF CF g gv CFh g gv Opposite in southern hemisphere as rotates clockwise to left CFh Coriolis Force 6 Coriolis effect on Earth In N hemisphere, earth rotates anti-clockwise Object going N, also moves E seen in inertial frame due to earth’s rotation Horizontal component of the centrifugal (CF) and gravity (g) forces balance for object at rest ω gh CFv CF g gv CFh CFh points out from centre of net rotation direction has changed giving component to east (right) Coriolis Force CFh CF hNS ω CFhEW gh Opposite in southern hemisphere as rotates clockwise to left 7 Coriolis effect on Earth In N hemisphere, earth rotates anti-clockwise Object going S, also moves E seen in inertial frame due to earth’s rotation Horizontal component of the centrifugal (CF) and gravity (g) forces balance for object at rest ω gh CFh points out from centre of net rotation direction has changed giving component to west (right) CFhNS CFv CFhWE Coriolis Force CF g gv CFh CFh ω gh Opposite in southern hemisphere as rotates clockwise to left 8 The myth: water down a plug People believe that the Coriolis force causes water to spin the opposite way down the plug in northern/southern hemispheres This is a myth: it can spin either way and the Coriolis force is way to weak to affect it under normal situations Consider unit mass (m) of water moving at v=0.1m/s in a sink of radius r=0.5m at θ=78o north FCorilois = 2 m v ω sinθ = 2 x 1kg x 0.1m/s x 2π/(24*60*60) rad/s x sin(78o) ≈ 1.4x10-5 N Fcent = mv2/r = 1kg x (0.1 m/s)2 / 0.5 m ≈ 2x10-2 N = 1400 x FCoriolis v = 0.1 m/s r = 0.5 m 9 Cyclones: a real Corilois effect Air wants to move straight from high to low pressure due to gradient force But, as we have shown, the Coriolis force acts to deviate it to the right (left) in northern (southern) hemisphere causing it to spiral Northern Hemisphere H Southern Hemisphere H L L = Pressure gradient force = Coriolis force Net result is the formation of cyclones that rotate anti-clockwise (clockwise) in northern (southern) hemisphere 10 Cyclones: a real Corilois effect Air wants to move straight from high to low pressure due to gradient force But, as we have shown, the Coriolis force acts to deviate it to the right (left) in northern (southern) hemisphere causing it to spiral Northern Hemisphere H Southern Hemisphere H L L Net result is the formation of cyclones that rotate anti-clockwise (clockwise) in northern (southern) hemisphere 11 Summary The Coriolis force is an apparent force, which explains the deviation of moving objects in a rotating frame of reference It deviates objects to the right (left) for anti-clockwise (clockwise) rotation The deviation vanishes at the equator and reaches its maximum at the poles It leads to the formation of cyclones which spin in opposite directions in the northern and southern hemispheres It is not responsible for water rotating in opposite directions as it goes down the plug hole since it is much too weak on this scale 12 Derivation Velocity in inertial frame = v in rotating frame + v due to rotation ω = constant angular velocity r = position in rotating frame Since nothing special about r, take it out to get an operator Calculate acceleration in inertial frame Apply to Newton’s 2nd law: FI = maI 13