From pof-edoffice@aip.org Tue Nov 17 15:20:14 2020 Received: from exdb05.ug.kth.se (192.168.32.115) by exdb04.ug.kth.se (192.168.32.114) with Microsoft SMTP Server (TLS) id 15.0.1497.2 via Mailbox Transport; Tue, 17 Nov 2020 15:20:14 +0100 Received: from mx6.kth.se (130.237.48.70) by exdb05.ug.kth.se (192.168.32.115) with Microsoft SMTP Server (TLS) id 15.0.1497.2; Tue, 17 Nov 2020 15:20:14 +0100 Received: from mx6.kth.se (localhost [127.0.0.1]) by mx6.kth.se (Postfix) with ESMTP id 8CDB91C00E4 for ; Tue, 17 Nov 2020 15:20:14 +0100 (CET) X-Virus-Scanned: by amavisd-new at kth.se Received: from mx6.kth.se ([127.0.0.1]) by mx6.kth.se (mx6.kth.se [127.0.0.1]) (amavisd-new, port 10024) with ESMTP id uKNMFdOoIETb for ; Tue, 17 Nov 2020 15:20:11 +0100 (CET) Received: from smtpprod.aip.org (unknown [52.144.53.66]) by mx6.kth.se (Postfix) with ESMTP for ; Tue, 17 Nov 2020 15:20:10 +0100 (CET) Received: from localhost.localdomain (unknown [52.144.53.90]) by smtpprod.aip.org (Postfix) with ESMTP id 14427600BB7E for ; Tue, 17 Nov 2020 09:20:09 -0500 (EST) DKIM-Filter: OpenDKIM Filter v2.11.0 smtpprod.aip.org 14427600BB7E DKIM-Signature: v=1; a=rsa-sha256; c=relaxed/simple; d=aip.org; s=default; t=1605622809; bh=zE40+t5zqlIxTNNtsj4yQgb3fJ03Ii0bUcMIeVXY7m4=; h=Date:To:Subject:From:Reply-To:From; b=jVXcY4V6uUTMD7dhPwCLjlzpT2VVK7VmnY6/rjq/2h6XrDSwHYD9U+HuxKm/AC7y/ F8qbqHuo0f94nRiKNynsEIVwz4mBDrmGOOr2g6Y4w01gfHJdK34I11MRRU/ZMUhaSX HfShQhFB+/aGwlXR+AziUX1Pv7A8c7sMKhuvx4j4= Content-Transfer-Encoding: binary Content-Type: multipart/mixed; boundary="_----------=_16056228091379641"; charset="iso-8859-1" X-Mailer: MIME::Lite 3.030 (F2.84; T1.38; A2.12; B3.13; Q3.13) Date: Tue, 17 Nov 2020 09:20:09 -0500 Message-ID: <0160562280986@d1-pxpweb-02cp.int.aip.org> To: brandenb@nordita.org Subject: Physics of Fluids - Decision Letter: MS #POF20-AR-IFM2020-03460 From: pof-edoffice@aip.org Reply-To: pof-edoffice@aip.org Return-Path: pof-edoffice@aip.org X-MS-Exchange-Organization-Network-Message-Id: 54395aed-5f61-4aa3-c4d4-08d88b03e6da X-MS-Exchange-Organization-AVStamp-Enterprise: 1.0 X-MS-Exchange-Organization-AuthSource: exdb05.ug.kth.se X-MS-Exchange-Organization-AuthAs: Anonymous MIME-Version: 1.0 Status: RO Content-Length: 18993 Lines: 302 --_----------=_16056228091379641 Content-Transfer-Encoding: binary Content-Type: multipart/alternative; boundary="_----------=_16056228091379642" X-Mailer: MIME::Lite 3.030 (F2.84; T1.38; A2.12; B3.13; Q3.13) Date: Tue, 17 Nov 2020 09:20:09 -0500 Message-ID: <6716056228092@d1-pxpweb-02cp.int.aip.org> --_----------=_16056228091379642 Content-Disposition: inline Content-Transfer-Encoding: 8bit Content-Type: text/plain Re: MS#POF20-AR-IFM2020-03460 "Turbulent radiative diffusion and turbulent Newtonian cooling" Axel Brandenburg and Upasana Das Dear Professor Brandenburg, I have now heard from the referees regarding your manuscript; their reports are attached or below. As you will see, the reports point to issues that require clarification and revision. If you feel you can satisfy these reviewers, then please send your revised manuscript, a cover letter that includes an overview of your changes, and a separate point-by-point response to each referee in the form: Response to Referee #m: text of referee's comment your response Response to Referee #n: text of referee's comment your response etc. Upload each reply as a separate file as we may forward each to the referee. Please upload two versions of the new submission. One, the "Article File," should be the final version of the revision and the other, uploaded as "Marked-Up Manuscript," should be the final version showing all changes from the former version. Do not provide a separate markup for each referee. When you are ready to submit your revision, please upload the source files for your revised manuscript and figures. If your paper is accepted, this will quicken its transition to production. Please see the information at the bottom of this decision letter. We expect to receive your revised manuscript by 08-Dec-2020. A later revision may be processed as a new submission, with a new received date and new referees. To submit your revised version, replies to the referees, and other materials, follow: https://pof.peerx-press.org/cgi-bin/main.plex?el=A4E3HIBf4A7EOFV7I3A9ftdP3pTJr1db1NbxBpjYQSdsQY Sincerely, Chunxiao Xu (许春晓), PhD Associate Editor, Physics of Fluids Professor of Fluid Mechanics Tsinghua University Beijing 100084, CHINA ------------------------------------ AIP Publishing 1305 Walt Whitman Road Suite 300 Melville, NY 11747-4300 USA phone: +1-516-576-2343 e-mail: pof-edoffice@aip.org ------------------------------------------------------------------------------ Manuscript PF#POF20-AR-IFM2020-03460: ASSOCIATE EDITOR COMMENTS: To strengthen your case for novelty and relevance, consider more recent fluids papers (last 5 years). Referee Comments: Referee #2 (Comments to Both Author and Editor): The work concerns with test of the thermal transfers inside a turbulent box submitted to temperature wave and under radiative conditions for different optical absorption conditions (from thin to thick optical depth). The paper tends to show how decay of scalar fluctuations evolved as a function of optical depth and turbulence levels. I couldn't support the publication of this work before clearing the followings points : 1) Precisions have to be given to explain the numerical forcing for turbulence : a. What is the form of this forcing ? b. Is the way this forcing is obtained susceptible to modify the results ? 2) Precision have to be given concerning the convergence of the results. What are the criteria chosen to obtain convergence of computational results ? What are the computational time duration versus integral scalar scales ? 3) The size of the box have to be related to the different physical scales (turbulence, temperature ... ) to show, for example, how the kinematic turbulence spectrum is accounted for. 4) Some hypothesis have to be justified : a) Is the viscosity u constant ? b) If yes is it valid for the present temperature range ? c) If no what is the relationship you use to account for ? 5) On P. 5 you have some comments on temperature fluctuation evolutions as : "We clearly see that the temperature equilibrates..." could you support this point of view with a clear criteria linked for example with temperature fluctuation levels in the flow and as a function of the different depth cases ? 6) Results plotted on figure 6 are not very clear to follow, even after reading the reference paper 6, as situation is not the same for the present work : a) Could you explain clearly the condition of the test ? b) For the scalar what is the diffusivity, the temperature conditions, ... 7) Figure 6 compare results from the present work with those of ref 6 in which there is simulated flow with rotation ... is it similar situation and in what way this could be compared ? From my point of view, this work is interesting but some hypothesis and computational conditions are difficult to follow probably due to lack of explanations. This needs to be improve for the reader. Referee #3 (Comments to Both Author and Editor): Review of the manuscript POF20-AR-IFM2020-03460 The present work is devoted to the investigation of influence of turbulent mixing on the decay rate of the temperature perturbations. It is interesting fundamental problem relevant for many applications. Authors should make some amendments to the text or give comments to the following questions before the publishing this work. Generally, speaking about the turbulence one keeps in mind the necessity of the broad band spectrum of initial perturbations but in your work only the growth of single mode perturbations are considered. Why do you think that it is enough for investigation of suggested problem? The situation is worse by the usage of very low Reynolds numbers that restricts perturbations development. Please comment this and clarify the corresponding parts in the text. Section II. On Fig 1 please use different line styles for curves (not only color). It is difficult to use the text in the white-black view. Section III. The section III should be supplemented by a short description of the numerical code. It would be useful to understand what approach do you use for solving basic set of equations. Also the clarification of the model is needed. It is not clear do you solve the radiation transport equation or just an equation of radiative heat conduction. Please provide explicit expression for forcing function f. Its physical meaning is unclear. And finally what do you expect from using more realistic EOS? ------------------------------------------------------------------------------ NOTES FROM THE EDITORIAL OFFICE: * Revised manuscript source files must be in Word or LaTeX/ReVTeX. Replace the current PDF file with an acceptable manuscript source file. * Separate figure files (separate from text and tables) are required for production purposes. Submit a separate figure file for each figure cited in the manuscript, not just one file containing all figures. The allowed file formats for figure files are TIF, PS, EPS, JPEG, or high-quality PDF. Figures may remain embedded in the manuscript. Number your separate figure files as they appear in the manuscript. For example 1, 2, 3. NOTE: DOC or DOCX figure files are not permitted.

This email message and any files transmitted with it contain confidential information. If you are not the intended recipient please notify the sender, delete this email and any attachments from your system, and destroy any copies you have made, electronic or otherwise.
--_----------=_16056228091379642 Content-Disposition: inline Content-Transfer-Encoding: base64 Content-Type: text/html CiAgICAgICAgPEhUTUw+CiAgICAgICAgPGhlYWQ+CiAgICAgICAgICA8bWV0YSBodHRwLWVxdWl2 PSJDb250ZW50LVR5cGUiIGNvbnRlbnQ9InRleHQvaHRtbDsgY2hhcnNldD1pc28tODg1OS0xIj4K ICAgICAgICAgIDxtZXRhIG5hbWU9IkF1dGhvciIgY29udGVudD0ia28iPgogICAgICAgICAgPG1l dGEgbmFtZT0iR0VORVJBVE9SIiBjb250ZW50PSJNb3ppbGxhLzQuNyBbZW5dIChXaW5OVDsgSSkg W05ldHNjYXBlXSI+CiAgICAgICAgPC9oZWFkPgogICAgICAgIDxib2R5IHRleHQ9IiMwMDAwMDAi IGJnY29sb3I9IiNGRkZGRkYiIGxpbms9IiNGRjAwMDAiIHZsaW5rPSIjQ0MwMDAwIiBhbGluaz0i I0ZGMDAwMCI+CiAgICBSZTogTVMjUE9GMjAtQVItSUZNMjAyMC0wMzQ2MCAiVHVyYnVsZW50IHJh ZGlhdGl2ZSBkaWZmdXNpb24gYW5kIHR1cmJ1bGVudCBOZXd0b25pYW4gY29vbGluZyIgQXhlbCBC cmFuZGVuYnVyZyBhbmQgVXBhc2FuYSBEYXMgPGJyPgogPGJyPgpEZWFyIFByb2Zlc3NvciBCcmFu ZGVuYnVyZywgPGJyPgogPGJyPgogSSBoYXZlIG5vdyBoZWFyZCBmcm9tIHRoZSByZWZlcmVlcyBy ZWdhcmRpbmcgeW91ciBtYW51c2NyaXB0OyB0aGVpciByZXBvcnRzIGFyZSBhdHRhY2hlZCBvciBi ZWxvdy4gQXMgeW91IHdpbGwgc2VlLCB0aGUgcmVwb3J0cyBwb2ludCB0byBpc3N1ZXMgdGhhdCBy ZXF1aXJlIGNsYXJpZmljYXRpb24gYW5kIHJldmlzaW9uLiA8YnI+CiA8YnI+CiBJZiB5b3UgZmVl bCB5b3UgY2FuIHNhdGlzZnkgdGhlc2UgcmV2aWV3ZXJzLCB0aGVuIHBsZWFzZSBzZW5kIHlvdXIg cmV2aXNlZCBtYW51c2NyaXB0LCBhIGNvdmVyIGxldHRlciB0aGF0IGluY2x1ZGVzIGFuIG92ZXJ2 aWV3IG9mIHlvdXIgY2hhbmdlcywgYW5kIGEgc2VwYXJhdGUgcG9pbnQtYnktcG9pbnQgcmVzcG9u c2UgdG8gZWFjaCByZWZlcmVlIGluIHRoZSBmb3JtOiA8YnI+CiA8YnI+ClJlc3BvbnNlIHRvIFJl ZmVyZWUgI206IDxicj4KIDxicj4KdGV4dCBvZiByZWZlcmVlJ3MgY29tbWVudCA8YnI+CnlvdXIg cmVzcG9uc2UgPGJyPgogPGJyPgpSZXNwb25zZSB0byBSZWZlcmVlICNuOiA8YnI+CiA8YnI+CnRl eHQgb2YgcmVmZXJlZSdzIGNvbW1lbnQgPGJyPgp5b3VyIHJlc3BvbnNlIDxicj4KZXRjLiA8YnI+ CiA8YnI+CiBVcGxvYWQgZWFjaCByZXBseSBhcyBhIHNlcGFyYXRlIGZpbGUgYXMgd2UgbWF5IGZv cndhcmQgZWFjaCB0byB0aGUgcmVmZXJlZS4gPGJyPgogPGJyPgogUGxlYXNlIHVwbG9hZCB0d28g dmVyc2lvbnMgb2YgdGhlIG5ldyBzdWJtaXNzaW9uLiBPbmUsIHRoZSAiQXJ0aWNsZSBGaWxlLCIg c2hvdWxkIGJlIHRoZSBmaW5hbCB2ZXJzaW9uIG9mIHRoZSByZXZpc2lvbiBhbmQgdGhlIG90aGVy LCB1cGxvYWRlZCBhcyAiTWFya2VkLVVwIE1hbnVzY3JpcHQsIiBzaG91bGQgYmUgdGhlIGZpbmFs IHZlcnNpb24gc2hvd2luZyBhbGwgY2hhbmdlcyBmcm9tIHRoZSBmb3JtZXIgdmVyc2lvbi4gRG8g bm90IHByb3ZpZGUgYSBzZXBhcmF0ZSBtYXJrdXAgZm9yIGVhY2ggcmVmZXJlZS4gPGJyPgogPGJy PgogV2hlbiB5b3UgYXJlIHJlYWR5IHRvIHN1Ym1pdCB5b3VyIHJldmlzaW9uLCBwbGVhc2UgdXBs b2FkIHRoZSBzb3VyY2UgZmlsZXMgZm9yIHlvdXIgcmV2aXNlZCBtYW51c2NyaXB0IGFuZCBmaWd1 cmVzLiBJZiB5b3VyIHBhcGVyIGlzIGFjY2VwdGVkLCB0aGlzIHdpbGwgcXVpY2tlbiBpdHMgdHJh bnNpdGlvbiB0byBwcm9kdWN0aW9uLiBQbGVhc2Ugc2VlIHRoZSBpbmZvcm1hdGlvbiBhdCB0aGUg Ym90dG9tIG9mIHRoaXMgZGVjaXNpb24gbGV0dGVyLiA8YnI+CiA8YnI+CiBXZSBleHBlY3QgdG8g cmVjZWl2ZSB5b3VyIHJldmlzZWQgbWFudXNjcmlwdCBieSAwOC1EZWMtMjAyMC4gQSBsYXRlciBy ZXZpc2lvbiBtYXkgYmUgcHJvY2Vzc2VkIGFzIGEgbmV3IHN1Ym1pc3Npb24sIHdpdGggYSBuZXcg cmVjZWl2ZWQgZGF0ZSBhbmQgbmV3IHJlZmVyZWVzLiA8YnI+CiA8YnI+CiBUbyBzdWJtaXQgeW91 ciByZXZpc2VkIHZlcnNpb24sIHJlcGxpZXMgdG8gdGhlIHJlZmVyZWVzLCBhbmQgb3RoZXIgbWF0 ZXJpYWxzLCBmb2xsb3c6IDxicj4KIDxicj4KPGEgaHJlZj0iaHR0cHM6Ly9wb2YucGVlcngtcHJl c3Mub3JnL2NnaS1iaW4vbWFpbi5wbGV4P2VsPUE0RTNISUJmNEE3RU9GVjdJM0E5ZnRkUDNwVEpy MWRiMU5ieEJwallRU2RzUVkiPmh0dHBzOi8vcG9mLnBlZXJ4LXByZXNzLm9yZy9jZ2ktYmluL21h aW4ucGxleD9lbD1BNEUzSElCZjRBN0VPRlY3STNBOWZ0ZFAzcFRKcjFkYjFOYnhCcGpZUVNkc1FZ PC9hPiA8YnI+CiA8YnI+ClNpbmNlcmVseSwgPGJyPgogPGJyPgpDaHVueGlhbyBYdSAoJiN4OEJC ODsmI3g2NjI1OyYjeDY2NTM7KSwgUGhEIDxicj4KQXNzb2NpYXRlIEVkaXRvciwgUGh5c2ljcyBv ZiBGbHVpZHMgPGJyPgpQcm9mZXNzb3Igb2YgRmx1aWQgTWVjaGFuaWNzIDxicj4KVHNpbmdodWEg VW5pdmVyc2l0eSA8YnI+CkJlaWppbmcgMTAwMDg0LCBDSElOQSA8YnI+Ci0tLS0tLS0tLS0tLS0t LS0tLS0tLS0tLS0tLS0tLS0tLS0tLSA8YnI+CiA8YnI+CiA8YnI+CkFJUCBQdWJsaXNoaW5nIDxi cj4KMTMwNSBXYWx0IFdoaXRtYW4gUm9hZCA8YnI+ClN1aXRlIDMwMCA8YnI+Ck1lbHZpbGxlLCBO WSAxMTc0Ny00MzAwIFVTQSA8YnI+CiA8YnI+CnBob25lOiArMS01MTYtNTc2LTIzNDMgPGJyPgpl LW1haWw6IHBvZi1lZG9mZmljZUBhaXAub3JnIDxicj4KIDxicj4KLS0tLS0tLS0tLS0tLS0tLS0t LS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0t LS0tIDxicj4KIDxicj4KTWFudXNjcmlwdCBQRiNQT0YyMC1BUi1JRk0yMDIwLTAzNDYwOiA8YnI+ CiA8YnI+CkFTU09DSUFURSBFRElUT1IgQ09NTUVOVFM6IDxicj4KVG8gc3RyZW5ndGhlbiB5b3Vy IGNhc2UgZm9yIG5vdmVsdHkgYW5kIHJlbGV2YW5jZSwgY29uc2lkZXIgbW9yZSByZWNlbnQgZmx1 aWRzIHBhcGVycyAobGFzdCA1IHllYXJzKS4gPGJyPgogPGJyPgpSZWZlcmVlIENvbW1lbnRzOiA8 YnI+CiA8YnI+ClJlZmVyZWUgIzIgKENvbW1lbnRzIHRvIEJvdGggQXV0aG9yIGFuZCBFZGl0b3Ip OiA8YnI+CiA8YnI+ClRoZSB3b3JrIGNvbmNlcm5zIHdpdGggdGVzdCBvZiB0aGUgdGhlcm1hbCB0 cmFuc2ZlcnMgaW5zaWRlIGEgdHVyYnVsZW50IGJveCBzdWJtaXR0ZWQgdG8gdGVtcGVyYXR1cmUg d2F2ZSBhbmQgdW5kZXIgcmFkaWF0aXZlIGNvbmRpdGlvbnMgZm9yIGRpZmZlcmVudCBvcHRpY2Fs IGFic29ycHRpb24gY29uZGl0aW9ucyAoZnJvbSB0aGluIHRvIHRoaWNrIG9wdGljYWwgZGVwdGgp LiA8YnI+CiA8YnI+ClRoZSBwYXBlciB0ZW5kcyB0byBzaG93IGhvdyBkZWNheSBvZiBzY2FsYXIg Zmx1Y3R1YXRpb25zIGV2b2x2ZWQgYXMgYSBmdW5jdGlvbiBvZiBvcHRpY2FsIGRlcHRoIGFuZCB0 dXJidWxlbmNlIGxldmVscy4gPGJyPgogPGJyPgpJIGNvdWxkbid0IHN1cHBvcnQgdGhlIHB1Ymxp Y2F0aW9uIG9mIHRoaXMgd29yayBiZWZvcmUgY2xlYXJpbmcgdGhlIGZvbGxvd2luZ3MgcG9pbnRz IDogPGJyPgogPGJyPgoxKSBQcmVjaXNpb25zIGhhdmUgdG8gYmUgZ2l2ZW4gdG8gZXhwbGFpbiB0 aGUgbnVtZXJpY2FsIGZvcmNpbmcgZm9yIHR1cmJ1bGVuY2UgOiA8YnI+CiA8YnI+CmEuIFdoYXQg aXMgdGhlIGZvcm0gb2YgdGhpcyBmb3JjaW5nID8gPGJyPgogPGJyPgpiLiBJcyB0aGUgd2F5IHRo aXMgZm9yY2luZyBpcyBvYnRhaW5lZCBzdXNjZXB0aWJsZSB0byBtb2RpZnkgdGhlIHJlc3VsdHMg PyA8YnI+CiA8YnI+CjIpIFByZWNpc2lvbiBoYXZlIHRvIGJlIGdpdmVuIGNvbmNlcm5pbmcgdGhl IGNvbnZlcmdlbmNlIG9mIHRoZSByZXN1bHRzLiBXaGF0IGFyZSB0aGUgY3JpdGVyaWEgY2hvc2Vu IHRvIG9idGFpbiBjb252ZXJnZW5jZSBvZiBjb21wdXRhdGlvbmFsIHJlc3VsdHMgPyBXaGF0IGFy ZSB0aGUgY29tcHV0YXRpb25hbCB0aW1lIGR1cmF0aW9uIHZlcnN1cyBpbnRlZ3JhbCBzY2FsYXIg c2NhbGVzID8gPGJyPgogPGJyPgozKSBUaGUgc2l6ZSBvZiB0aGUgYm94IGhhdmUgdG8gYmUgcmVs YXRlZCB0byB0aGUgZGlmZmVyZW50IHBoeXNpY2FsIHNjYWxlcyAodHVyYnVsZW5jZSwgdGVtcGVy YXR1cmUgLi4uICkgdG8gc2hvdywgZm9yIGV4YW1wbGUsIGhvdyB0aGUga2luZW1hdGljIHR1cmJ1 bGVuY2Ugc3BlY3RydW0gaXMgYWNjb3VudGVkIGZvci4gPGJyPgogPGJyPgo0KSBTb21lIGh5cG90 aGVzaXMgaGF2ZSB0byBiZSBqdXN0aWZpZWQgOiA8YnI+CiA8YnI+CmEpIElzIHRoZSB2aXNjb3Np dHkgdSBjb25zdGFudCA/IDxicj4KIDxicj4KYikgSWYgeWVzIGlzIGl0IHZhbGlkIGZvciB0aGUg cHJlc2VudCB0ZW1wZXJhdHVyZSByYW5nZSA/IDxicj4KIDxicj4KYykgSWYgbm8gd2hhdCBpcyB0 aGUgcmVsYXRpb25zaGlwIHlvdSB1c2UgdG8gYWNjb3VudCBmb3IgPyA8YnI+CiA8YnI+CjUpIE9u IFAuIDUgeW91IGhhdmUgc29tZSBjb21tZW50cyBvbiB0ZW1wZXJhdHVyZSBmbHVjdHVhdGlvbiBl dm9sdXRpb25zIGFzIDogPGJyPgogPGJyPgoiV2UgY2xlYXJseSBzZWUgdGhhdCB0aGUgdGVtcGVy YXR1cmUgZXF1aWxpYnJhdGVzLi4uIiA8YnI+CiA8YnI+CiBjb3VsZCB5b3Ugc3VwcG9ydCB0aGlz IHBvaW50IG9mIHZpZXcgd2l0aCBhIGNsZWFyIGNyaXRlcmlhIGxpbmtlZCBmb3IgZXhhbXBsZSB3 aXRoIHRlbXBlcmF0dXJlIGZsdWN0dWF0aW9uIGxldmVscyBpbiB0aGUgZmxvdyBhbmQgYXMgYSBm dW5jdGlvbiBvZiB0aGUgZGlmZmVyZW50IGRlcHRoIGNhc2VzID8gPGJyPgogPGJyPgo2KSBSZXN1 bHRzIHBsb3R0ZWQgb24gZmlndXJlIDYgYXJlIG5vdCB2ZXJ5IGNsZWFyIHRvIGZvbGxvdywgZXZl biBhZnRlciByZWFkaW5nIHRoZSByZWZlcmVuY2UgcGFwZXIgNiwgYXMgc2l0dWF0aW9uIGlzIG5v dCB0aGUgc2FtZSBmb3IgdGhlIHByZXNlbnQgd29yayA6IDxicj4KIDxicj4KYSkgQ291bGQgeW91 IGV4cGxhaW4gY2xlYXJseSB0aGUgY29uZGl0aW9uIG9mIHRoZSB0ZXN0ID8gPGJyPgogPGJyPgpi KSBGb3IgdGhlIHNjYWxhciB3aGF0IGlzIHRoZSBkaWZmdXNpdml0eSwgdGhlIHRlbXBlcmF0dXJl IGNvbmRpdGlvbnMsIC4uLiA8YnI+CiA8YnI+CjcpIEZpZ3VyZSA2IGNvbXBhcmUgcmVzdWx0cyBm cm9tIHRoZSBwcmVzZW50IHdvcmsgd2l0aCB0aG9zZSBvZiByZWYgNiBpbiB3aGljaCB0aGVyZSBp cyBzaW11bGF0ZWQgZmxvdyB3aXRoIHJvdGF0aW9uIC4uLiBpcyBpdCBzaW1pbGFyIHNpdHVhdGlv biBhbmQgaW4gd2hhdCB3YXkgdGhpcyBjb3VsZCBiZSBjb21wYXJlZCA/IDxicj4KIDxicj4KRnJv bSBteSBwb2ludCBvZiB2aWV3LCB0aGlzIHdvcmsgaXMgaW50ZXJlc3RpbmcgYnV0IHNvbWUgaHlw b3RoZXNpcyBhbmQgY29tcHV0YXRpb25hbCBjb25kaXRpb25zIGFyZSBkaWZmaWN1bHQgdG8gZm9s bG93IHByb2JhYmx5IGR1ZSB0byBsYWNrIG9mIGV4cGxhbmF0aW9ucy4gVGhpcyBuZWVkcyB0byBi ZSBpbXByb3ZlIGZvciB0aGUgcmVhZGVyLiA8YnI+CiA8YnI+CiA8YnI+ClJlZmVyZWUgIzMgKENv bW1lbnRzIHRvIEJvdGggQXV0aG9yIGFuZCBFZGl0b3IpOiA8YnI+CiA8YnI+ClJldmlldyBvZiB0 aGUgbWFudXNjcmlwdCBQT0YyMC1BUi1JRk0yMDIwLTAzNDYwIDxicj4KIDxicj4KVGhlIHByZXNl bnQgd29yayBpcyBkZXZvdGVkIHRvIHRoZSBpbnZlc3RpZ2F0aW9uIG9mIGluZmx1ZW5jZSBvZiB0 dXJidWxlbnQgbWl4aW5nIG9uIHRoZSBkZWNheSByYXRlIG9mIHRoZSB0ZW1wZXJhdHVyZSBwZXJ0 dXJiYXRpb25zLiBJdCBpcyBpbnRlcmVzdGluZyBmdW5kYW1lbnRhbCBwcm9ibGVtIHJlbGV2YW50 IGZvciBtYW55IGFwcGxpY2F0aW9ucy4gPGJyPgogPGJyPgpBdXRob3JzIHNob3VsZCBtYWtlIHNv bWUgYW1lbmRtZW50cyB0byB0aGUgdGV4dCBvciBnaXZlIGNvbW1lbnRzIHRvIHRoZSBmb2xsb3dp bmcgcXVlc3Rpb25zIGJlZm9yZSB0aGUgcHVibGlzaGluZyB0aGlzIHdvcmsuIDxicj4KIDxicj4K R2VuZXJhbGx5LCBzcGVha2luZyBhYm91dCB0aGUgdHVyYnVsZW5jZSBvbmUga2VlcHMgaW4gbWlu ZCB0aGUgbmVjZXNzaXR5IG9mIHRoZSBicm9hZCBiYW5kIHNwZWN0cnVtIG9mIGluaXRpYWwgcGVy dHVyYmF0aW9ucyBidXQgaW4geW91ciB3b3JrIG9ubHkgdGhlIGdyb3d0aCBvZiBzaW5nbGUgbW9k ZSBwZXJ0dXJiYXRpb25zIGFyZSBjb25zaWRlcmVkLiBXaHkgZG8geW91IHRoaW5rIHRoYXQgaXQg aXMgZW5vdWdoIGZvciBpbnZlc3RpZ2F0aW9uIG9mIHN1Z2dlc3RlZCBwcm9ibGVtPyBUaGUgc2l0 dWF0aW9uIGlzIHdvcnNlIGJ5IHRoZSB1c2FnZSBvZiB2ZXJ5IGxvdyBSZXlub2xkcyBudW1iZXJz IHRoYXQgcmVzdHJpY3RzIHBlcnR1cmJhdGlvbnMgZGV2ZWxvcG1lbnQuIFBsZWFzZSBjb21tZW50 IHRoaXMgYW5kIGNsYXJpZnkgdGhlIGNvcnJlc3BvbmRpbmcgcGFydHMgaW4gdGhlIHRleHQuIDxi cj4KIDxicj4KU2VjdGlvbiBJSS4gPGJyPgpPbiBGaWcgMSBwbGVhc2UgdXNlIGRpZmZlcmVudCBs aW5lIHN0eWxlcyBmb3IgY3VydmVzIChub3Qgb25seSBjb2xvcikuIEl0IGlzIGRpZmZpY3VsdCB0 byB1c2UgdGhlIHRleHQgaW4gdGhlIHdoaXRlLWJsYWNrIHZpZXcuIDxicj4KIDxicj4KU2VjdGlv biBJSUkuIDxicj4KVGhlIHNlY3Rpb24gSUlJIHNob3VsZCBiZSBzdXBwbGVtZW50ZWQgYnkgYSBz aG9ydCBkZXNjcmlwdGlvbiBvZiB0aGUgbnVtZXJpY2FsIGNvZGUuIEl0IHdvdWxkIGJlIHVzZWZ1 bCB0byB1bmRlcnN0YW5kIHdoYXQgYXBwcm9hY2ggZG8geW91IHVzZSBmb3Igc29sdmluZyBiYXNp YyBzZXQgb2YgZXF1YXRpb25zLiBBbHNvIHRoZSBjbGFyaWZpY2F0aW9uIG9mIHRoZSBtb2RlbCBp cyBuZWVkZWQuIEl0IGlzIG5vdCBjbGVhciBkbyB5b3Ugc29sdmUgdGhlIHJhZGlhdGlvbiB0cmFu c3BvcnQgZXF1YXRpb24gb3IganVzdCBhbiBlcXVhdGlvbiBvZiByYWRpYXRpdmUgaGVhdCBjb25k dWN0aW9uLiA8YnI+CiA8YnI+ClBsZWFzZSBwcm92aWRlIGV4cGxpY2l0IGV4cHJlc3Npb24gZm9y IGZvcmNpbmcgZnVuY3Rpb24gZi4gSXRzIHBoeXNpY2FsIG1lYW5pbmcgaXMgdW5jbGVhci4gPGJy PgogPGJyPgpBbmQgZmluYWxseSB3aGF0IGRvIHlvdSBleHBlY3QgZnJvbSB1c2luZyBtb3JlIHJl YWxpc3RpYyBFT1M/ICA8YnI+CiA8YnI+Ci0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0t LS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLS0tLSA8YnI+CiA8YnI+ Ck5PVEVTIEZST00gVEhFIEVESVRPUklBTCBPRkZJQ0U6IDxicj4KIDxicj4KKiBSZXZpc2VkIG1h bnVzY3JpcHQgc291cmNlIGZpbGVzIG11c3QgYmUgaW4gV29yZCBvciBMYVRlWC9SZVZUZVguIFJl cGxhY2UgdGhlIGN1cnJlbnQgUERGIGZpbGUgd2l0aCBhbiBhY2NlcHRhYmxlIG1hbnVzY3JpcHQg c291cmNlIGZpbGUuIDxicj4KIDxicj4KICogU2VwYXJhdGUgZmlndXJlIGZpbGVzIChzZXBhcmF0 ZSBmcm9tIHRleHQgYW5kIHRhYmxlcykgYXJlIHJlcXVpcmVkIGZvciBwcm9kdWN0aW9uIHB1cnBv c2VzLiBTdWJtaXQgYSBzZXBhcmF0ZSBmaWd1cmUgZmlsZSBmb3IgZWFjaCBmaWd1cmUgY2l0ZWQg aW4gdGhlIG1hbnVzY3JpcHQsIG5vdCBqdXN0IG9uZSBmaWxlIGNvbnRhaW5pbmcgYWxsIGZpZ3Vy ZXMuIFRoZSBhbGxvd2VkIGZpbGUgZm9ybWF0cyBmb3IgZmlndXJlIGZpbGVzIGFyZSBUSUYsIFBT LCBFUFMsIEpQRUcsIG9yIGhpZ2gtcXVhbGl0eSBQREYuIEZpZ3VyZXMgbWF5IHJlbWFpbiBlbWJl ZGRlZCBpbiB0aGUgbWFudXNjcmlwdC4gTnVtYmVyIHlvdXIgc2VwYXJhdGUgZmlndXJlIGZpbGVz IGFzIHRoZXkgYXBwZWFyIGluIHRoZSBtYW51c2NyaXB0LiBGb3IgZXhhbXBsZSAxLCAyLCAzLiA8 YnI+Ck5PVEU6IERPQyBvciBET0NYIGZpZ3VyZSBmaWxlcyBhcmUgbm90IHBlcm1pdHRlZC4gPGJy PgogPGJyPgogPGJyPgogPGJyPgo8YnI+Cjxicj4KPGJyPjxicj5UaGlzIGVtYWlsIG1lc3NhZ2Ug YW5kIGFueSBmaWxlcyB0cmFuc21pdHRlZCB3aXRoIGl0IGNvbnRhaW4gY29uZmlkZW50aWFsIGlu Zm9ybWF0aW9uLiBJZiB5b3UgYXJlIG5vdCB0aGUgaW50ZW5kZWQgcmVjaXBpZW50IHBsZWFzZSBu b3RpZnkgdGhlIHNlbmRlciwgZGVsZXRlIHRoaXMgZW1haWwgYW5kIGFueSBhdHRhY2htZW50cyBm cm9tIHlvdXIgc3lzdGVtLCBhbmQgZGVzdHJveSBhbnkgY29waWVzIHlvdSBoYXZlIG1hZGUsIGVs ZWN0cm9uaWMgb3Igb3RoZXJ3aXNlLjxicj48L2JvZHk+CjwvSFRNTD4K --_----------=_16056228091379642-- --_----------=_16056228091379641--