Steadystate forms of channel profiles shaped by debrisflow and fluvial processes
 ^{1}The University of Arizona, Department of Geosciences, GouldSimpson Building, 1040 East Fourth Street, Tucson, Arizona 85721, USA
 ^{2}Department of Geological Sciences and Engineering, University of Nevada, Reno, Reno, NV, 89557, USA
 ^{3}Géosciences Environnement Toulouse (GET), UMR 5563, CNRS/IRD/CNES/UPS, Observatoire MidiPyrénées, Toulouse, France
 ^{4}U.S. Geological Survey, P.O. Box 25046, MS 966, Denver, Colorado 80225, USA
 ^{1}The University of Arizona, Department of Geosciences, GouldSimpson Building, 1040 East Fourth Street, Tucson, Arizona 85721, USA
 ^{2}Department of Geological Sciences and Engineering, University of Nevada, Reno, Reno, NV, 89557, USA
 ^{3}Géosciences Environnement Toulouse (GET), UMR 5563, CNRS/IRD/CNES/UPS, Observatoire MidiPyrénées, Toulouse, France
 ^{4}U.S. Geological Survey, P.O. Box 25046, MS 966, Denver, Colorado 80225, USA
Abstract. Debris flows regularly traverse bedrock channels that dissect steep landscapes, but our understanding of the dominant controls that set rates and spatial patterns of landscape evolution by debris flows is still rudimentary. As a result, much of our understanding of steep bedrock channel networks is derived from application of geomorphic transport laws designed to represent erosion by waterdominated flows. To quantify the link between debrisflow mechanics and steep channel network form, establishment of a geomorphic transport law that quantifies bedrock erosion by debris flows and development of methods capable of handling the transient, nonlocal behavior of debris flows throughout the steep channel network are needed. Here, we propose a landscape evolution model to simulate longitudinal channel profiles that evolve in response to both debrisflow and fluvial processes. The model framework, which includes a methodology to explicitly track spatial variations in bulk debrisflow properties (e.g. flow depth, velocity) along the length of the channel profile, is designed to allow for the exploration of a range of potential debrisflow incision laws. We propose a relationship in which the debrisflow erosion rate is a function of debrisflow depth and channel slope. By comparing the morphology of modeled channel profiles to that typically seen in natural channels, we place constraints on a debrisflow incision law with this general form. Modeled channel profiles are consistent with observations of channel morphology in debrisflowdominated terrain when the debrisflow incision rate is related to local channel slope raised to a power greater than one and approximately linearly related to debrisflow depth. Model results indicate that erosion by debris flows can explain the occurrence of a scaling break in the slopearea curve at low drainage areas and that uppernetwork channel morphology may be useful for inferring catchmentaveraged erosion rates in quasisteady landscapes. These results improve our ability to interpret topographic signals within steep channel networks and provide a general framework for exploring the role of debrisflow erosion within landscape evolution models.
Luke A. McGuire et al.
Status: final response (author comments only)

RC1: 'Comment on esurf202247', Anonymous Referee #1, 06 Oct 2022
The sharp slope inflection in the areaslope relationship observed for loworder channels has long been documented in worldwide topographies, and has been explained as due to dominant debris flow erosion. However, the controls and magnitude of channel head erosion by debris flows have been addressed in a limited manner: direct field measurements of erosion are almost nonexistent, and models are also lacking. McGuire and coauthors attempt to address this second issue by proposing two separate models based on several parameters, and then explore the sensitivity of these models to their different parameters. The main constraint to validating their model is the qualitative observation that the slope of the upper part of the channels increases slowly but continuously to the head of the channel.
The subject matter of this research is appropriate for the journal Earth Surface Dynamics, and the proposed approaches could represent an interesting first step in the direction of quantifying the role of debris flows in landscape evolution. Unfortunately, the way the study is designed and the paper is written does not really accomplish this goal. I would actually suggest that the authors completely reconsider the organization of their paper, including a modification (or deletion) of the processbased model to include the firstorder components that are not considered and yet have a major impact on the shape of the inflection discussed in the preamble.
First, as long as the only proposed validating constraint is the observation that “the slope continues to increase or remain constant as drainage area decreases…”, the whole processbased model, as it is proposed, should be rejected, even if for very high value of alfa this increase becomes so attenuated that it could be confused (in the sense of the R2 criterion used by the authors) with a uniform slope not depending on A. This left me a little confused!
A preliminary simplified analytic exploration of the empirical model (which is very briefly and incompletely done on line 381) would have permitted the authors to identify the important ingredients for the model, by indicating quite clearly what controls the areaslope relationship along the channel heads (i.e. for A < Adf). Considering the erosion equation (eq. 4), and equation (13), the expression for “tp” (eq 14) and assuming as a first approximation that capital theta is uniform and close to 1 (shear stress >> tauy) along the head channel reaches, we can derive such relation at steady state.
S depends on uplift and drainage area according to a power relation: S proportional to A^N, with
N = (beta/3.(gamma.c2 – b) + gamma.(1c2))/(alfa – beta/3)
The sign of this exponent N controls the slope of the S=f(A) relationship for channel heads. For explored values of alfa >= 2, the denominator is always positive so that the main controlling parameter appears to be the numerator, and among others the sign of (gamma.c2 – b) modulated by beta. We immediately see that if this term is positive then the slope is constantly decreasing downstream. In contrast if this term is negative then the downstream slope increase observed on fig. 2 and 3 becomes possible. If c2 is fixed, the most fundamental parameters are gamma and b. In other words for gamma =0, for the empirical as well as probably for the process based model, the downstream decrease in erosive efficiency (for a uniform channel slope) is due to the channel widening (parameter b) that induces a decrease of the flow thickness h. If gamma is not zero, then there is a critical value for which the slope trend reverses (for gamma larger than b/c2 according to the authors, but in fact for gamma larger than beta.b/3/(1 + (beta /31).c2) ).
Once these two main influences on the sign of the slope of S=f(A) have been identified, the one due to the widening of the channel and the one due to the increase in the volume of debris flowing downstream, we must ask ourselves:
 if they correspond to a reality;
 if so, if they are well taken into account by the model:
To the first question, one can notice that the parameter b is given for the fluvial domain, but that its implicit transposition to the debris flow domain, as done in this article, has no theoretical or empirical basis. Insofar as this debris flow eroded domain behaves differently from the fluvial domain, the transposition is difficult to justify. That an important trend in the model results is controlled by a parameter that is unknown and uncalibrated is quite problematic. Furthermore, as described below, the assumption of w>>h (although not made explicit in the paper) and of a rectangular channel is another problem associated with how w = f(A, M) can be injected into the equations. Regarding the increase in the volume or frequency of debris flows downstream, one need only look at Fig. 2 of Stock and Dietrich (2003) to see that the number of debris flow sources in the contributing basin of a given point will increase downstream, more or less in proportion to the area drained. Taking this increase into account is essential to any model looking at the longterm evolution of the channel profile.
To the second question, we can notice that the processbased model does not include this essential element. This poses a double problem: firstly if we want to compare the performances of the two models, the boundary conditions must be the same (the addition of sediment downstream can be seen as a boundary condition), and more importantly if it is an essential element to the results, it must be implemented (below, I suggest to the authors a quick way to take it into account without needing to modify the core of their equations). In other words, the processbased model is unnecessarily complicated in some aspects while it does not include first order elements.
Given these two deficiencies, it seems to me that the proposed models are for the moment of little use to the community in that some important ingredients are missing and in that these models do not clearly pass a validation or refutation criterion, so that it is impossible to say whether or not these models are suitable to reproduce reality.
Moreover, the architecture of the paper should be modified. It seems to me that a clearer and more rational approach from the point of view of the construction of a physical model would be schematically the following:
1. What are we trying to demonstrate or test? A spatially variable model of instantaneous erosion? An erosion model representative of the long term geometry at equilibrium (if this notion means anything on slopes affected by landslides)?
2. What are the constraining observables to validate or invalidate the models? In the submitted study, if I understand correctly the only constraining observable, presented just in a qualitative way is the fact that in general, past the fluvial/debris flows transition the slope continues to increase going towards the source. This constraint being unique, it is essential to be clear on this constraint. Is this observation general? Or is it just observed for 3 drainages in the San Gabriel Mtns (fig. 1)? It would be helpful to offer a minisynthesis of observations made on this topic in the literature. And to add quantitative criteria (e.g. the ratio between the slope at the source (Sch) and the slope at the transition (S(A=Adf)), or another criterion quantifying whether the slope remains stable or continues to increase above the transition A=Adf). On this point of quantification it is essential to know if the slope continues to increase as suggested by the authors. If so, as said before, this systematically disqualifies the processbased model that predicts an increase in the downstream slope between Ach and Adf regardless of the values of alfa and beta.
3. To build the model, one needs to keep the essential elements (as for a Taylor expansion, do we keep all the details at order 1 (there is no point in keeping terms of order 2 if all the terms of order 1 are not kept). In the absence of a theoretical framework allowing to make this choice, one can at least define, given the points 1 and 2, what are the elements of the model that it is essential to keep. I understand that it can be complex to introduce into the equation (6) an aggregation term (M increasing downstream) of the sediments (and of its momentum) during downstream transport, but it is on the other hand extremely easy to conceive just a multiplicative term in the frequency of passage of the debris flows at a given point, which increases according to the drained area (and to the number of upstream talwegs likely to generate debris flows departures) _ this is equivalent to introduce a “kdf” that would depend linearly (or not) on A.
4. Propose in particular for a simplified model like the empirical model here a first simplified analytical resolution to predict the main trends. In the present study, given this analysis highlighting the role of gamma as a parameter conditioning the increase or reduction of A downstream, the phenomenon carried by the gamma parameter cannot be neglected or dismissed. It must be taken into account. At this stage, the authors in their study should have resumed their model, added this aggregation to the processbased model, and proposed a new model (i.e. discard the old model which can be considered as a first draft) and only talk to us about this last model.
5. Verify or deepen these first conclusions using the numerical simulation. For the "empirical" model, the simulation will allow us to take into account the capital theta term and to have an analysis based on an unapproximated solution.
6. Possibly propose a more advanced model if the empirical model does not allow to account for the observables.
Other issues :
 I found in several equations some problems with the dimensions that are not respected; because I did not check everything in detail, I encourage the authors to recheck all the equations. There is also a vagueness about the volume of debris flow and how it is introduced for the processbased model. To be corrected.
 Why are the ranges of exploration of the parameters external to the model (M0, kdf, ke ...) not the same for the two models? If we want to compare the performances and predictions of the two models, it seems to me obvious to explore the same ranges of values.
 If we want to model the landscape, then it is required to be conservative with respect to the sediments. This is indirectly addressed in the discussion through the coupling between U and kdf , but it must be done more rigorously (especially since it is simple to do). For instance (lines 339, 356), the choice of the relations between U and kdf is totally arbitrary, and is not even the same between the two models (this choice is not trivial because it will condition the subset of orange points and the slope of the relation Sdf=f(U) for this). For example, for the process based model, increasing the uplift rate by a factor 10 leads, given the chosen coefficients within the inequality, to vary kdf by on average a factor 2. In theory, and excluding a small proportion of material exported by other processes ( wet ravelling, subfluvial process? ), an increase of erosion rate by a factor 10 should lead to an increase of the debris flow frequency by a factor 10 (assuming that their volume remains constant).
 It seems to me that in order to reproduce a long term geometry, introducing a temporal distribution of debris flows could be necessary. Indeed, the authors rely for the fluvial part on the relation proposed by Lague (2014). It seems to me that one of the main conclusions of this study is that the exponents of the law E=f(S,A) depend strongly on the distribution of floods because the instantaneous incision law includes a threshold (tauC) below which erosion is zero. For debris flows, since there is also a threshold for the motion onset or efficiency of erosion (tau_y), one can anticipate that the resultant of the mean law will be sensitive to the combination of a threshold and an event distribution with small events traveling little distance because h and tau will be small), and that this may impact the position of Adf, as well as the shape of the transition between the two domains which will be more gradual. In other words, it is again a matter of trying to be consistent: as the problem (and in particular the transition zone) depends on the law of river incision downstream and debris flow upstream, it is important to include the same level of detail in the models on both sides.
 I would suggest adding a schematic graph describing the processbased model, and (in appendix?) one or more results of the propagation of a debris flow downstream as simulated by the processbased model.
Figure 1 caption : add « (eq. 17) » to link the equation to the text. Indicate the projection system (UTM zone ??). I tried to look at the location of these points but it does not correspond to a drainage basin that can be unambiguously identified)
Figure 1: add the P value for ach fit
Line 68: would it be possible to indicate another reference, i.e. other than this PhD thesis that cannot be easily accessed ?
Line 111: those values seem to me quite arbitrary. Why this choice? In addition, the ratio ms/ns=0.6 seems a bit high compared to classical curvature parameter values of 0.40.5.
Line 114: I would suggest to provide a number to this equation, and to discuss more at length the choice of the parameters, and in the discussion the implications of this choice.
Line 126 and Eq (3): where this equation coming from? It needs to be explained and justified. This relation is not detailed at all and refers to a thesis that is not readily available online and to a work that has not been peer reviewed. It is impossible for me to judge its relevance in these conditions, and it seems essential to me to publish beforehand or to include in this paper the developments proposed in this PhD thesis.
Line 127: for reasons given above (and to justify/discuss the sensitivity to uplift rate), it would be more appropriate to display Fdf explicitly instead of hiding it in kdf.
Line 142 (eq. 4): this equation is not homogenous. Either some terms are missing (like the frequency of debris flows), or the kdf units (as given in table B2 to B6) is incorrect
Line 153: “in a rectangular channel” This is a major hypothesis. As much a river channel constrained by its banks or in a canyon can possibly present a rectangular section, as much an ephemeral channel head presents, for what I saw in the nature, a rather widened or prismatic shape. This choice was made for simplicity I assume, but it would be necessary to discuss the adequacy of this assumption and in the discussion whether having a wider channel would change the results.
Line 156 (eq. 6): this equation contains several errors.
The 3^{rd} term on the left hand side is not homogeneous. I assume it is rather gz.h^2
I assume that gx (1rst term on the right hand side) has to be replaced by the projection of the weight onto the channel sloping direction (otherwise, gx=0); and similarly, gz has to be replaced by the projection of the weight onto the direction normal to the sloping channel bed.
Line 187: “introducing this effect … is beyond the scope of this study”. This sentence is quite paradoxical: why do you decide not to incorporate this effect in the process based model, and to do so in the empirical model? If you want to compare the performance of the two models, then you need to consider equivalent boundary conditions and hypothesis on flow volumes.
Again I presume that incorporating this effect in the eq. (6) is uneasy. However, one can easily play with the frequency of debris flows to introduce this dependence (linear or by a power relation with an exponent gamma’ between 0 and 1) to the drainage area. In that case, you should do it similarly for the two models (i.e. not consider the relation M=M0.A^gamma for the empirical model, and saying/demonstrating that you will capture the two effects with only one process)
Line 194198: this part was not clear to me until I realized that there is no distribution of the volumes of debris flow but always the same one running through the channel. Did I understand correctly?
Line 206: this equation seems to me oversimplified: first one should use the hydraulic radius instead of h, except if one can demonstrate that w>>h; second for steep slopes, S should be replaced by sin(theta) with theta the slope angle. The more exact equation should be first written and then the potential simplification justified
Line 210: “we specify debris flow volume at each grid cell”. Do you mean “passing through each grid cell ”?
Line 211: how A is expressed ? in m2 ?
Line 225 (eq 13): where is the 10^6 factor in front of A. Are A units now km2?
Line 305: “some parameter combinations …”: some ? No, ALL parameter combinations according to fig.2 for which Smax is always strictly larger than Sch.
Line 308: “… is inconsistent with observations that indicate slope continues to increase or remain constant as drainage area decreases…” . In other words, given above remarks, the whole processbased model should be rejected … as long as it does not include a downstream increase of the volume or of the frequency of debris flows.
Lines 331, 332: those conclusions are a bit obvious (except on the relation between U and Adf). No need of doing numerical simulations for this.
Line 364: replace kdf by gamma within the inequality. Again the choice of a coefficient 0.5 seems quite arbitrary. In addition, and in contrast with the DF frequency, it remains unclear to me why this gamma parameter should be modified with U.
Line 376: “data and numerical experiments presented here are not capable of differentiating… although cases where alfa < 3 and beta > 2 generally perform poorly”. The authors are quite honest and objective in this sentence. They should start from this sentence, instead of introducing the section insisting on the fact that McCoy’s (2012) model with alfa=6 and beta =1 perform well. It seems to me that present study does not permit to reject this model, but neither does it validate it.
Line 407408: This is obvious: from the moment when, by definition of equation (17), Sdf is defined where the slope becomes constant and deviates from the fluvial relation S=f(A), it goes without saying that Sdf becomes disconnected from any parameterization of the fluvial law (except if ms is close to 0).
Line 418: is Penserini et al. (2017) the only paper that tested the relation between channel head slope and uplift rate? Have the authors checked the literature in the whole US, Italy, Taiwan, HimalayaTibet, etc ?
Line 423: ok for the regression in fig. 10b but in contrast the difference in fig. 7b does not seem major between orange and blue points.
Lines 445446: these lines are redundant with lines 418. The whole discussion should be condensed on these points.
Line 457: “the channel width scaling, b, may … exert control over the long term channel”. I would rather say that this unconstrained parameter has a primary role in the fact that the slope increases downstream until ~Adf instead of slightly decreasing.
Lines 476, 487: “the landscape evolution model presented here …”. This model cannot be called a landscape evolution model because it is 1D and, above all, does not conserve water or sediments. Introducing progressive aggregation of larger sediment supply as we go donwstream in order to respect steady state erosion of the landscape would be the minimum. The introduction of gradual aggregation of larger sediment fluxes as one moves downstream (whatever it I achieved playing with M or Fdf) in order to respect steadystate landscape erosion would be the minimum requirement in that direction.
Line 487: “demonstrate” should be replaced by “propose”
Appendix A: Given that many parameters are jut arbitrary (for example Deff) , I don’t see the point to describe this section since it is already done in Lague (2014). But if the authors prefer to keep that section for the reader, then the instantaneous incision law should be explicitly described or written.
Line 503: if Rc is a runoff, it should have units (m or m/yr)
Line 504: the equation should be provided with a number (A1 ?) and t should be subscripted into "kt".
Table B3: why M0 is not varied among the different parameters?
Tables B3 and B5: Problem of units for ke
Table B3 and B4: I would suggest putting in a different table the fluvial and forcing parameters, which are common to the two models (U, M0, ke)
Table 5: U is given as constant whereas it is supposed to vary over a certain range

RC2: 'Comment on esurf202247', Alexander Densmore, 24 Nov 2022
This is an interesting and timely manuscript that seeks to develop an approach for modelling the combined effects of debrisflow and fluvial incision on river long profiles. Debris flows have long been recognised as important agents of erosion and sediment transport in many mountain catchments, but they have typically been left out of attempts to model channel erosion or landscape evolution. The authors have taken some initial steps toward that goal. The manuscript is highly relevant to the journal and will, I think, be of interest to the journal readership.
The manuscript is wellwritten and wellpresented overall, but I do have some comments on the text and figures. Most of these are fairly minor and should be easy for the authors to address. One more substantive comment is that I was surprised to see that neither the processbased nor the empirical model conserve mass, and only the empirical model considers flow volume variation downstream (although this is imposed as being monotonic). Work in the Illgraben catchment and elsewhere has shown that flows can both lose and gain volume downstream, so while the imposed rule from Santi and Morandi (2013) is certainly a place to start, it would be good to see a little more context around its usage. More importantly, I wondered about comparing the two models given that one assumes the flow volume is uniform downstream and the other does not.
The introduction, while clear and pretty easy to follow, lays out a few different motivations for the work that don’t necessarily all track through the rest of the manuscript. I think this could be streamlined and focused on what the authors are actually doing here. For example, the mention of the need to ‘identify robust topographic signatures of debrisflow erosion’ isn’t something that is addressed here – instead, they are taking a single measure (slope increases monotonically upstream but at a decreasing rate, as in Fig 1) as that signature. It would have been good to be more clear about this up front. Fig 1 is cited as an example of this, but it’s not clear how widespread that morphology is; a parameter A_df and an equation are introduced in the caption but aren’t actually described in the text until p. 10, which could be confusing for the reader. Elsewhere in the intro, there is a goal (lines 8688) which isn’t really clearly motivated at that point in the manuscript, and a separate set of objectives (9197), but then there are two other goals on lines 239242 that overlap with the third and fourth objectives. I’d encourage the authors to restructure the introduction to keep the focus on what they are going to do here (e.g., while I agree that flow frequency is critical as mentioned on lines 7880, that’s not something they address), and to motivate the model comparison that is at the heart of this manuscript.
Some more specific comments by line number:
line 2: ‘rates and spatial patterns of landscape evolution by debris flows’ is ambiguous – should this be ‘…of erosion by debris flows’?
3640: these sentences are written as if these are two different concepts, but aren’t they equivalent?
45: that identification has (apparently) already been made in line 34. This is repeated again in lines 4950
50: here and throughout the manuscript, I would suggest using ‘rock uplift rate’ consistently. There are also places where U is variously used for ‘uplift rate’ or just ‘uplift’, and again I think this needs to be made consistent
7173: while I agree, I think this sentence is also missing the idea that this will happen over multiple flows which themselves are drawn from distributions of volume and flow properties, if we are interested in landscape evolution. This sentence could be read as being about properties in a single flow that’s traversing the landscape
79: I think this should read ‘For example, the frequency…has been shown to be a key factor’
130: given that flow volumes and properties are not constant from flow to flow but follow distributions, I’m not sure what is meant by a ‘representative’ flow. I think it’s really important to be explicit that eqn 3 is defined for a single flow, and that it is being applied over a series of flows that are assumed (rightly or wrongly) to be identical. That’s a really restrictive assumption and I think it needs to be made more obvious. The authors are later clear about how future work could use these distributions (lines 235237), which is great.
140: again this is assuming that h is constant for a given channel location in a single flow. And given that this is a representative value for h rather than the true flow thickness over time (as used in eqn 3) I wondered whether a different symbol would make sense…
167: this is potentially confusing because later D is allowed to vary – not sure why a single value is specified here
184187: our work at the Illgraben (Schuerch et al. 2011 Geology) documented flow volume variations with distance downstream, both positive and negative as flows traversed the lower part of the catchment and the fan
187189: in other words, mass is not conserved, right?
195199: I think I followed this, but it could perhaps be more clearly explained
250266: this partly repeats text in the intro, but this is actually clearer and introduces eqn 17 which has already been shown. I think this text should be merged with the intro so that Fig 1 can be better understood
274: up to here the tense has been present (We assess… we compute), but here it changes to past. This should be kept consistent
272273: I don’t disagree with this criterion… but it’s kind of hidden here, despite the fact that this becomes the primary way in which the authors accept or reject model runs. I think this needs to be highlighted (perhaps in the intro where they are describing what they are trying to match)
277: parameter k_e is introduced here but eqn 2 is in the form of K – it’s not obvious where k_e has come from. A reference to appendix A might help
288: I think I missed the flow frequency – is there a flow every year? Or every timestep?
327: ‘of the steadystate channel profiles’ – I’m not sure if this is referring to the model results or to observations
328: I think this should be ‘minimum drainage area’?
336: ‘increases with rock uplift rate’. More broadly, while I agree with the overall sense of the argument here and this is certainly a reasonable supposition (all else being equal), I’m not sure what is gained by exploring a single, arbitrary relationship between U and k_df. This might just need some more contextual information. Flow frequency should also depend very strongly on where you are in the catchment…
343: I don’t think the ‘e.g.’ makes sense here, because k_df is explicitly defined as the product of an erodibility and flow frequency
350: ‘rock uplift rate U’
375: I’m not sure what is meant by ‘infrequent instances’ – is this referring to individual numerical experiments in the sensitivity tests, or localised parts of the profile within a single experiment, or…?
381: if E_df needs to decrease slightly with A, why does that imply that h must increase with A? That seems to run counter to eqn 4
383: reference to flow discharge is potentially confusing here, because gamma has been defined in terms of downstream changes in flow volume, not discharge. I agree that they might be related, but that relationship isn’t necessarily simple (or the same for all flows)
398: ‘rock uplift rate’
406: I’m a little confused by this leading statement – isn’t this conceptual model what has been assumed? In which case, how can the results be seen as supporting this conceptual model? I suppose what the authors are saying is that there are parameter sets for which this assumed model form can reproduce aspects of observed long profiles – that’s a more restrictive statement (which they make elsewhere). That doesn’t rule out other conceptual models which might also reproduce those long profile aspects, of course
472: because we are considering landscape evolution, then flow volume will change not just by sediment entrainment from the bed and banks but also by bedrock erosion
479: ‘where changes in flow volume can be neglected’ – I’m not sure when that would ever be the case, given that real flows have continuouslyvarying downstream lag rates which can be both positive and negative (and can both erode and deposit within a single channel cross section)
482485: that’s true, although there isn’t much mention throughout of t_p in eqn 4 – this seems like a pretty big unknown if the goal is to model channel erosion over kyrMyr time scales. I guess this comes back to the idea of a ‘representative’ debris flow, which elsewhere the authors also refer to as a ‘characteristic’ flow, and what that means
487: I’m not sure I’d call this a landscape evolution model – it’s really a model of channel profile evolution
Appendix A: D_eff has units of m which should be repeated here
Fig 1: the equation for the bestfit curves is going to be confusing for the reader because it doesn’t show up again in the text until p. 10 – as noted above I suggest moving that material to the intro.
Fig 4: the panels here seem to show the same thing as Fig 2 and don’t match the caption.
Fig 5,8: I think it would be useful to include the units for each parameter on the axis labels
Fig 6,9: again it would be useful to include the units for each parameter, either in the legend or caption
Fig 7,10: ‘Uplift’ should be ‘Rock uplift rate’ on the xaxis, and the units are given in m/kyr here but in m/yr in most other parts of the manuscript; the same comment applies to Fig 10.
Luke A. McGuire et al.
Luke A. McGuire et al.
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