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Surface Alfven Wave Damping in a 3D Simulation of the Solar Wind

Here we investigate the contribution of surface Alfven wave damping to the heating of the solar wind in minima conditions. These waves are present in regions of strong inhomogeneities in density or magnetic field (e. g., the border between open and closed magnetic field lines). Using a 3-dimensional Magnetohydrodynamics (MHD) model, we calculate the surface Alfven wave damping contribution between 1-4 solar radii, the region of interest for both acceleration and coronal heating. We consider waves with frequencies lower than those that are damped in the chromosphere and on the order of those dominating the heliosphere. In the region between open and closed field lines, within a few solar radii of the surface, no other major source of damping has been suggested for the low frequency waves we consider here. This work is the first to study surface Alfven waves in a 3D environment without assuming a priori a geometry of field lines or magnetic and density profiles. We determine that waves with frequencies>2.8x10^-4 Hz are damped between 1-4 solar radii. In quiet sun regions, surface Alfven waves are damped at further distances compared to active regions, thus carrying additional wave energy into the corona. We compare the surface Alfven wave contribution to the heating by a variable polytropic index and find that it an order of magnitude larger than needed for quiet sun regions. For active regions the contribution to the heating is twenty percent. As it has been argued that a variable gamma acts as turbulence, our results indicate that surface Alfven wave damping is comparable to turbulence in the lower corona. This damping mechanism should be included self consistently as an energy driver for the wind in global MHD models.

should be included self consistently as an energy driver for the wind in global MHD models.

Introduction
The physical mechanisms behind the heating of the solar corona and the acceleration of the fast solar wind are two major unresolved issues in solar physics. Thermal heating alone is not sufficient to bring models into agreement with observations of the lower corona and at Earth (Usmanov & Goldstein 2003). The acceleration of the solar wind occurs predominantly within a few solar radii of the surface (Hartmann & MacGregor 1980;Grall et al. 1996). Additionally, Solar and Heliospheric Observatory (SOHO) observations have shown that ions are heated below 4 R ⊙ (Kohl et al. 1998;Esser et al. 1999). Grall et al. (1996) suggested that because the locations for the heating of the corona and the acceleration of the solar wind are the same, it is possible that the same mechanism could contribute to both.
One source of heating is magnetic reconnection associated with flares and nanoflares at the solar surface. Using extreme ultraviolet observations, Patsourakos & Klimchuk (2009) have suggested the heating of active regions is impulsive, and therefore could be associated with nanoflares. In the high speed solar wind, reconnection events current sheets and filaments have been suggested as a heating mechanism (Mattheaus et al. 2003).
Global magnetohydrodynamics (MHD) models that do not include waves employ different methods such as empirical heating functions or varied polytropic index distribution to drive and heat the solar wind and are able to match well with Ulysses, Yohkoh, Helios and Advanced Composition Explorer data (Mikic et al. 1999;Groth et al. 2000;Roussev et al. 2003). To include Alfvén wave damping in a realistic model of the solar environment, physical damping mechanisms must be specified. Some MHD models use Alfvén waves without specifying a damping mechanism. Global (Usmanov & Goldstein 2006) and local (Cranmer, van Ballegooijen & Edgar 2007) models include additional equations for the waves and prescribe an empirical damping length. These studies are benchmarked with Ulysses and Helios observations. Alternatively, one can include the wave energy and momentum without damping (Lionello, Linker & Mikic 2009), and match SOHO Extreme Ultraviolet and Yohkoh soft X-ray observations.
Of the numerous possible mechanisms for damping Alfvén waves, those which we expect to be important for low frequency waves are nonlinear turbulent damping, phase mixing, surface Alfvén waves. In this paper, we study the contribution of surface Alfvén wave damping by utilizing a 3D global MHD simulation of a thermally-driven solar wind (Cohen et al. 2007). In this model, the lower corona is the inner boundary (chromosphere and transition region are not resolved.) Waves are not explicitly included in the model, nor can low frequency waves be resolved due to spatial and temporal resolution limits (to be discussed further in Section 2.2).
In this study we are interested in a damping mechanism that acts in the lower corona (Grall et al. 1996). In the chromosphere, Alfvén waves with frequencies above 0.6 Hz are damped by ion-neutral collisional damping and frequencies below 10 −2 Hz were unaffected (De Pontieu, Martens & Hudson 2001;Leake et al. 2005). Cranmer & van Ballegooijen (2005) found that waves below 10 −2 Hz were not damped by any mechanism in the chromosphere. Cranmer & van Ballegooijen (2005) also found that nonlinear damping occurred over the extended corona. Verdini & Velli (2007) found waves 10 −6 − 10 −4 Hz were reflected by a gradient in the background Alfvén profile, and dissipated not in the lower layers of the atmosphere, but over distance of a few solar radii. In the corona, the ion-cyclotron frequency is 10 4−6 Hz, so cyclotron resonance damping is not relevant for low frequency waves. Phase mixing of outgoing and reflected incoming Alfvén waves has also been studied Suzuki & Inutsuka (2005. Using a combination of three damping mechanisms (nonlinear damping, surface Alfvén wave damping, and phase mixing), Jatenco-Pereira & Opher (1989) were able to match observations of mass loss rates and terminal velocities for cool, giant stars. They applied their model to the Sun and were able to obtain coronal heating and match wind velocity and Alfvén wave power density observations in a 1D simulation (Jatenco-Pereira, Opher & Yamamoto 1994). In this paper, we extend their work on surface Alfvén wave damping in a 3D simulation of the solar corona.
Surface Alfvén waves form on a magnetic interface -a finite thickness boundary separating two regions of plasma with a strong inhomogeneity in magnetic field and/or density. The Alfvén wave in each region can interact, damp and transfer energy into the resonant layer separating the two plasmas (resonant absorption). Ionson (1978) first utilized surface Alfvén waves and resonant absorption as a mechanism to heat coronal loops. The transfer of MHD wave energy by resonant absorption was also studied in Hollweg (1987) and Wentzel (1979). An alternative dissipation mechanism for surface Alfvén waves is nonlinear wave steepening (Ruderman 1992). These and other efforts, e.g. (Lee & Roberts 1986) have resulted in damping lengths which depend on the frequency of the waves, the nature of the magnetic interface, and the local plasma parameters (density, magnetic field and velocity).
Utilizing these relations, the profile of the damping length in the wind has been estimated (Jatenco-Pereira & Opher 1989;Narain & Sharma 1998). All previous studies made assumptions about the wind. For example, (Narain & Sharma 1998) calculated nonlinear viscous damping of surface Alfvén waves in polar coronal holes. They assumed two values of the superradial expansion of the magnetic field lines, profiles for density (based on observations), and a single frequency (0.01 Hz). They obtained one profile, and concluded that the nonlinear damping of the surface Alfvén waves in region of strong magnetic field expansion should contribute significantly to the heating in the solar wind.
The surface Alfvén wave damping length depends on the profile of the background Alfvén speed. As was shown in a survey of Alfvén speed profiles from several MHD models (Evans et al. 2008), the Alfvén profiles for Verdini & Velli (2007) and Cranmer, van Ballegooijen & Edgar (2007) are almost identical below 10 R ⊙ , and the profiles were different from MHD models using empirical heating functions. The profile for Usmanov & Goldstein (2006) is similar to these two, but differs very low in the corona. Evans et al. (2008) concluded that the inclusion of Alfvén waves with empirical damping brought MHD models better in alignment with local heating studies that had the best agreement with observations.
In the present study, we quantify the surface Alfvén wave damping length for use in an MHD wave-driven model. We expect to find surface Alfvén waves in the border between the fast and slow solar wind for two reasons: a) the gradient in density and b) the superradial expansion of the open magnetic field required to fill the space over closed streamers. We will focus on the superradial expansion of the field lines and compare our 3D MHD model with the observational study of Dobrzycka et al. (1999). Our calculations show that waves with periods less than 1 hour (frequency greater than 2.8 ×10 −4 Hz) are damped in the region between 1-4 R ⊙ , the region of interest for both solar wind acceleration and coronal heating (Grall et al. 1996). No other major source of damping has been suggested for these waves in this region. We demonstrate the importance of the 3D geometry in our results. We show that the contribution of the damping of surface Alfvén waves to the wind is on the order of magnitude as (or in some cases larger than) turbulence. It is important to note that this study of waves in a solar wind solution was not self consistent -we did not consider any back effects on the waves from the plasma.
The paper is organized as follows: in section 2 we describe the theory and numerical simulation background. In section 3 we calculate the location of coronal hole boundaries, and the damping length profile along those lines. In section 4 we estimate the energy surface Alfvén waves will deposit below 4 R ⊙ . We also calculate the heating invoked in a semi-empirical thermodynamical model, compare with the wave flux and discuss the results. Finally, conclusions can be found in section 5.

Theory
The inhomogeneity in density and/or magnetic field that gives rise to the surface Alfvén waves can be described analytically as either a discontinuity or finite layer (Hasegawa & Uberoi 1982), such as a flux tube. For the case of a rapidly expanding flux tube of width a, (where a is much smaller than the radius of the flux tube), surface Alfvén waves form on the inner and outer surfaces. These waves can interact, damp and deposit energy into the surrounding plasma with a damping rate (Lee & Roberts 1986), wherek is the average wave number, ω is the frequency and ω 1 and ω 2 are the Alfvén wave frequency on either side of the flux tube (1 representing inside and 2 outside.) We assume the width of the flux tube to be much smaller than the radius. This allows us to takeka = 0.1, as in Jatenco- Pereira & Opher (1989). If the frequency on the outside is much larger than the frequency inside (i.e., a strong inhomogeneity), then the damping rate is The surface Alfvén wave damping length can be written as the Alfvén speed v A = B 2 4πρ divided by the damping rate, The initial damping length L 0 can be written as which, by takingka = 0.1, can be simplified to Utilizing the relation that a ∝ A(r) 1 2 ∝ r S 2 (where S is the superradial expansion factor of the field line), and fixing the frequency of the waves to be constant with height, the damping length in the inertial frame is is the magnetic field strength, ρ is the mass density. The subscript 0 indicates the variable is to be evaluated at the reference height.
In the present study the model does not treat the chromosphere or the transition region; the lower corona is the inner boundary. The cell size at the inner boundary is 3 128 R ⊙ , and so we chose r 0 =1.04R ⊙ as our reference height to assure that calculations would not include the solar surface inner boundary cells.
We quantify the expansion of open field lines by S, given by.
where A cs (r) is the cross sectional area of the flux tube at distance r. A value of 2 for S indicates pure radial expansion. The lines which border closed field lines must open faster than radial to fill the space above the closed loops. In studies where S is not a function of r, typical values chosen were 2-6 for open field regions from 1-10 R ⊙ (Moore et al. 1991;Jatenco-Pereira, Opher & Yamamoto 1994;Narain & Sharma 1998). Here we determine S explicitly as a function of height from 1.04-10 R ⊙ .
A similar parameter for the expansion of a field line is the superradial diverging factor or superradial enhancement factor f , as in We will use a 3D MHD model as a laboratory to estimate the contribution of the surface waves to the wind from 1.04-10 R ⊙ .

Generation of Steady State
We obtain steady state solar wind solutions by using the Solar Corona component of the Space Weather Modeling Framework (SWMF), developed by the University of Michigan (Toth et al. 2005). This 3D global magnetohydrodynamics (MHD) model incorporates Michelson Doppler Imager (MDI) magnetograms to generate an initial magnetic field configuration with the Potential Field Source Surface model (see Cohen et al. (2007) for details). An initial density is assumed on the solar surface (3.4 × 10 8 cm −3 ), and the MHD equations are evolved in local time steps (12,000 iterations) and time accurate calculations (for ten minutes) to achieve steady state solutions for solar minima conditions in a 24 × 24 × 24 R ⊙ domain.
The steady state was generated with Carrington Rotation (CR) 1912. Solar wind solutions from SWMF were validated in Cohen et al. (2008) from CR1916-1929 by comparing with Advanced Composition Explorer and Wind satellite data (near 1 AU). CR1912 was chosen to allow for comparisons to an observational study of the expansion of open field lines (Dobrzycka et al. 1999).
Waves occur naturally as a perturbation to the MHD equations, and so their presence may be expected when solving the MHD equations in space and time. However, in global simulations waves have to be included explicitly (Usmanov & Goldstein 2003) due to time and spatial limitations. The time step of this simulation (0.2 seconds) is less than the smallest period considered in this analysis (3 seconds). Additionally, the grid resolution is not enough to spatially resolve the waves. Dobrzycka et al. (1999) (herein referred to as DO99) characterized the large-scale solar magnetic topology during solar minima conditions (August 1996) using data from the Solar and Heliospheric Observatory's (SOHO) Ultraviolet Coronagraph Spectrometer instrument. They analyzed the latitudinal dependence of two line emission intensities and found the values were constant within the large polar coronal holes but suddenly increased at the border of the holes and equatorial streamers. DO99 used this increase in intensity to identify the colatitude of coronal hole boundary (CHB), i.e. the border between open and closed magnetic field lines. In the present study, we identify the CHB locations as the open field line with the largest colatitude (the angle measured from the pole to the equator) in the steady state described in the previous section. We compare our calculation of the field expansion with the observed values from DO99. Figure 1 shows the 3D coronal hole boundary (CHB) field lines obtained from the model. The different colors refer to: red as northeast (NE); blue as southeast (SE); green as southwest (SW); and purple as northwest (NW). The solar surface is shown colored by the radial component of the magnetic field. On 1996 August 17, there was an active region near the center of the disk, and mostly quiet sun at the intersection of the plane of the sky with the photosphere.

Location and Expansion Factor
The first two rows of Table 1 provide CHB colatitudes (angle measured from the pole to the CHB footpoint) found in DO99 and this study. We find that 3 of the 4 simulated CHB are higher in latitude (i.e., smaller colatitude) compared to DO99. As we discuss below, these differences could be due to projection effects.
The superradial expansion factor S and superradial enhancement factor f were calculated as a function of height for each CHB field line. In Figure 2 we show f for the CHB lines in this study. Additionally, we have included the f profiles which correspond to the minimum and maximum asymptotic values of f for CHBs determined in DO99. Rows 3 and 4 in Table 1 provide the asymptotic superradial enhancement factor value for each line. We find that both S and f cover a larger range of values compared to DOB99. Only the SW line from our simulation falls in the range from DO99 and only from 3-6 R ⊙ . In general, we find that 3 of the 4 boundary lines (all except SW) have lower values in our simulation compared to DO99.
The best agreement for the location of the CHB between the studies is the SW line. The southern hemisphere from the simulation is more similar to the results deduced from observations in the plane of the sky in DO99 than the northern hemisphere. Overall, we find that Dobrzycka et al. (1999) had larger values of f , and a small range of values, for the same field lines. As we show below, this result is due to 3D vs. 2D projection effects.

Projection Effects
In order to quantify the significance of 2D projection effects in the context of the expansion of field lines, we calculated f for four field lines shown in Figure 3a. The projection of the field lines on the plane of the sky is shown in Figure 3b. Contours of solar wind speed (in km s ) are shown in Figures 3a and b, and the solar surface is shown as white sphere. Figure 3c provides the superradial enhancement factor f , calculated according to Equation 8 for each field line (labeled A, B, C and D as in Figure 3b). The calculation of the 3D line is shown as solid lines, and the 2D projection line calculation is shown as dashed lines. Figure 3c demonstrates that a 2D projection of a 3D field line on the plane of the sky can overestimate the divergence of the line. The 3D lines from A-D all approach values of f 4 while the 2D estimates vary between 4 and 13. This projection effect explains why the values for f from our simulation are smaller than those determined in the observational study of DO99. It is crucial, therefore, to do studies of surface Alfvén wave damping in a 3D simulation in order to capture the true divergence of the field lines.

Damping Length
In Figure 4, we plot L SW (see Eq. 6) which was calculated using parameters ρ, B and u sw from the steady state solution. Figure 4a presents L SW for the coronal hole boundary field lines in Figure 1 with frequency 4.17 × 10 −3 Hz, normalized to the initial damping length L 0 of the SW line (chosen because of the agreement with DO99). This normalization allows for comparison of the profile features from different source regions as a function of height. In Figure 4b we feature only the SW line and present L SW for several frequencies, from 3.3 × 10 −1 − 3.8 × 10 −6 Hz. It can be seen in Figure 4b that frequencies above 2.8 × 10 −4 (short dashed line) will be appreciably damped within a few solar radii of the surface. Figure 4a shows distinctly different profiles from the southern and northern CHB lines. We examined the source region of each footpoint and found that the SE and SW lines originated near small active regions in which the radial component of the magnetic field B r ≈ 50 G. Both northern hemisphere lines originated from quiet sun regions (B r ≈ 1 G). For SWMF and other MHD models, Evans et al. (2008) showed that the Alfvén profile will contain a maximum, or hump, if the source region is quiet sun. The profile from an active region in global models begins at a maximum value, and drops to less than a few hundred km s within one solar radius from the surface. The profile of L SW is controlled by the Alfvén speed profile. The normalized profiles in Fig.  4a show that the position corresponding to L SW = 1R ⊙ is closest to the Sun for active regions. The profiles from quiet Sun source regions have a plateau, pushing L SW = 1R ⊙ further from the Sun. The implication of this result can be seen in the equation relating the Alfvén wave energy density, If the damping length is 1R ⊙ or less, then the waves will be damped close to the Sun. Therefore, the presence of the hump means the energy of the surface Alfvén wave can travel further into the corona before substantial damping occurs. This means that the quiet sun region will damp more surface waves at further distances, so it is more efficient in carrying the wave momentum out into the corona. Active regions will damp closest to the Sun.

Wave Energy
In the previous section we considered how surface Alfvén waves at the solar surface with the frequency range 3.8 × 10 −6 to 3.3 × 10 −1 Hz (Cranmer & van Ballegooijen 2005) would be damped in our background solar wind environment. We found that waves with frequency above 2.8 × 10 −4 Hz were appreciably damped below 4R ⊙ . We now consider the contribution of their wave flux to the energy of the wind. There will be a contribution to the momentum of the wind as well, but in this analysis we ignore this contribution. We assume that the wave damping will contribute solely to heating the wind; therefore we derive here an upper limit on their contribution to the heating of the plasma. The spectra of the surface Alfvén waves (Jatenco-Pereira, Opher & Yamamoto 1994) is: where φ 0 = 1.3 × 10 5 erg cm 2 sHz ,ω is the mean frequency in the observed range and the power index corresponding to the low frequency waves we are considering is α=0.6 (Tu et al. 1989).
We assume that this flux of Surface Alfvén waves is propagating along open field lines during solar minima. This flux will decrease with distance as where L SW is the damping length, for each frequency. With the damping lengths calculated in the previous section, we calculate how much flux is lost between R = 1.04 (our self-imposed reference height) and 4R ⊙ . The height of 4R ⊙ was chosen because the contribution to solar wind acceleration and coronal heating must be deposited within a few solar radii of the Sun (Kohl et al. 1998;Esser et al. 1999).
The contribution to the solar wind at each frequency is where the limits are r 1 = 1.04R ⊙ and r 2 = 4R ⊙ , and the definition of L sw from Equation 6 has been included (v A , S, M A , are all functions of r.) We replace L 0 in Eq. 12 with Eq. 5. The total flux lost is found using where the limits are ω 1 = 2.8 × 10 −4 Hz and ω 2 = 0.3 Hz.
Next we compare the potential contribution of the wave flux to the heating in the model (Eq. 22). It should be stressed that we are not doing a self-consistent calculation: we are estimating wave flux from a model that does not include waves, and we are not considering any feedback of the waves on the plasma.

Heating of the Corona
The simulation analyzed in this paper is that of a thermally driven solar wind. The polytropic index Γ in the model varies in space by utilizing the Wang-Sheeley-Arge model and the conservation of energy along a solar wind field line using the Bernoulli equation. This serves to artificially heat the wind (Cohen et al. 2007) in a manner mimicking turbulence Roussev et al. (2003). Figure 5 shows the distribution of Γ in the plane of the sky on 1996 August 17. In this section we quantify the heating due to this variable gamma, and do a comparison with the energy deposited by damped surface Alfvén waves, as in Eq. 13.
The first law of thermodynamics attributes changes in the internal energy U of a gas to work done on or by the gas W , and heat added to or removed from the gas Q. In the case of an ideal gas, the change in internal energy can be written as dU = c v dT , where c v is the specific heat at constant volume. The work is expressed as dW = −pdV , where p is the pressure and V is the volume. The first law can therefore be written as By introducing the ideal gas equation of state and assuming that the ratios of specific heats are constants, one can derive a polytropic equation, p where α is referred to as the polytropic index. The notation stems from Parker (1963) to clarify that this index can (but need not) be the ratio of specific heats, and that we are not necessarily considering an adiabatic process. The symbol γ is typically used for the ratio of specific heats, and in the case of an adiabatic expansion (no heating enters or leaves the system), α = 5 3 . An isothermal wind expansion would be characterized by α = 1. Observations of the solar wind have indicated that α=1.46-1.58 in the heliosphere (Totten, Freeman & Arya 1995). A value closer to unity is adopted in some global MHD models in the region near the Sun in order to generate fast solar wind and match temperature observations in the heliosphere (Usmanov & Goldstein 2003).
All previous discussion had the underlying assumption that α was constant with height. If that condition is not met, then the polytropic index is referred to as an effective (or local) polytropic index and written as Γ (Totten, Freeman & Arya 1995). The polytropic equation (Eq. 15) is modified to such that the relationship between density and pressure is not simple. The variation of Γ with height has been utilized to heat the solar wind used in this paper. We will characterize the additional heating provided by the prescribed distribution of Γ in our solar wind simulation, and argue that surface Alfvén waves damped near the Sun could replace this artificial heating and move the model towards a more physical treatment of the solar environment. For a solar wind with a constant ratio of specific heats γ, the conservation of energy can be written as (Manchester et al. 2004): where p is the thermal pressure, q is the additional heating function, and the energy density is Recent global MHD studies adopt an exponential function for the form of q with several free parameters in order to benchmark the model with observations during solar minima conditions (Groth et al. 2000;Manchester et al. 2004). Substituting Eq. 18 into Eq. 17, and setting time derivatives to zero for a steady solar wind, we find: As discussed at the beginning of this section, there is no heating function q in the simulation used in this paper, and the ratio of specific heats γ is replaced by the effective gamma Γ, Although Γ has both latitudinal and azimuthal dependence below 4R ⊙ , we consider only at the radial variation, and so we replace ∇ by d dr . We assume that we have exactly the same solar wind solution in the two cases we are considering: that of a variable gamma and of an additional volumetric heating function with γ = 5 3 . In order to quantify the amount of heating in the model with variable gamma, we subtract equation 20 from 19: Equation 21 can be written as: Knowing how Γ, p and u r vary along any radial line, and setting γ = 5 3 we can integrate equation 22 between r 1 =1.04R ⊙ and r 2 =4R ⊙ to find the heat input along any field line: This equation gives the heat deposited into the system between the two heights. We compare Q with the flux of damped surface Alfvén waves (Equation 13.) Table 1 provides φ lost and Q for the CHB field lines. The expansion f of the NW line from the simulation has the best match to the observations (5.55 compared to 6.0). The surface Alfvén wave flux along this line, and along the NE lin, is larger than the heating Q by an order of magnitude. The geometrical properties of the SW line also match well with observations, however the wave flux for it (and also the SE line) account for 20 % of the required heating. The distinction between the southern and northern lines is the source region: they come from a stronger magnetic field region. Near an active region, the second term in Eq. 22 (which includes the pressure and radial velocity) is larger than a quiet sun region. Therefore, we expect Q to be larger than the surface Alfvén wave flux along lines from active regions.
As we assumed all of the wave flux goes to heating, this procedure gives an upper limit on the contribution of the damping of surface Alfvén waves along an open magnetic field line to the heating along that line. A random sampling of 7 open field lines in the northern hemisphere with footpoints in the plane of the sky (see Figure 3) yielded φ lost that were on the order, or an order of magnitude larger than the Q.

Conclusions
This work is the first study to look at surface Alfvén waves in a 3D environment without assuming a priori a geometry of the field lines or magnetic and density profiles and strengths. We showed the calculation of the expansion of field lines must be done in a 3D environment. Our calculations show that waves with periods less than 1 hour (frequency greater than 2.8 ×10 −4 Hz) are damped in the region between 1-4 R ⊙ , the region of interest for both solar wind acceleration and coronal heating (Grall et al. 1996). We showed that the quiet sun region will damp surface waves at further distances, so it is more efficient in carrying the wave momentum out into the corona. Surface waves formed on flux tubes with footpoints in an active region will damp closer to the Sun. The required heating from an active region was found to be larger than the damping of surface Alfvén wave flux, therefore another mechanism (such as turbulence) may be the dominant heating in these regions, with surface Alfvén waves contributing approximately 20% of the heating.
We estimated damping of surface Alfvén waves in the border between open and closed field lines at heights 1.04-4 R ⊙ due to the superradial expansion of the field lines. As some of the wave flux would go to the momentum of the wind, we provide an upper limit on the contribution of surface Alfvén waves to the heating of the solar wind. In the region between open and closed field lines, within a few solar radii of the surface, no other major source of damping has been suggested for the low frequency waves we consider here.
Our results demonstrate that it is not necessary to have turbulence in order to heat the solar wind -and that it is imperative to include the physics of surface Alfvén wave damping in solar wind models in order to more physically model the heating. Surface Alfvén waves could also be present in the solar wind, in the flux tube structures said to fill interplanetary space (Borovsky 2008). Another environment which could support these waves are Corotating Interaction Regions (CIRs), due to the inhomogeneity in density present in these structures (Tsubouchi 2009). Both of these topics will be addressed in future works.
It is important to note that this study of waves in a solar wind solution was not self consistent -we did not consider any back effects on the waves from the plasma. We simply tried to estimate if the waves could produce the heating required to create the solar wind solution from the model. In the future we will pursue other damping mechanisms with the goal of incorporating the key mechanisms of wave damping in self-consistently in global MHD models to improve the lower corona.
We would like to thank NASA Ames for the use of the Columbia supercomputer. This research was supported by the NSF CAREER Grant ATM 0747654 and LWS NNGO6GB53G .  Fig. 1 (colors correspond) from 1.04-10 solar radii (Rs). We also show the profiles which correspond to the minimum (dashed line) and maximum (dash-dot line) values of f determined in the observational study by Dobrzycka et al. (1999). We find that f covers a larger range of values compared to the observational study.  Fig.  1 (colors correspond), normalized to the L 0 of the SW line (green) from 1.04-10 solar radii (Rs). Note the plateau in the profiles for lines whose source region on the sun is quiet sun, differing from field lines with footpoints near active regions, whose profiles drop quickly. b) Profiles for the SW coronal hole boundary field line corresponding to different frequencies. From the bottom up to top profile: 3.3 × 10 −1 Hz (dash-dot-dot line); 1 × 10 −2 Hz (dash-dot line); 4.17 × 10 −3 Hz (dot line); 1.67 × 10 −4 Hz (long dash line); 2.8 × 10 −4 Hz (short dash line); 1.5 × 10 −5 Hz (thin solid line); 3.8 × 10 −6 Hz (thick solid line). Waves with frequencies above 2.8 × 10 −4 are appreciably damped below 4Rs. August 17. Γ is specified on the solar surface (shown as white sphere) using the Bernoulli integral, and is interpolated to 1.1 at 2.5 Rs (inner black circle). Above 2.5Rs, Γ varies linearly until 12.5Rs (outer black circle), above which it has the value 1.5. The white lines show the boundaries of grid refinement. .62 Q c ( erg cm 2 s ) 8.9 × 10 3 8.0 × 10 3 2.7 × 10 5 3.1 × 10 5 φ lost d ( erg cm 2 s ) 6.1 × 10 4 6.2 × 10 4 6.4 × 10 4 6.4 × 10 4 a Colatitude of the line -angle measured from the pole to the footpoint on the solar surface.
b Value for the superradial enhancement factor at R=10 R⊙ c Heating calculated along the field line (see section 4.2) d Alfvén wave flux deposited into the wind (see section 4.1)