Earth:Topographic Rossby waves

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Short description: Description of waves in the ocean and atmosphere created by bottom irregularities
Animation of propagating Rossby wave.

Topographic Rossby waves are geophysical waves that form due to bottom irregularities. For ocean dynamics, the bottom irregularities are on the ocean floor such as the mid-ocean ridge. For atmospheric dynamics, the other primary branch of geophysical fluid dynamics, the bottom irregularities are found on land, for example in the form of mountains. Topographic Rossby waves are one of two types of geophysical waves named after the meteorologist Carl-Gustaf Rossby. The other type of Rossby waves are called planetary Rossby waves and have a different physical origin. Planetary Rossby waves form due to the changing Coriolis parameter over the earth. Rossby waves are quasi-geostrophic, dispersive waves. This means that not only the Coriolis force and the pressure-gradient force influence the flow, as in geostrophic flow, but also inertia.

Physical derivation

This section describes the mathematically simplest situation where topographic Rossby waves form: a uniform bottom slope.

Shallow water equations

A coordinate system is defined with x in eastward direction, y in northward direction and z as the distance from the earth's surface. The coordinates are measured from a certain reference coordinate on the earth's surface with a reference latitude φ0 and a mean reference layer thickness H0. The derivation begins with the shallow water equations:

ut+uux+vuyf0v=gηxvt+uvx+vvy+f0u=gηyηt+xhu+yhv=0,

where

u is the velocity in the x direction, or zonal velocity
v is the velocity in the y direction, or meridional velocity
h is the local and instantaneous fluid layer thickness
η is the height deviation of the fluid from its mean height
g is the acceleration due to gravity
f0 is the Coriolis parameter at the reference coordinate with f0=2Ωsin(φ0), where Ω is the angular frequency of the Earth and φ0 is the reference latitude

In the equation above, friction (viscous drag and kinematic viscosity) is neglected. Furthermore, a constant Coriolis parameter is assumed ("f-plane approximation"). The first and the second equation of the shallow water equations are respectively called the zonal and meridional momentum equations, and the third equation is the continuity equation. The shallow water equations assume a homogeneous and barotropic fluid.

Linearization

For simplicity, the system is limited by means of a weak and uniform bottom slope that is aligned with the y-axis, which in turn enables a better comparison to the results with planetary Rossby waves. The mean layer thickness H for an undisturbed fluid is then defined as

A layer of homogeneous fluid over a sloping bottom and the attending notation.

H=H0+α0ywithα=|α0|LH01,

where α0 is the slope of bottom, α the topographic parameter and L the horizontal length scale of the motion. The restriction on the topographic parameter guarantees that there is a weak bottom irregularity. The local and instantaneous fluid thickness h can be written as

h(x,y,t)=H0+α0y+η(x,y,t).

Utilizing this expression in the continuity equation of the shallow water equations yields

ηt+(uηx+vηy)+η(ux+vy)+(H0+α0y)(ux+vy)+α0v=0.

The set of equations is made linear to obtain a set of equations that is easier to solve analytically. This is done by assuming a Rossby number Ro (= advection / Coriolis force), which is much smaller than the temporal Rossby number RoT (= inertia / Coriolis force). Furthermore, the length scale of η ΔH is assumed to be much smaller than the thickness of the fluid H. Finally, the condition on the topographic parameter is used and the following set of linear equations is obtained:

utf0v=gηxvt+f0u=gηyηt+H0(ux+vy)+α0v=0.

Quasi-geostrophic approximation

Next, the quasi-geostrophic approximation Ro, RoT 1 is made, such that

u=u¯+u~withu¯=gf0ηyv=v¯+v~withv¯=gf0ηx,

where u¯ and v¯ are the geostrophic flow components and u~ and v~ are the ageostrophic flow components with u~u¯ and v~v¯. Substituting these expressions for u and v in the previously acquired set of equations, yields:

gf02ηyt+u~tf0v~=0gf02ηxt+v~t+f0u~=0ηt+H0(u~x+v~y)+α0gf0ηx+α0v~=0.

Neglecting terms where small component terms (u~,v~,t and α0) are multiplied, the expressions obtained are:

v~=gf022ηytu~=gf022ηxtηt+H0(u~x+v~y)+α0gf0ηx=0.

Substituting the components of the ageostrophic velocity in the continuity equation the following result is obtained:

ηtR2t2η+α0gf0ηx=0,

in which R, the Rossby radius of deformation, is defined as

R=gH0f0.

Dispersion relation of topographic Rossby waves.

Dispersion relation

Taking for η a plane monochromatic wave of the form

η=Acos(kxx+kyyωt+ϕ),

with A the amplitude, kx and ky the wavenumber in x- and y- direction respectively, ω the angular frequency of the wave, and ϕ a phase factor, the following dispersion relation for topographic Rossby waves is obtained:

ω=α0gf0kx1+R2(kx2+ky2).

If there is no bottom slope (α0=0), the expression above yields no waves, but a steady and geostrophic flow. This is the reason why these waves are called topographic Rossby waves.

The maximum frequency of the topographic Rossby waves is

|ω|max=|α0|g2|f0|R,

which is attained for kx=R1 and ky=0. If the forcing creates waves with frequencies above this threshold, no Rossby waves are generated. This situation rarely happens, unless α0 is very small. In all other cases |ω|max exceeds |f0| and the theory breaks down. The reason for this is that the assumed conditions: α1 and RoT 1 are no longer valid. The shallow water equations used as a starting point also allow for other types of waves such as Kelvin waves and inertia-gravity waves (Poincaré waves). However, these do not appear in the obtained results because of the quasi-geostrophic assumption which is used to obtain this result. In wave dynamics this is called filtering.

Phase speed

The phase speed of the waves along the isobaths (lines of equal depth, here the x-direction) is

The phase speed of topographic Rossby waves in x-direction on the northern hemisphere.

cx=ωkx=α0gf011+R2(kx2+ky2),

which means that on the northern hemisphere the waves propagate with the shallow side at their right and on the southern hemisphere with the shallow side at their left. The equation of cx shows that the phase speed varies with wavenumber so the waves are dispersive. The maximum of cx is

|cx|max=α0gf0,

which is the speed of very long waves (kx2+ky20). The phase speed in the y-direction is

cy=ωky=kxkycx,

which means that cy can have any sign. The phase speed is given by

c=ωk=kxkcx,

from which it can be seen that |c||cx| as |k|=kx2+ky2|kx|. This implies that the maximum of |cx| is the maximum of |c|.[1]

Analogy between topographic and planetary Rossby waves

Planetary and topographic Rossby waves are the same in the sense that, if the term α0g/f0 is exchanged for β0R2 in the expressions above, where β0 is the beta-parameter or Rossby parameter, the expression of planetary Rossby waves is obtained. The reason for this similarity is that for the nonlinear shallow water equations for a frictionless, homogeneous flow the potential vorticity q is conserved:

dqdt=0withq=ζ+fh,

with ζ being the relative vorticity, which is twice the rotation speed of fluid elements about the z-axis, and is mathematically defined as

ζ=vxuy,

with ζ>0 an anticlockwise rotation about the z-axis. On a beta-plane and for a linearly sloping bottom in the meridional direction, the potential vorticity becomes

q=f0+β0y+ζH0+α0y+η..

In the derivations above it was assumed that

β0L|f0| : small planetary number β[ζ]|f0| : small Rossby number Roα0LH0 : small topographic parameter αΔHH : linear dynamics,

so

q=f0(1+β0yf0+ζf0)H0(1+α0yH0+ηH0)=f0H0(1+β0yf0+ζf0)(1α0yH0ηH0+),

where a Taylor expansion was used on the denominator and the dots indicate higher order terms. Only keeping the largest terms and neglecting the rest, the following result is obtained:

qf0H0(1+β0yf0+ζf0α0yH0ηH0).

Consequently, the analogy that appears in potential vorticity is that β0/f0 and α0/H0 play the same role in the potential vorticity equation. Rewriting these terms a bit differently, this boils down to the earlier seen β0R2 and α0g/f0, which demonstrates the similarity between planetary and topographic Rossby waves. The equation for potential vorticity shows that planetary and topographic Rossby waves exist because of a background gradient in potential vorticity.

The physical mechanisms that propel topographic waves. Displaced fluid parcels react to their new location by developing either clockwise or counterclockwise vorticity. Intermediate parcels are entrained by neighboring vortices, and the wave progresses forward.

The analogy between planetary and topographic Rossby waves is exploited in laboratory experiments that study geophysical flows to include the beta effect which is the change of the Coriolis parameter over the earth. The water vessels used in those experiments are far too small for the Coriolis parameter to vary significantly. The beta effect can be mimicked to a certain degree in these experiments by using a tank with a sloping bottom. The substitution of the beta effect by a sloping bottom is only valid for a gentle slope, slow fluid motions and in the absence of stratification.[1]

Conceptual explanation

As shown in the last section, Rossby waves are formed because potential vorticity must be conserved. When the surface has a slope, the thickness of the fluid layer h is not constant. The conservation of the potential vorticity forces the relative vorticity ζ or the Coriolis parameter f to change. Since the Coriolis parameter is constant at a given latitude, the relative vorticity must change. In the figure a fluid moves to a shallower environment, where h is smaller, causing the fluid to form a crest. When the height is smaller, the relative vorticity must also be smaller. In the figure, this becomes a negative relative vorticity (on the northern hemisphere a clockwise spin) shown with the rounded arrows. On the southern hemisphere this is an anticlockwise spin, because the Coriolis parameter is negative on the southern hemisphere. If a fluid moves to a deeper environment, the opposite is true. The fluid parcel on the original depth is sandwiched between two fluid parcels with one of them having a positive relative vorticity and the other one a negative relative vorticity. This causes a movement of the fluid parcel to the left in the figure. In general, the displacement causes a wave pattern that propagates with the shallower side to the right on the northern hemisphere and to the left on the southern hemisphere.[1]

Measurements of topographic Rossby waves in the Northern Atlantic.[2] Northward (thicker lines) and eastward (thinner lines) velocity measurements in cm/s at 100, 500, 1000 and 2000 meters depth.

Measurements of topographic Rossby waves on earth

From 1 January 1965 till 1 January 1968, The Buoy Project at the Woods Hole Oceanographic Institution dropped buoys on the western side of the Northern Atlantic to measure the velocities. The data has several gaps because some of the buoys went missing. Still they managed to measure topographic Rossby waves at 500 meters depth.[2] Several other research projects have confirmed that there are indeed topographic Rossby waves in the Northern Atlantic.[3][4][5]

In 1988, barotropic planetary Rossby waves were found in the Northwest Pacific basin.[6] Further research done in 2017 concluded that the Rossby waves are no planetary Rossby waves, but topographic Rossby waves.[7]

In 2021, research in the South China Sea confirmed that topographic Rossby waves exist.[8][9]

In 2016, research in the East Mediterranean showed that topographic Rossby Waves are generated south of Crete due to lateral shifts of a mesoscale circulation structure over the sloping bottom at 4000 m (https://doi.org/10.1016/j.dsr2.2019.07.008).

References

  1. Jump up to: 1.0 1.1 1.2 Cushman-Roisin, Benoit; Beckers, Jean-Marie (2011), Introduction, International Geophysics, 101, Elsevier, pp. 3–39, doi:10.1016/b978-0-12-088759-0.00001-8, ISBN 9780120887590, http://dx.doi.org/10.1016/b978-0-12-088759-0.00001-8, retrieved 2022-03-17 
  2. Jump up to: 2.0 2.1 Thompson, Rory (January 1971). "Topographic Rossby waves at a site north of the Gulf Stream". Deep Sea Research and Oceanographic Abstracts 18 (1): 1–19. doi:10.1016/0011-7471(71)90011-8. ISSN 0011-7471. Bibcode1971DSRA...18....1T. http://dx.doi.org/10.1016/0011-7471(71)90011-8. 
  3. Louis, John P.; Petrie, Brian D.; Smith, Peter C. (January 1982). <0047:ootrwo>2.0.co;2 "Observations of Topographic Rossby Waves on the Continental Margin off Nova Scotia". Journal of Physical Oceanography 12 (1): 47–55. doi:10.1175/1520-0485(1982)012<0047:ootrwo>2.0.co;2. ISSN 0022-3670. Bibcode1982JPO....12...47L. http://dx.doi.org/10.1175/1520-0485(1982)012<0047:ootrwo>2.0.co;2. 
  4. Oey, L-Y.; Lee, H-C. (December 2002). "Deep Eddy Energy and Topographic Rossby Waves in the Gulf of Mexico". Journal of Physical Oceanography 32 (12): 3499–3527. doi:10.1175/1520-0485(2002)032<3499:deeatr>2.0.co;2. ISSN 0022-3670. Bibcode2002JPO....32.3499O. 
  5. Hamilton, Peter (July 2009). "Topographic Rossby waves in the Gulf of Mexico". Progress in Oceanography 82 (1): 1–31. doi:10.1016/j.pocean.2009.04.019. ISSN 0079-6611. Bibcode2009PrOce..82....1H. http://dx.doi.org/10.1016/j.pocean.2009.04.019. 
  6. Schmitz, William J. (March 1988). <0459:eotefi>2.0.co;2 "Exploration of the Eddy Field in the Midlatitude North Pacific". Journal of Physical Oceanography 18 (3): 459–468. doi:10.1175/1520-0485(1988)018<0459:eotefi>2.0.co;2. ISSN 0022-3670. Bibcode1988JPO....18..459S. http://dx.doi.org/10.1175/1520-0485(1988)018<0459:eotefi>2.0.co;2. 
  7. Miyamoto, Masatoshi; Oka, Eitarou; Yanagimoto, Daigo; Fujio, Shinzou; Mizuta, Genta; Imawaki, Shiro; Kurogi, Masao; Hasumi, Hiroyasu (May 2017). "Characteristics and mechanism of deep mesoscale variability south of the Kuroshio Extension". Deep Sea Research Part I: Oceanographic Research Papers 123: 110–117. doi:10.1016/j.dsr.2017.04.003. ISSN 0967-0637. Bibcode2017DSRI..123..110M. http://dx.doi.org/10.1016/j.dsr.2017.04.003. 
  8. QUAN, QI; CAI, ZHONGYA; JIN, GUANGZHEN; LIU, ZHIQIANG (2021-03-22). "Topographic Rossby Waves in the Abyssal South China Sea". Journal of Physical Oceanography 51 (6): 1795. doi:10.1175/jpo-d-20-0187.1. ISSN 0022-3670. Bibcode2021JPO....51.1795Q. 
  9. Wang, Qiang; Zeng, Lili; Shu, Yeqiang; Li, Jian; Chen, Ju; He, Yunkai; Yao, Jinglong; Wang, Dongxiao et al. (October 2019). "Energetic Topographic Rossby Waves in the Northern South China Sea". Journal of Physical Oceanography 49 (10): 2697–2714. doi:10.1175/jpo-d-18-0247.1. ISSN 0022-3670. Bibcode2019JPO....49.2697W. http://dx.doi.org/10.1175/jpo-d-18-0247.1.