## 1. Introduction

Energy balance analysis is useful for advancing our current understanding of the mechanisms maintaining the ocean currents. This balance is closely tied to the nature of the interaction between eddies and the mean flow because of the role of eddies in redistributing momentum and heat in the ocean (Flury and Rummel 2007). Eddies can transport energy to distant regions of the basin, interact with the mean flow, and finally dissipate much of the energy into the bottom and lateral friction (Holland et al. 1983).

Eddies play a central role in ocean dynamics, and the kinetic energy of eddies is usually an order of magnitude larger than that of the mean circulation (Ferrari and Wunsch 2009). Accordingly, most energy analysis studies focus on understanding the eddy kinetic energy properties of the flow. For instance, Yang et al. (2013) studied the eddy energy sources and sinks of the South China Sea (SCS). Their energy budget analysis suggests that the most important eddy energy source for the SCS is the energy released from the available potential energy, followed by the energy convergence from surrounding areas in a horizontal direction and energy released from barotropic instabilities. Zhan et al. (2016) examined the sources, sinks, and redistribution of eddy kinetic energy in the Red Sea. They conclude that the eddies acquire kinetic energy predominantly from the conversion of eddy available potential energy, followed by the transfer from the mean kinetic energy and from the direct generation due to time-varying wind stress. The eddy energy sources in the Sea of Okhotsk are investigated in the work of Stepanov (2018). He argues that the contribution of baroclinic instabilities predominates over that of barotropic instabilities in the generation of mesoscale variability along the western boundary of the Sea of Okhotsk. The work of Zhai and Marshall (2013) is particularly interesting because it focuses on the vertical fluxes of eddy energy in the North Atlantic subtropical and subpolar gyres and studying such fluxes in the Gulf of Mexico (GoM) is the primary motivation for this article. Zhai and Marshall (2013) concluded that the vertical energy flux is downward in the subtropical gyre and upward in the subpolar gyre to reconcile the mismatch between the depth of eddy energy sources related to baroclinic instabilities and the vertical structure of the horizontal dispersion of eddy energy. However, the work of Zhai and Marshall (2013) was limited to exploring the eddy kinetic energy generation and energy fluxes and did not take into consideration the exploration of the whole energy cycle, thereby including in their analysis the generation, dissipation, conversion, and pathways of the mean kinetic energy, mean available potential energy, and eddy available potential energy reservoirs. Kang and Curchitser (2015, hereafter KC15) derived the energy equations to analyze the energy exchange cycle of the Gulf Stream and concluded that eddy kinetic energy in the region is generated predominantly by the barotropic instability followed by the baroclinic instability. A quantitative description of the deep GoM energy cycle is crucial for improving the current understanding of how the deep Gulf general circulation functions. The energy equations presented by KC15 consist of a theoretical framework for the evaluation of the deep GoM energy cycle and provides us with a means of establishing a broader physical picture of the processes involved in maintaining the deep circulation.

The GoM forms a semienclosed region with connections to the Caribbean Sea through the Yucatan Channel and to the Atlantic Ocean through the Florida strait and is often approximated as a two-layer system where the boundary between the upper and the deeper layer is usually situated at 1000-m depth (Hamilton 2009; Cardona and Bracco 2016; Chang and Oey 2011). The upper-layer circulation is dominated by the Loop Current (LC), and is covered fairly well in the literature (Alvera-Azcárate et al. 2009; Hamilton et al. 1999; Oey et al. 2005), while the deep layer has attracted less attention because it is less easily observed. Numerical studies present a general cyclonic mean flow of the deep Gulf (Oey and Lee 2002; Lee and Mellor 2003; Chang and Oey 2011; Maslo et al. 2020), which has been supported by observations (Weatherly et al. 2005; DeHaan and Sturges 2005; Pérez-Brunius et al. 2018). Observations indicate that the deep GoM is a surprisingly energetic environment, where the recorded speeds in the northern Gulf can exceed 90 cm s^{−1} (Hamilton and LugoFernandez 2001). Recently, Pérez-Brunius et al. (2018) analyzed 158 drifting float trajectories, the largest deep GoM float study thus far, and presented the mean velocity vector field. The mean deep GoM circulation deduced from the subsurface floats consists of two mean flow structures: a cyclonic boundary current and a deep cyclonic gyre in the western part of the Gulf. The same mean flow structures were also simulated reasonably well by Maslo et al. (2020) using a 5-yr (2010–14) ROMS numerical simulation to study the connectivity of the deep Gulf, and the same numerical dataset is employed in this study.

The studies exploring the sources of energy in the deep GoM and the interaction between the upper and lower layer are mostly concentrated in the eastern Gulf due to high interest in understanding the dynamics of the LC and the mechanism related to the detachments of its anticyclonic eddies. Oey and Lee (2002) simulation results show that the source of deep eddy kinetic energy east of approximately 91°W comes from the LC while over the western Gulf additional source is from the southwestward propagating Loop Current eddies (LCEs). Lee and Mellor (2003) suggested, based on their model results, that the deep cyclonic circulation in the eastern Gulf, driven by the LC fluctuations of the upper layer, plays an important role as an energy source for the whole deep Gulf circulation. Oey (2008) analyzed the results of a high-resolution numerical model to explain the origin of the deep eddies and their important role in forcing the topographic Rossby waves that disperse energy at the northern slopes of the Gulf. Hamilton et al. (2016) presented an overview of an observational study of the LC and reported that the lower layer proved to be highly energetic only during relatively short periods of time (2–3 months), just prior to or during the eddy detachment due to baroclinic instability. Donohue et al. (2016) observed a marked increase of deep eddy kinetic energy during the LCEs detachment and formation events. Moreover, they reported that the deep eddies that occur during these events gain their high-energy levels in a pattern consistent with developing baroclinic instability. However, little is known about the processes and pathways by which energy is transported through the rest of the Gulf. Comprehending the physics of these processes is fundamental for improving the understanding and prediction of the deep-water environment that impacts oil and gas operations, as well as biological, sediment, and pollutant transport.

This paper focuses on the deep Gulf energy cycle, eddy–mean flow interaction, and energy pathways based on a 5-yr (2010–14) ROMS numerical simulation. In particular, we aim to answer the following research questions: 1) How is the energy driving the deep GoM circulation maintained? 2) What are the characteristics of the eddy–mean flow interaction in the deep GoM? 3) How and where is the energy transferred from the upper layer to the deeper layer?

The paper is organized as follows: section 2 describes the energy equations and a numerical simulation employed in this study, section 3 presents the main results about the energetics of the deep GoM, and section 4 summarizes the paper.

## 2. Methodology

### a. Energy budget equations

**u**= (

*u*,

*υ*,

*w*) is the velocity vector,

*f*is the Coriolis frequency,

*ρ*is density with

*ρ*

_{0}= 1000 kg m

^{−3}its constant value,

*p*is pressure,

*g*is the gravitational acceleration. The density and pressure are given in Eq. (5), where

*ρ*

_{r}and

*p*

_{r}are the reference density and pressure, and

*ρ*

_{a}and

*p*

_{a}represent the perturbation density and pressure. The reference density and reference pressure were chosen to be the time mean and area mean values that are constant at a given depth. The density transport in Eq. (6) is derived according to Storch et al. (2012) from the temperature

*T*and salinity

*S*transport and the equation of state

*ρ*=

*ρ*(

*T*,

*S*,

*z*). The variable

*N*in Eq. (6) is the buoyancy frequency defined by

*ρ*

_{0}

*u*′ and

*ρ*

_{0}

*υ*′, respectively, and then taking the time average of their sum to give

*F*& TD) of Eqs. (14)–(17), denote change rates of EKE, MKE, EPE, and MPE due to forcing, density sources, and turbulent diffusivity (TD) induced by the subgrid processes (Stepanov 2018). In Eq. (14), the first term on the RHS,

**u**

_{h}are the horizontal velocities and ∇

_{h}is the horizontal gradient operator. The second term,

In Eq. (15), the first term on the RHS,

In Eq. (16), the first term in the RHS,

### b. Model configuration and validation

The ocean model used in this study is the Regional Ocean Modeling System (ROMS, Shchepetkin and McWilliams 2005). ROMS is a three-dimensional, terrain-following, free-surface, ocean circulation model, which uses hydrostatic and Boussinesq approximation to solve the Reynolds-averaged Navier–Stokes equations. The model domain extends from 97.7° to 79°W and from 15.6° to 30.5°N. The model is implemented with a horizontal resolution of about 5 km and 36 vertical terrain-following levels. Vertical eddy diffusivity was computed using the Mellor–Yamada 2.5 scheme (Mellor and Yamada 1982; Galperin et al. 1988), while the horizontal diffusion was represented using a Smagorinsky (1963) eddy parameterization. A free-running simulation was integrated for the calendar years of 2010–14 (5 years total), and its daily mean results are analyzed in this study. This model has been used previously to study the connectivity of the deep GoM (Maslo et al. 2020), where the model was validated for the deep Gulf using 158 floats drifting between 1500- and 2500-m depth and current velocity data from 28 moorings. We encourage the reader to turn to this publication for more information about the simulation configuration.

As discussed in the introduction, the dynamics of the upper layer affect the energetics of the deep layer. Therefore, a validation of the model in the upper layer is also recommended. In this regard, the surface MKE and EKE obtained from the geostrophic currents provided by Archiving, Validation and Interpretation of Satellite Oceanographic data (AVISO; https://www.aviso.altimetry.fr/en/my-aviso.html), and the geostrophic currents calculated from ROMS altimetry are compared to determine if they present a similar distribution and overall magnitude of values to be considered suitable for use in the energetics analysis. The AVISO dataset has a spatial resolution of 0.25° and a temporal resolution of 1 day (January 2010–June 2014), while the spatial resolution of the ROMS altimetry has been reduced to match the one from AVISO.

Comparing the mean LC position, denoted by the 17-cm sea surface high (SSH) contour (Leben 2013) of the model and AVISO results (Figs. 1a,b), one can see that the model results match reasonably well the elongation and thickness of the mean LC position obtained from the observations. Both the model and observed MKE distribution presents its highest values in the area of the LC where observed maximum values reach 500 J m^{−3} (Fig. 1b) and the modeled 600 J m^{−3} (Fig. 1a). Another point to observe is that the MKE derived from observation is predominantly concentrated in the eastern part of the Gulf while the model displays an additional current close to the west coast with MKE values reaching 150 J m^{−3}. Similarly the EKE obtained from the satellite observation (Fig. 1d) is concentrated in the eastern part of the GoM (eastward of 90°W) with its values reaching 300 J m^{−3} while the model EKE (Fig. 1c) displays lower energy values (~200 J m^{−3}) and its distribution extend deep into the western part of the Gulf. Although there are differences in distribution and range between the model and the observed MKE and EKE, it can be assumed that the simulated circulation in GoM is sufficiently accurate and is therefore considered appropriate for the following energetics analysis.

## 3. Results

### a. Energy cycle

Equations (14)–(17) include eight conversion terms that exchange energy among the energy reservoirs. These exchanges describe a cycle of energy, which is often represented in a schematic diagram called the Lorenz energy cycle (Lorenz 1955). A traditional Lorenz energy cycle is very often used to illustrate the energy pathways in the global oceans and atmosphere or in a closed region where the divergence terms in Eq. (18) vanish resulting in a direct conversion of energy and a simpler energy diagram. However, in the open regions it is also necessary to take into consideration the transport of energy due to advection and due to the divergence of the pressure work. The latter adds some complexity to the diagram and changes its simple shape. Accordingly, we prefer to omit the term Lorenz energy cycle to avoid confusion.

It is important to emphasize that the values of the reference density *ρ*_{r} and reference pressure *p*_{r} in the energy equations depend on the choice of the area to be analyzed. Thus, in this work, we analyzed only the area of the Gulf bounded by the Yucatan and Florida straits, as denoted by the dashed red lines in Fig. 1.

Since ROMS uses a generalized vertical terrain-following coordinate system, the velocities were linearly interpolated to 33 depths. These depths mimic the standard oceanic depths (Levitus 1982) except on the first layer where we chose to start at a depth of 1 m to avoid blank values due to free surface fluctuation. Using the interpolated model output, we evaluated the four ocean energy components MKE, EKE [Eqs. (9) and (10)], MPE, and EPE [Eqs. (12) and (13)] as well the energy conversion terms Eqs. (14)–(17). It is important to note that the last terms on the RHS of Eqs. (14)–(17) representing the change rates of energy due to forcing, density sources and turbulent diffusivity are not explicitly evaluated from the model results but evaluated from Eqs. (14)–(17) based on the fact that all other terms have been evaluated.

The area-mean energy densities of energy reservoirs are displayed in Fig. 2. As mentioned in the introduction, the depth of 1000 m is usually adopted to divide the Gulf into two layers. It is interesting to note that also from an energy analysis perspective, the depth of 1000 m represents a clear distinction between the upper and the deeper layer. In the upper layer, all reservoir energy densities are of the same order of magnitude decreasing exponentially until the 1000-m depth. Under the 1000-m depth EKE and MKE (KE) remains approximately constant, while MPE and EPE (PE) continue to decrease until the 1500- and 2000-m depths, respectively. This means that under 1000 m the PE terms receive less energy inflow to sustain themselves in respect to KE reservoirs. Very similar results were found by KC15 in their Gulf Stream along-coast region (see Fig. 5c in KC15).

The energy transfer diagram in Fig. 3 displays only the dominant (nonnegligible) terms from Eqs. (14)–(17) separately for the upper and the deeper layer of the Gulf, while the energy diagram for the whole Gulf can be obtained by summing the two parts together. These terms have at least an order of magnitude higher values than the neglected terms.

The dominant energy source for the upper layer is the MKE horizontal ^{8} W). The PW has a divergence form and is zero in a closed domain, which means that the energy is entering into the Gulf with the LC. Another source of energy in the Gulf is the wind, which has not been explicitly evaluated in this work but one can observe its effect in the ^{8} W) because the generation of energy due to wind is higher than the dissipation of energy due to turbulence. Because the LC spatial variability at the Yucatan and Florida straits is constrained by the coast, the EKE horizontal PW′ contribution to the EKE generation in the Gulf is minor.

In the upper layer, the mean flow drives the eddy flow, where the EKE → MKE conversion term releases the energy from the mean flow and the MKE → EKE term is used to convert this energy into the eddies. The whole energy transfer related to barotropic instabilities (MKE → EKE) in the upper layer amounts to 34.9 × 10^{8} W while the sum of energy transfer related to baroclinic instabilities (EPE → EKE) amounts to 25.9 × 10^{8} W, which means that in the upper-layer barotropic instabilities or horizontal shear is the dominant generator of eddies. Typically, the eddy generation from MKE is believed to be of importance for regions characterized by an intense current of about 1 m s^{−1} as seen in the Labrador Sea (Eden and Böning 2002), the Gulf Stream region (KC15) or South China Sea (Yang et al. 2013), while the baroclinic instability appears to be the most important mechanism in generating mesoscale eddies activity in most other parts of the ocean (Beckmann et al. 1994; Storch et al. 2012). Another thing to note is that the conversion term MKE → EKE is approximately equal to the term EKE → MKE and MPE → EPE is approximately equal to EPE → MPE indicating that the Gulf is behaving like a closed domain and displaying a local conversion of energy.

An important part of analyzing the upper layer was to determine how the transfer of energy into the deep layer occurs. The energy is transported downward by vertical PW (

About 75% of the energy sustaining the deep KE is transferred from the upper to the deep layer by the vertical PW, approximately 6% by the horizontal PW through the Yucatan and Florida straits and ~19% is generated through the processes related to baroclinic instabilities. The vertical PW′ generated by the eddy flow is more than 2 times higher than the vertical *S* & TD), where the subgrid diffusion (parameterized in the model) is destabilizing the stratification by diffusing the water from a denser layer into a lighter one and consequently changing the perturbation density *ρ*_{a} in Eqs. (12) and (13), resulting in an increase of APE in the deep layer. It is important to point out that density sources [*S* & TD terms is purely from the turbulent diffusion.

In the deep layer, the eddy flow drives the mean flow, where the MKE → EKE barotropic term releases the energy from the eddies, and the EKE → MKE term is used to convert this energy into the mean flow. This is the opposite of the mechanism found in the upper layer. Although this process is important in sustaining the MKE reservoir its contribution of about 1.6 × 10^{8} W is much smaller than the contribution of the vertical PW of approximately 6.4 × 10^{8} W. Another difference with the upper layer is that in the deep layer the baroclinic conversion term EPE → EKE (4.7 × 10^{8} W) is higher than the barotropic conversion term EKE → MKE (1.6 × 10^{8} W) and that the energy conversion due to vertical shear is higher than the conversion due to horizontal shear. The conversion terms MPE → EPE and EPE → MPE in the deep layer are negligible while the term MKE → EKE is approximately equal to the term EKE → MKE indicating a local conversion of energy also in the deep layer. In the end, the energy of the deep GoM is dissipated through the *F*′ & TD′ terms by the bottom drag and turbulent viscous stresses. Regarding the analysis of the energy cycle, we would also like to point out that the MPE → EPE and EPE → EKE conversion terms (in the upper and lower layer) are not in the same order of magnitude (Fig. 3). The latter is not in line with a traditional baroclinic instability energy pathway (Youngs et al. 2017), usually present in the global-scale Lorenz energy cycles (Olbers et al. 2012).

### b. Energy generation and dissipation

The goal of this section is to understand how the energy that drives the deep GoM circulation is maintained. Equations (14)–(17) describe energy inflow and outflow into each energy reservoir separately. The terms in this equation displaying positive values represent the energy flux into the reservoir and as such are sustaining the energy, while the terms with negative values represent the energy losses.

It is common in the literature to analyze only the EKE reservoir sources and sinks and to display the spatial distribution of each term in Eq. (14) in separate figures, usually resulting in six figures (Yang et al. 2013). Because we are examining all four energy reservoirs in two layers with a split horizontal and vertical transfer of energy, a complete analysis would amount to an overwhelming (~50) number of figures. The shortcoming of this kind of analysis is that it is difficult to summarize the results and understand which process is dominant in a specific part of the domain. To avoid this scenario an innovative approach has been adopted. Instead of examining each term in a separate figure and determine where each term is a source or sink of an energy reservoir based on its sign and strength, we decided to display all the terms corresponding to a specific energy reservoir in only two figures. The first figure focusing on the energy generation (energy sources) and the second figure on energy dissipation (energy sinks). To create the energy generation figure we searched in each computational cell of the Gulf for the term with the largest positive value, while in the energy dissipation figure we searched for the most negative term.

Because it is difficult to distinguish between more than four colors in a single figure, the mean horizontal *S*′ & TD′ term have been joined together. The reasons for this are twofold. The first reason is that this work focuses on understanding how the energy in the deep GoM is maintained and less on its dissipation. The second reason is that a similar merging has already been done in the work of Zhai and Marshall (2013), where they join together all the terms in Eq. (14) except the vertical PW′ and EKE source term EPE → EKE. The difference between our approach and that of Zhai and Marshall (2013), is that we also examined separately the barotropic MKE → EKE term and we did not join this term together with the other horizontal eddy energy fluxes.

#### 1) EKE generation and dissipation

The magnitude and the distribution of the EKE energy reservoir and the EKE conversion terms depth-integrated separately for the upper and lower layer is presented in Fig. 4. The upper-layer EKE reservoir (Fig. 4a) shows the highest values in the area of the LC and then gradually decreases its energy level toward the western Gulf, while maintaining higher values between the 25° and 28°N, where approximately 80% of LCEs go through (Vukovich 2007). Comparing the EKE distribution of the upper (Fig. 4a) and deeper layer (Fig. 4b) it can be observed that they share a similar form, possibly indicating the connectivity between the upper and deeper layer EKE. The deep EKE also displays a very similar distribution as the EKE produced by the drifting floats (see Figs. 3–38 in Hamilton et al. 2016). Higher values of EKE (Fig. 4a) occupy a larger area in the eastern-central part of the Gulf, while the higher MKE values (Fig. 5a) are mostly confined to the sharp boundary currents. A strong mean-to-eddy MKE → EKE conversion term (corn color in Fig. 4c) related to barotropic instabilities can be observed in the area of the LC from the Yucatan channel up to its tip. Similar results were also simulated by Garcia-Jove et al. (2016). Another noticeable color in Fig. 4c is red (EPE → EKE), denoting the EKE generation by the release of APE stored in the tilted isopycnals. The EPE → EKE term displays the highest values on the eastern half of the LC from its tip down to 24°N and in contrast to the MKE → EKE term, which is dominant on its western side. This term, although weaker, also seems to be important in the central part of the Gulf. As mentioned in the section 3a, the divergence of vertical PW′ (Fig. 4e) in the upper layer is directly connected to the convergence of the vertical PW′ in the deep layer (Fig. 4d), where a prevailing green color can be observed across the Gulf and especially inside the contour representing the mean LC position (Fig. 4d).

The latter confirms the quantitative results presented in section 3a that the vertical PW contributes to about 75% of the energy influx into the deep GoM. Also noticeable is the contribution of the horizontal PW′ + *F*′ & TD′ term. Nevertheless, the latter is mostly redistributing the energy with the horizontal PW′ across the deep Gulf as the total contribution of the *F*′ & TD′ term is negative (Fig. 3b). The last term that has some influence in the generation of EKE in the deep layer is the EPE → EKE term related to baroclinic instabilities. The EPE → EKE term is most effective in disturbing the stable stratification under the area of the LC and over the area of the steep slopes along the 26°N. These steep slopes also represent the locations where the deep eddies collide with the continental slope and release the energy (MKE → EKE in Fig. 4f) to generate MKE. Comparing Fig. 4d and Fig. 4f it is possible to note that the areas of the generation of EKE due to vertical PW′ (Fig. 4d) are balanced by the dissipation of the energy by the horizontal PW′ + *F*′ & TD′ term (Fig. 4f). The latter indicates that the horizontal PW′ + *F*′ & TD′ term redistribute and diffuse the energy inflow into the deep layer due to the vertical PW′.

#### 2) MKE generation and dissipation

The upper and lower EKE reservoirs (Figs. 4a,b) have a very similar distribution of energy, while the MKE reservoirs displays a very different distribution of energy between the upper and lower layer (Figs. 5a,b). In the upper layer, the strongest MKE values are following the shape of the mean boundary of the LC (Fig. 5a) while in the deep layer the MKE is concentrated in the areas of the sharp boundary currents (Fig. 5b). The latter is possibly indicating weaker energy connectivity between the upper- and lower-layer MKE energy reservoirs in comparison to the EKE reservoirs.

An important part of the energy inflow into the upper layer is redistributed and diffused across the Gulf by the

The EKE generation and dissipation terms of the deep layer (Figs. 4d,f) are roughly evenly distributed in the Gulf interior as well as on its boundary, while the MKE generation and dissipation terms (Figs. 5d,f) are mostly concentrated on its boundary, where the strongest boundary currents are located. The highest values of the mean vertical ^{8} W of MKE energy is generated in the deep also by MPE → MKE term extracting energy stored in the mean stratification mostly in the eastern Gulf. Another term that has an important role in maintaining the circulation in the deep Gulf is the

#### 3) EPE and MPE generation and dissipation

Because in the cases of the EPE and MPE reservoirs the amount of energy transfer from the upper to the lower layer is negligible (Fig. 3), the upper-layer EPE and MPE terms are not relevant to this work and consequently will not be analyzed.

In comparison to the analysis of the EKE and MKE reservoirs where several terms are affecting their energy generation and dissipation, the EPE and MPE analysis is rather simple because there are only two terms affecting each energy reservoir. It can be seen in Fig. 6a that the highest values of EPE are located under the LC and in the northwestern corner of the Gulf, also called the “eddy graveyard” (Biggs et al. 1996). A noticeable area of higher EPE can also be observed in the western part of the Gulf in the area of the deep gyre (Maslo et al. 2020). It can be observed in Fig. 6b that the EPE is generated mostly by the turbulent diffusion term (*S*′ & TD′) and by a lesser extent from the EKE → EPE term. The turbulent diffusion term is generating EPE in the areas of rough bathymetry, steep slopes, and under the LC. The only two nonnegligible terms in Eq. (16) in the deep GoM are the *S*′ & TD′ and the EKE → EPE terms. This means that the *S*′ & TD′ term is approximately equal to −EKE → EPE, which itself is equal to EPE → EKE term in Eq. (14). The latter indicates that the EPE generated by the turbulent diffusion (*S*′ & TD′) is converted to EKE by the EPE → EKE term and is related to baroclinic instabilities. The distribution of EKE → EPE along the boundary presents both positive (Fig. 6c) and negative values (Fig. 6d), indicating the energy flux from the eddies to the mean stratification (Yang et al. 2013), which is related to the interaction between the flow and the topography.

By comparing Figs. 6b and 6c with Figs. 7b and 7c a very similar color pattern can be observed indicating a similar energy conversion for the MPE reservoir. The turbulent diffusion term

Comparing the MPE reservoir energy distribution using the whole computational domain (not shown) to the results with the domain limited to the GoM (Fig. 7a), it can be observed that the reference density has a noticeable effect on the result. The latter was also observed by KC15 and Storch et al. (2012), and consequently further analysis of the MPE is not particularly meaningful. Although the reference density also has an effect on the conversion terms presented in Figs. 7b and 7c this effect does not change the MPE energy generation and conversion physics as discussed before.

### c. Energy pathways

As discussed in the previous sections, the energy transport between the upper- and lower-layer MPE and EPE is negligible and therefore will not be analyzed. The focus of this section is to understand the general energy transport of the EKE and MKE terms between the upper and lower layer and between the eastern and western part of the Gulf as a whole. A possible way to achieve this would be to divide the Gulf into many cross sections and then summarize the result for the whole Gulf. Nevertheless, we chose to use another method that consists of integrating the energy terms along the meridian direction (south–north) in a similar way as is usually done in a vertical direction (depth integrated).

#### 1) EKE sources and pathways

The ROMS vertical coordinate is defined to be negative when pointing from the surface to the ocean floor. Accordingly, the vertical eddy PW′ flux must be negative to transfer energy into the deep GoM. To achieve the negative vertical PW′ flux the values of eddy pressure *p*′ and eddy vertical velocity *w*′ must have opposite signs. In the simulations, cyclonic eddies predominantly exhibit negative *p*′ values, because their pressure is smaller than the average pressure, and they display positive *w*′ values, which means that the vertical velocities are higher than the average *p*′ values are positive, and *w*′ values are negative.

The article by Zhai and Marshall (2013) was the main inspiration for the analysis of the energy pathways, which proposed that the vertical eddy energy fluxes

As already mentioned in this work, a divergence of the vertical PW energy in the upper layer must result in a convergence of vertical PW energy in the lower layer. Therefore, to understand the vertical transport of energy, it is necessary to understand the intricacies between the divergence of vertical PW and the other terms in Eqs. (14) and (15). These equations represent a budget, where the LFS is approximately zero, and the terms on the RHS are in balance. This means that the outflow of energy with one term must be balanced by the inflow of energy by the other terms. In this context, we were interested in finding out which are the terms causing the outflow of energy by the divergence of the vertical PW in the upper layer, which results in a convergence of vertical PW energy in the lower layer.

Figure 8 presents the basin-averaged vertical profiles of the terms in Eq. (14) subsampled over the cells that contain only the divergent vertical PW′, which has a central role in transferring the EKE from the upper layer to the lower layer. We can observe that the most negative values of vertical PW′ are predominantly balanced by the horizontal PW′ + *F*′ & TD′ term and that the horizontal redistribution and diffusion of energy has a dominant role in pushing the energy in the vertical direction. Moreover, we can note that the baroclinic term (EPE → EKE) and the barotropic term (MKE → EKE) are a range of magnitude smaller, while the baroclinic term still presents higher values than the barotropic term. The discovery of the primary source of the vertical energy flux represents an important contribution of this work.

The EKE reservoir (Fig. 9a) illustrates higher values of energy in the deep layer in respect to MKE reservoir (Fig. 11a) as previously observed in the energy diagram (Fig. 3). The deep EKE is noticeably stronger in the eastern part of the Gulf under the mean location of the LC approximately from 88° to 85°W, as previously observed in Fig. 4b. Although a beam of energy reaching the floor can also be observed in the western part of the Gulf.

Most of the conversion term related to the baroclinic instabilities (EPE → EKE) is confined to the upper 1000 m, while most of the energy conversion between the mean and the eddy flow related to barotropic instabilities (MKE → EKE) is confined to the upper 500 m (Fig. 9c). Both conversion terms are especially strong and penetrate deeper into the water column in the eastern part of the Gulf under the LC. The dashed black squares in Figs. 9b, 9c, and 9e denote the area of the Gulf where the vertical energy transfer by the vertical eddy PW′ is particularly noticeable and will be further discussed. High values of vertical eddy PW′ can be observed in the lower part of the square (below 1000 m) and a colorful representation of all the other terms in its upper part (Fig. 9c), supporting the finding that in the Gulf the EPE → EKE term is not the dominant term causing vertical energy transport.

Although Fig. 9c indicates that the EPE → EKE term is not the dominant term in the area of pronounced vertical transport, it does not provide the information from exactly which terms originate in the vertical PW′ in the deep GoM. To obtain this information we have to compare the distribution of the energy terms in the upper layer of the EKE generation Fig. 9c to the area covered by the vertical PW′ in the upper layer of the EKE dissipation Fig. 9e. It can be observed that vertical eddy PW′ (green color area in Fig. 9e) covers mostly the area of the EPE → EKE term (Fig. 9c) and the area near the surface covered by the horizontal PW′ + *F*′ & TD′ term (Fig. 9c). Although the contribution of the EPE → EKE term (Fig. 9c) to the dissipation (divergence) of vertical PW′ (Fig. 9e) appear to be higher than the other energy terms, its basin averaged values are a range of magnitude smaller than the contribution of the horizontal PW′ + *F*′ & TD′ term, especially up to a depth of 250 m (Fig. 8). Finally, the energy transported from the upper layer by the vertical PW′ is redistributed and dissipated in the lower layer by the horizontal PW′ + *F*′ & TD′ term (Fig. 9e).

As expected, strong vertical energy flux

Figure 9d presents the horizontal (east–west) eddy energy flux

#### 2) MKE sources and pathways

Figure 10 shows that also in the case of MKE the dominant term pushing the energy downward is the

The maintaining of the MKE reservoir by the different contributions of the dominant terms can be observed by the comparison of Figs. 11a and 11c, respectively. In contrast to the EKE reservoir (Fig. 9a) where the energy beams to the deep layer are gradually decreasing from the surface to the seafloor, the MKE reservoir presents an increase of MKE energy most noticeably between 1500- and 2500-m depth in the eastern side of the Gulf and below 2000 m in its western side. The increase of MKE in the eastern side is related to the generation of MPE by the turbulent diffusion over the rough bathymetry and steep slopes (Fig. 7b) and is then converted to MKE by the MPE → MKE conversion term (Figs. 7c and 11c). On the other hand, the increase of MKE in the western side below 2000-m depth is related to the vertical

Figure 11d presents the horizontal (east–west) mean energy flux, where the same strong westward energy transport can be observed below 2000-m depth, as observed in the case of the horizontal eddy energy pathways (Fig. 9d). As in the aforementioned case, this result is expected because the amount of the vertical

## 4. Summary and conclusions

Based on the outputs of the ROMS ocean model, the energetics of the deep GoM have been investigated in this study. The theoretical framework for the analysis is based on the energy equations for the time-mean and time-varying flow (KC15), where some of the terms were additionally split into their horizontal and vertical components to monitor the energy pathways as introduced by Zhai and Marshall (2013). Using these equations, we examined the energy cycle, eddy–mean flow interactions, and energy pathways focusing on the deep Gulf.

The evaluation of the deep GoM energy cycle is an important contribution of this article and provided the answer to our main research question about how the energy driving the deep GoM circulation is sustained. We find that the KE of the deep circulation is predominantly maintained (75%) by the energy redistribution from the upper to the lower layer by the vertical PW, followed by a considerable amount (19%) by the conversion of energy from the potential to kinetic energy related to baroclinic instabilities and the rest (~6%) by the horizontal PW. Finally, it is interesting to note that in the upper layer, the mean circulation is a generator of eddies while in the deep layer, the eddies drive the mean circulation. These results appear to suggest that, in the GoM, accurately simulating the current in the upper layer is necessary to also successfully simulate the circulation in the deep layer.

A more complete understanding of the spatial distribution of the terms from the energy equations was achieved by analyzing their depth-integrated values, separately, for the upper and the deep layer. To avoid an overwhelming number of figures, which is usually associated with the energetics analysis, and to determine the energy terms with a dominant role in maintaining the deep circulation, a novel approach was implemented to analyze the result. The new approach consisted of analyzing all the terms in a specific energy equation at the same time in only two figures, the first figure focusing on the energy generation and the second figure on the energy dissipation. The benefit of this approach is the density of information about the dominant energy generation and dissipation terms. The disadvantage is that information was lost regarding the nondominant terms, especially when there exist generation (dissipation) terms having comparable strengths. Nevertheless, we believe that the advantages outweigh the disadvantages and that the method could be used in the future for energetics analyses exploring the dominant terms.

The EKE generation and dissipation terms in the deep layer are roughly evenly distributed across the Gulf, while the most intense MKE generation and dissipation terms are concentrated along its boundary where the strongest boundary currents are located. The results show a strong eddy energy transfer from the upper to the deep layer by the vertical PW′ below the area delimited by the mean LC (17-cm SSH contour) position. On the other hand, the highest values of mean vertical

In contrast to the analysis of the EKE and MPE reservoirs, the interpretation of the EPE and MPE results is rather simple because there are only two dominant terms affecting each energy reservoir, the turbulent diffusion terms (*S*′ & TD′ and

Another important part of this research was to understand the general energy transport pathways between the upper and lower layers and the eastern and western parts of the Gulf. The energy transport between the upper and lower layer MPE and EPE was found to be negligible, and therefore only the EKE and MKE energy pathways were analyzed. The latter showed very similar properties of the general energy pathways. Energy is transferred downward in the eastern and the western part of the Gulf and upward in the deep central-western part. Because the downward transport of energy underneath the LC in the eastern GoM is greater than in the western GoM, a strong westward energy transport can be observed below 2000-m depth. Furthermore, we observed that the primary source for the vertical energy flux is the horizontal PW and the turbulent diffusion in the upper layer. This represents a difference between our work and the work of Zhai and Marshall (2013) and highlights an important conclusion of this work. This conclusion is that the baroclinic term is not, by default, the primary source of the vertical eddy energy flux and that further analysis is necessary to determine which are the dominant terms in the energy equations generating the energy transport in the vertical direction.

Although great care was taken to ensure the highest accuracy of the results, there is still room to reduce their computational error. The error arises with the interpolation of the ROMS terrain-following coordinates onto the constant depth coordinates. A better approach might be to implement the energy equations into ROMS and interpolate the final results. Similarly, other authors using models with terrain-following vertical coordinates (KC15; Stepanov 2018) did not report using energy equations adjusted for the sigma coordinates from what we are deducing that they probably used interpolations in their analysis. Accordingly, we are assuming that the interpolated results are sufficiently accurate, and therefore considered appropriate in the energetics analysis.

This paper presents a first attempt in describing a three-dimensional picture of the deep GoM energy cycle, eddy–mean flow interactions, and the energy pathways. These results could present a benchmark for a future model and observational studies of the deep Gulf. Furthermore, the methods described in this work can be applied to other regional or global oceans to study the energy cycle and pathways between the surface and the bottom waters. It should be noted that more studies are required to clarify the triggering mechanism of the downward energy transfer, and more work is required to fully understand the process related to the generation of EKE from EPE in the case of nontraditional baroclinic instability energy pathway.

## Acknowledgments

The study was funded by the National Academies of Sciences, Gulf Research Program (NASGRP) under Grant Number 200006422 and by the National Council of Science and Technology of Mexico, Mexican Ministry of Energy, Hydrocarbon Trust, as part of the Gulf of Mexico Research Consortium (CIGoM), project 201441. The authors wish to thank Matt K. Gough who reviewed and provided useful comments on the manuscript.

## APPENDIX

### Divergence of Vertical PW in the Upper Layer of the Gulf Causes a Convergence of Vertical PW in the Lower Layer

In this section, we provide evidence that a divergence of vertical PW in the upper layer of the GoM must result in a convergence of vertical PW energy in the lower layer and vice versa. The evidence is presented only for the eddy vertical PW′ because the proof for the mean vertical

Figure A1 represents a sketch of the water column control volume consisting of two subvolumes. The lower volume *V*_{1} is bounded by the surface *S*_{1} while the upper volume *V*_{2} is bounded by the surface *S*_{2}. Both surfaces are oriented outward, where **n** is the positive normal to the surface. The upper surface of the control volume (*S*_{1m}) is placed at 1-m depth (rather than on the sea surface) because by following the definition of the divergence theorem the vector field has to be defined inside the control volume, which above the 1-m depth is not always the case due to the free-surface fluctuations. The surface *S*_{1000m} represents a common face between the two subvolumes.

**k**direction (Fig. A1) is equal to the volume integral of the partial derivative with respect to the variable

*z*(Fig. A1) of that component over the region inside the surface. Accordingly, the following equations can be written for the eddy vertical PW′ separately for each subvolume:

The second term on the RHS in Eq. (A2) is neglected because our data show that the *S*_{1m} at 1-m depth is a range of magnitude smaller than the *w* at 1-m depth represents the slow variations of the free-surface high. On the other hand, the second term on the RHS in Eq. (A3) is equal to zero for the following reasons:

- In fluid mechanics, we generally assume that in a thin (few millimeters) layer of fluid in contact with a solid boundary the normal and the parallel velocity to a boundary are equal to zero from which follows that the vertical velocity
*w*at the bottom is equal to zero no matter the slope of the bottom and consequently, also the value of the related term$\overline{{w}^{\prime}{p}^{\prime}}$ at the bottom is equal to zero. - In the ROMS simulations, a quadratic function of velocity (Cushman-Roisin and Beckers 2011) was used to parameterize the bottom friction with a nondimensional constant bottom drag coefficient Cd = 0.003. The estimation of the drag coefficient (Lueck and Lu 1997) assumes a logarithmic velocity profile near the sea bed (Cushman-Roisin and Beckers 2011), where the parallel velocity in contact with a boundary is zero. Thus, also in the simulations the vertical velocity
*w*at the bottom and the related term in Eq. (A3) are zero no matter the slope of the sea bed.

Equation (A4) shows that the divergence of the vertical eddy PW′ in the upper volume must result in the convergence of vertical eddy PW′ in the lower volume and this is how the energy is transferred from the upper layer to the lower layer and the other way around.

## REFERENCES

Alvera-Azcárate, A., A. Barth, and R. H. Weisberg, 2009: The surface circulation of the Caribbean Sea and the Gulf of Mexico as inferred from satellite altimetry.

,*J. Phys. Oceanogr.***39**, 640–657, https://doi.org/10.1175/2008JPO3765.1.Beckmann, A., C. W. Böning, B. Brügge, and D. Stammer, 1994: On the generation and role of eddy variability in the central North Atlantic Ocean.

,*J. Geophys. Res.***99**, 20 381–20 391, https://doi.org/10.1029/94JC01654.Biggs, D. C., G. S. Fargion, P. Hamilton, and R. R. Leben, 1996: Cleavage of a Gulf of Mexico loop current eddy by a deep water cyclone.

,*J. Geophys. Res.***101**, 20 629–20 641, https://doi.org/10.1029/96JC01078.Cardona, Y., and A. Bracco, 2016: Predictability of mesoscale circulation throughout the water column in the Gulf of Mexico.

,*Deep-Sea Res. II***129**, 332–349, https://doi.org/10.1016/j.dsr2.2014.01.008.Chang, Y.-L., and L.-Y. Oey, 2011: Loop current cycle: Coupled response of the loop current with deep flows.

,*J. Phys. Oceanogr.***41**, 458–471, https://doi.org/1.1175/2010JPO4479.1.Chen, R., G. R. Flierl, and C. Wunsch, 2014: A description of local and nonlocal eddyMean flow interaction in a global eddy-permitting state estimate.

,*J. Phys. Oceanogr.***44**, 2336–2352, https://doi.org/10.1175/JPO-D-14-0009.1.Chen, R., A. F. Thompson, and G. R. Flierl, 2016: Time-dependent eddy-mean energy diagrams and their application to the ocean.

,*J. Phys. Oceanogr.***46**, 2827–2850, https://doi.org/10.1175/JPO-D-16-0012.1.Cushman-Roisin, B., and J.-M. Beckers, 2011:

. Academic Press, 828 pp.*Introduction to Geophysical Fluid Dynamics: Physical and Numerical Aspects*DeHaan, C. J., and W. Sturges, 2005: Deep cyclonic circulation in the Gulf of Mexico.

,*J. Phys. Oceanogr.***35**, 1801–1812, https://doi.org/10.1175/JPO2790.1.Donohue, K. A., D. R. Watts, P. Hamilton, R. Leben, and M. Kennelly, 2016: Loop current eddy formation and baroclinic instability.

,*Dyn. Atmos. Oceans***76**, 195–216, https://doi.org/10.1016/j.dynatmoce.2016.01.004.Eden, C., and C. Böning, 2002: Sources of eddy kinetic energy in the Labrador Sea.

,*J. Phys. Oceanogr.***32**, 3346–3363, https://doi.org/10.1175/1520-0485(2002)032<3346:SOEKEI>2.0.CO;2.Ferrari, R., and C. Wunsch, 2009: Ocean circulation kinetic energy: Reservoirs, sources, and sinks.

,*Annu. Rev. Fluid. Mech.***41**, 253–282, https://doi.org/10.1146/annurev.fluid.40.111406.102139.Flury, J., and R. Rummel, 2007:

. Springer Science and Business Media, 164 pp.*Future Satellite Gravimetry and Earth Dynamics*Galperin, B., L. H. Kantha, S. Hassid, and A. Rosati, 1988: A quasi-equilibrium turbulent energy model for geophysical flows.

,*J. Atmos. Sci.***45**, 55–62, https://doi.org/10.1175/1520-0469(1988)045<0055:AQETEM>2.0.CO;2.Garcia-Jove, M., J. Sheinbaum, and J. Jouanno, 2016: Sensitivity of loop current metrics and eddy detachments to different model configurations: The impact of topography and Caribbean perturbations.

,*Atmósfera***29**, 235–265, https://doi.org/10.20937/ATM.2016.29.03.05.Gill, A. E., 1982:

. Academic Press, 662 pp.*Atmosphere-Ocean Dynamics*Hamilton, P., 2009: Topographic Rossby waves in the Gulf of Mexico.

,*Prog. Oceanogr.***82**, 1–31, https://doi.org/10.1016/j.pocean.2009.04.019.Hamilton, P., and A. LugoFernandez, 2001: Observations of high speed deep currents in the northern Gulf of Mexico.

,*Geophys. Res. Lett.***28**, 2867–2870, https://doi.org/10.1029/2001GL013039.Hamilton, P., G. Fargion, and D. Biggs, 1999: Loop current eddy paths in the western Gulf of Mexico.

,*J. Phys. Oceanogr.***29**, 1180–1207, https://doi.org/10.1175/1520-0485(1999)029<1180:LCEPIT>2.0.CO;2.Hamilton, P., A. Bower, H. Furey, R. Leben, and P. Pérez-Brunius, 2016: Deep circulation in the Gulf of Mexico: A Lagrangian study. OCS Study BOEM 2016-081, 289 pp., https://www.boem.gov/Gulf-of-Mexico-OCS-Region-Publications-G/#GULF%20OF%20MEXICO.

Harrison, D. E., and A. R. Robinson, 1978: Energy analysis of open regions of turbulent flows—Mean eddy energetics of a numerical ocean circulation experiment.

,*Dyn. Atmos. Oceans***2**, 185–211, https://doi.org/10.1016/0377-0265(78)90009-X.Holland, W. R., D. E. Harrison, and A. J. Semtner, 1983: Eddy-resolving numerical models of large-scale ocean circulation.

*Eddies in Marine Science*, A. R. Robinson, Ed., Springer, 379–403.Kang, D., and E. N. Curchitser, 2015: Energetics of eddy–mean flow interactions in the Gulf Stream region.

,*J. Phys. Oceanogr.***45**, 1103–1120, https://doi.org/10.1175/JPO-D-14-0200.1.Kang, D., and E. N. Curchitser, 2017: On the evaluation of seasonal variability of the ocean kinetic energy.

,*J. Phys. Oceanogr.***47**, 1675–1683, https://doi.org/10.1175/JPO-D-17-0063.1.Leben, R. R., 2013: Altimeter-derived loop current metrics.

*Circulation in the Gulf of Mexico: Observations and Models*,*Geophys. Monogr.*, Vol. 161, Amer. Geophys. Union, 181–201.Lee, H.-C., and G. L. Mellor, 2003: Numerical simulation of the Gulf Stream system: The loop current and the deep circulation.

,*J. Geophys. Res.***108**, 3043, https://doi.org/10.1029/2001JC001074.Levitus, S., 1982:

. National Oceanic and Atmospheric Administration, 173 pp.*Climatological Atlas of the World Ocean*Lorenz, E. N., 1955: Available potential energy and the maintenance of the general circulation.

,*Tellus***7**, 157–167, https://doi.org/10.3402/tellusa.v7i2.8796.Lueck, R. G., and Y. Lu, 1997: The logarithmic layer in a tidal channel.

,*Cont. Shelf Res.***17**, 1785–1801, https://doi.org/10.1016/S0278-4343(97)00049-6.Maslo, A., J. M. A. C. de Souza, F. Andrade-Canto, and J. R. Outerelo, 2020: Connectivity of deep waters in the Gulf of Mexico.

,*J. Mar. Syst.***203**, 103267, https://doi.org/10.1016/J.JMARSYS.2019.103267.Mellor, G. L., and T. Yamada, 1982: Development of a turbulence closure model for geophysical fluid problems.

,*Rev. Geophys.***20**, 851–875, https://doi.org/10.1029/RG020i004p00851.Oey, L., and H. Lee, 2002: Deep eddy energy and topographic Rossby waves in the Gulf of Mexico.

,*J. Phys. Oceanogr.***32**, 3499–3527, https://doi.org/10.1175/1520-0485(2002)032<3499:DEEATR>2.0.CO;2.Oey, L., T. Ezer, and H. Lee, 2005: Loop current, rings and related circulation in the Gulf of Mexico: A review of numerical models and future challenges.

*Circulation in the Gulf of Mexico: Observations and Models*,*Geophys. Monogr.*, Vol. 161, Amer. Geophys. Union, 31–56.Oey, L.-Y., 2008: Loop current and deep eddies.

,*J. Phys. Oceanogr.***38**, 1426–1449, https://doi.org/10.1175/2007JPO3818.1.Olbers, D., J. Willebrand, and C. Eden, 2012:

. Springer Science and Business Media, 703 pp., https://doi.org/10.1007/978-3-642-23450-7.*Ocean Dynamics*Orlanski, I., and M. D. Cox, 1972: Baroclinic instability in ocean currents.

,*Geophys. Fluid Dyn.***4**, 297–332, https://doi.org/10.1080/03091927208236102.Pérez-Brunius, P., H. Furey, A. Bower, P. Hamilton, J. Candela, P. García-Carrillo, and R. Leben, 2018: Dominant circulation patterns of the deep Gulf of Mexico.

,*J. Phys. Oceanogr.***48**, 511–529, https://doi.org/10.1175/JPO-D-17-0140.1.Shchepetkin, A. F., and J. C. McWilliams, 2005: The Regional Oceanic Modeling System (ROMS): A split-explicit, free-surface, topography-following-coordinate oceanic model.

,*Ocean Modell.***9**, 347–404, https://doi.org/10.1016/j.ocemod.2004.08.002.Smagorinsky, J., 1963: General circulation experiments with the primitive equations.

,*Mon. Wea. Rev.***91**, 99–164, https://doi.org/10.1175/1520-0493(1963)091<0099:GCEWTP>2.3.CO;2.Stepanov, D. V., 2018: Eddy energy sources and mesoscale eddies in the Sea of Okhotsk.

,*Ocean Dyn.***68**, 825–845, https://doi.org/10.1007/S10236-018-1167-3.Storch, J.-S., and et al. , 2012: An estimate of the Lorenz energy cycle for the world ocean based on the STORM/NCEP simulation.

,*J. Phys. Oceanogr.***42**, 2185–2205, https://doi.org/10.1175/JPO-D-12-079.1.Vukovich, F. M., 2007: Climatology of ocean features in the Gulf of Mexico using satellite remote sensing data.

,*J. Phys. Oceanogr.***37**, 689–707, https://doi.org/10.1175/JPO2989.1.Weatherly, G. L., N. Wienders, and A. Romanou, 2005: Intermediate-depth circulation in the Gulf of Mexico estimated from direct measurements.

*Circulation in the Gulf of Mexico: Observations and Models*,*Geophys. Monogr.*, Vol. 161, Amer. Geophys. Union, 315–324.Yang, H., L. Wu, H. Liu, and Y. Yu, 2013: Eddy energy sources and sinks in the South China Sea.

,*J. Geophys. Res. Oceans***118**, 4716–4726, https://doi.org/10.1002/jgrc.20343.Youngs, M. K., A. F. Thompson, A. Lazar, and K. J. Richards, 2017: ACC meanders, energy transfer, and mixed barotropic–baroclinic instability.

,*J. Phys. Oceanogr.***47**, 1291–1305, https://doi.org/10.1175/JPO-D-16-0160.1.Zhai, X., and D. P. Marshall, 2013: Vertical eddy energy fluxes in the North Atlantic subtropical and subpolar gyres.

,*J. Phys. Oceanogr.***43**, 95–103, https://doi.org/10.1175/JPO-D-12-021.1.Zhan, P., A. C. Subramanian, F. Yao, A. R. Kartadikaria, D. Guo, and I. Hoteit, 2016: The eddy kinetic energy budget in the Red Sea.

,*J. Geophys. Res. Oceans***121**, 4732–4747, https://doi.org/10.1002/2015JC011589.