<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AJAC</journal-id><journal-title-group><journal-title>American Journal of Analytical Chemistry</journal-title></journal-title-group><issn pub-type="epub">2156-8251</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajac.2014.516122</article-id><article-id pub-id-type="publisher-id">AJAC-51724</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Fundamental Open Questions on Engineering of “Super” Hydrogen Sorption in Graphite Nanofibers: Relevance for Clean Energy Applications
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ury</surname><given-names>S. Nechaev</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Alp</surname><given-names>Yürüm</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Adem</surname><given-names>Tekin</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Nilgün</surname><given-names>Karatepe Yavuz</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yuda</surname><given-names>Yürüm</given-names></name><xref ref-type="aff" rid="aff5"><sup>5</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>T.</surname><given-names>Nejat Veziroglu</given-names></name><xref ref-type="aff" rid="aff6"><sup>6</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Nanotechnology Research and Application Center, Sabanci University, Istanbul, Turkey</addr-line></aff><aff id="aff6"><addr-line>International Association for Hydrogen Energy, Miami, USA</addr-line></aff><aff id="aff5"><addr-line>Faculty of Engineering and Natural Sciences, Sabanci University, Istanbul, Turkey</addr-line></aff><aff id="aff1"><addr-line>Bardin Institute for Ferrous Metallurgy, Moscow, Russia</addr-line></aff><aff id="aff4"><addr-line>Energy Institute, Istanbul Technical University, Istanbul, Turkey</addr-line></aff><aff id="aff3"><addr-line>Informatics Institute, Istanbul Technical University, Istanbul, Turkey</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Yuri1939@inbox.ru(USN)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>11</month><year>2014</year></pub-date><volume>05</volume><issue>16</issue><fpage>1151</fpage><lpage>1165</lpage><history><date date-type="received"><day>15</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>31</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>16</day>	<month>November</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Herein, some fundamental open questions on engineering of “super” hydrogen sorption (storage) in carbonaceous nanomaterials are considered, namely: 1) on thermodynamic stability and related characteristics of some hydrogenated graphene layers nanostructures: relevance to the hydrogen storage problem; 2) determination of thermodynamic characteristics of graphene hydrides; 3) a treatment and interpretation of some recent STM, STS, HREELS/LEED, PES, ARPS and Raman spectroscopy data on hydrogensorbtion with epitaxial graphenes; 4) on the physics of intercalation of hydrogen into surface graphene-like nanoblisters in pyrolytic graphite and epitaxial graphenes; 5) on the physics of the elastic and plastic deformation of graphene walls in hydrogenated graphite nanofibers; 6) on the physics of engineering of “super” hydrogen sorption (storage) in carbonaceous nanomaterials, in the light of analysis of the Rodriguez-Baker extraordinary data and some others. These fundamental open questions may be solved within several years. 
  
 
</p></abstract><kwd-group><kwd>Hydrogen “Super” Sorption (Storage)</kwd><kwd> Graphenes</kwd><kwd> Carbon Nanotubes</kwd><kwd> Graphite Nanofibers</kwd><kwd> A Breakthrough Hydrogen Storage Nanotecnology</kwd><kwd> Clean Energy Applications</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Hydrogen is currently one of the most promising “green” fuels, owing to the fact that its gravimetric (mass) energy density of 142 MJ/kg (39.5 kWh/kg), (<xref ref-type="fig" rid="fig1">Figure 1</xref>, [<xref ref-type="bibr" rid="scirp.51724-ref1">1</xref>] ) exceeds that of petroleum (oil) by a factor of three and that the product of its combustion is water vapor. On the other hand, the volumetric (volume) energy density of molecular gaseous hydrogen at 1 bar pressure is lower by several orders than that of oil (<xref ref-type="fig" rid="fig1">Figure 1</xref>, [<xref ref-type="bibr" rid="scirp.51724-ref1">1</xref>] ), but it can exceed the oil quantity at megabar pressures (<xref ref-type="fig" rid="fig1">Figure 1</xref>, [<xref ref-type="bibr" rid="scirp.51724-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] ). In light of this, the issue of finding systems and materials for a compact and energy efficient hydrogen storage assumes a primary importance. The known data on volumetric (volume) and gravimetric (mass) energy densities for different energy carriers [<xref ref-type="bibr" rid="scirp.51724-ref1">1</xref>] are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The additional symbol (the red circle) corresponds to the analytical data [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] on the molecular solid hydrogen intercalated into the hydrogenated graphite nanofibers (GNFs); those are related to the extraordinary data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] (being under consideration in this paper). As is noted in a number of studies, for instance in the recent review [<xref ref-type="bibr" rid="scirp.51724-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref14">14</xref>] , hydrogen-based fuel cells are promising solutions for the efficient and clean delivery of electricity. Since hydrogen is an energy carrier, a key step for the development of a reliable hydrogen-based technology requires solving the issue of efficient storage and transport of hydrogen. During the last few decades several proposals based on the design of advanced materials such as metal hydrides and carbon structures have been made to overcome the limitations of the conventional solution of compressing or liquefying of hydrogen in tanks.</p><p>Nevertheless, none of the proposed systems, with the exception of the nobody reproduced extraordinary experimental data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] and the related analytical data [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] , are currently offering the required performances for the on-board hydrogen storage in fuel-cell-powered electrical vehicles [<xref ref-type="bibr" rid="scirp.51724-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref16">16</xref>] . The performances are usually formulated in terms of hydrogen storage gravimetric (mass) and volumetric (volume) capacities (<xref ref-type="fig" rid="fig2">Figure 2</xref>, [<xref ref-type="bibr" rid="scirp.51724-ref17">17</xref>] ) and control of adsorption/desorption processes, particularly, relevance to so called “reversibility” of the stored hydrogen. Therefore the problem of hydrogen efficient storage remains so far unsolved and it continues to represent a significant bottleneck to the advancement and proliferation of fuel cell and hydrogen technologies [<xref ref-type="bibr" rid="scirp.51724-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref19">19</xref>] .</p><p>It is shown [<xref ref-type="bibr" rid="scirp.51724-ref17">17</xref>] , with regards to the known achievements, that the US Department of Energy (DOE) targets for the on-board hydrogen storage systems in fuel-cell-powered vehicles [<xref ref-type="bibr" rid="scirp.51724-ref15">15</xref>] , relevant to gravimetric (mass) and</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Data on volumetric (volume) and gravimetric (mass) energy densi- ties for different energy carriers</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x6.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Correlation between volume and mass of hydrogen densities of various materials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x7.png"/></fig><p>volumetric (volume) storage densities (capacities) of “reversible” hydrogen for 2010 (6.0 mass% H<sub>2</sub> (of the system mass), 45 kg (H<sub>2</sub>)/m<sup>3</sup> (system)) and for 2015 (9.0 mass% H<sub>2</sub> (of the system mass), 81 kg (H<sub>2</sub>)/m<sup>3</sup> (system)). These values are higher than the targets established by the E.U and/or Japan. The additional symbol (the large red circle) corresponds to the analytical data [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] on the molecular solid hydrogen intercalated into the hydrogenated graphite nanofibers (GNFs); those are related to the extraordinary data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] (being under consideration in this paper). The 2017 targets [<xref ref-type="bibr" rid="scirp.51724-ref16">16</xref>] are of 5.5 mass% H<sub>2</sub> (of the system mass) and 40 kg (H<sub>2</sub>)/m<sup>3</sup> (system). As has been noted in [<xref ref-type="bibr" rid="scirp.51724-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref19">19</xref>] : 1) “… to realize a compact and energy efficient hydrogen storage is a key technology” [<xref ref-type="bibr" rid="scirp.51724-ref18">18</xref>] ; 2) “… breakthroughs in hydrogen densities are strongly required” [<xref ref-type="bibr" rid="scirp.51724-ref18">18</xref>] ; 3) it is necessary “to find a breakthrough technology” [<xref ref-type="bibr" rid="scirp.51724-ref19">19</xref>] .</p></sec><sec id="s2"><title>2. Some of the materials under study in CoE’s</title><p>There are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref> the prognosis data [<xref ref-type="bibr" rid="scirp.51724-ref18">18</xref>] (amended in January 2011) on market entry of fuel cell powered vehicles (FCVs) and hydrogen charging stations. Particularly, it is shown that year 2015 can be related to the target commercialization start of FCVs to general public (see further shown Items 6 and 7—the Toyota announcement—2014), and Year 2025—to an increase numbers of FCVs and hydrogen stations based on profitable business. As is also shown (<xref ref-type="fig" rid="fig3">Figure 3</xref>, [<xref ref-type="bibr" rid="scirp.51724-ref18">18</xref>] ), the present time is a very suitable (in the plan of the market entry prognosis) for such a developments. In this connection, it’s also expedient to note about a number of communications of 2013-2014 (in Internet) on the nowadays market situation, relevance to fuel-cell electrical vehicles (FCVs) and hydrogen charging stations, for instance the following.</p><sec id="s2_1"><title>2.1. Hyundai’s fuel-cell vehicle Could Be a massive success. The Motley Fool</title><p>Oct. 24, 2013: Hyundai isn’t the only manufacturer in the race for FCVs. Toyota Motors, Daimler’s Mercedes-Benz, BMW, and a number of other car companies have spent billions in fuel-cell technology, and are all competing to see who can be the first to market with a consumer-friendly FCV.</p></sec><sec id="s2_2"><title>2.2. Hydrogen and Fuel Cells: GM—Honda Collaboration on Next-Generation Fuel Cell Technologies (03.07.2013)</title><p>(http://www.netinform.net/h2/Aktuelles_Detail.aspx?ID=3285.) Goal is commercially feasible fuel cell and hydrogen storage in 2020 time frame.</p><p>On July 2, 2013: General Motors (NYSE: GM) and Honda (NYSE: HMC) announced a long-term, definitive master agreement to co-develop next-generation fuel cell system and hydrogen storage technologies, aiming for the 2020 time frame. The collaboration expects to succeed by sharing expertise, economies of scale and common sourcing strategies. Source: www.gm.com.</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The prognosis data on market entry of fuel cell powered vehicles and hydrogen charging stations</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x8.png"/></fig></sec><sec id="s2_3"><title>2.3. Ballard signs long-term engineering services contract to advance Volkswagen AG Fuel Cell Automotive Research Program Ballard Power</title><p>Mar. 7, 2013: Ballard Power Systems has announced signing of an agreement with Volkswagen Group for a major Engineering Services contract to advance development of fuel cells for use in powering demonstration cars in Volkswagen’s fuel cell automotive research program. The contract term is for 4 years, with an option for an extension. The expected contract value is in the range of $60 - $100 million.</p></sec><sec id="s2_4"><title>2.4. Hydrogen fuel research May benefit from shift in auto industry (Hydrogen Fuel News)</title><p>Feb. 7, 2013: Ford, Daimler, and Nissan recently joined forces to make progress in the field of hydrogen fuel cell technology. Each of the companies has an ambitious goal in mind in terms of hydrogen transportation, but each has also been faces with challenges that threaten to derail these goals. The automakers decided to team up in order to overcome some of these challenges and introduce new standards to hydrogen fuel cell technology as a whole.</p></sec><sec id="s2_5"><title>2.5. US Department of Energy launches new hydrogen fuel initiative (Hydrogen Fuel News)</title><p>May 23, 2013: Hydrogen fuel has become a major focus for the global auto industry and this focus is likely to transform the transportation sector around the world. As automakers put more emphasis on clean transportation, global markets are beginning to respond by supporting the promotion of hydrogen fuel in the transportation sector. Much of this support comes in the form of governments working to establish a working hydrogen fuel infrastructure that will be capable of supporting a new generation of fuel cell vehicles.</p></sec><sec id="s2_6"><title>2.6. As Is noted in “CHFCA Weekly Fuel” of January 2014, Toyota unveils zero-emissions hydrogen fuel-cell “Car of the Future” for sale next year (Think Progress)</title><p>Toyota announced the launch of a hydrogen-powered fuel-cell car in the US next year at the annual Consumer Electronics Show (CES) in Las Vegas. The car, which resembles the popular Corolla, is yet to be named, but like the birth of a royal child it’s the pedigree that counts—and Toyota is the largest auto manufacturer in the world.</p></sec><sec id="s2_7"><title>2.7. As Is noted in “CHFCA Weekly Fuel” of January 2014, Toyota touts hydrogen fuel vehicles despite criticism (The Detroit News)</title><p>A top US Toyota Motor Corp. executive strongly stood by its focus on hydrogen fuel cell vehicles, defending their safety and dismissing criticism from the top executives at Tesla Motors, Nissan Motor Co. and others. “I realize there is no shortage of naysayer regarding the viability of this technology and the infrastructure to support it,” said Bob Carter, senior vice president for automotive operations, Toyota Motor Sales USA Inc.</p><p>In connection with this, it is also expedient to take into account the long-term corporation (partnership) of Shell and General Motors Companies, relevance to hydrogen charging stations and fuel cell electrical vehicles, for instance:</p><p>1) July 2011: “The hydrogen infrastructure for automobiles is economically viable and do-able,” said Larry Burns, Ph.D., General Motors Vice President, Research &amp; Development and Strategic Planning… Shell Hydrogen has been developing hydrogen and fuel cell businesses since 1999 www.minichamps.ru/2011/general-motors-shell-fuel-up-on-hydrogen-in-los/angeles.</p><p>2) It was installed in November 2007 by Shell and General Motors to provide a venue for demonstrations to federal lawmakers and officials. Hydrogen fuel cells have long been touted as the next great energy revolution: www.thelivingmoon.com/41pegasus/02files/Alternate_Fuel_Shell_Oil_Hydrogen.html.</p><p>3) November 2004: The hydrogen-dispensing pump is the first installed at a public gas station in the country, according to officials from Shell Hydrogen and General Motors Corp., who will team up today to… Virtually all the major auto manufacturers have prototype vehicles that run on fuel cells and are refining the technology: www.washingtonpost.com/wp-dyn/articles/A38168-2004Nov9.html.</p><p>4) Washington DC, March 5, 2003—General Motors Corp. and Shell Hydrogen are combining resources to help make hydrogen fuel cell vehicles a commercially viable reality, the two announced today. “The partnership brings together two leaders in hydrogen energy and transportation to take a coordinated, comprehensive approach,” said Donald Huberts, chief executive officer of Shell Hydrogen. “By combining GM’s expertise in vehicle technology with Shell’s leadership in refueling technologies, the initiative represents an important step forward in the commercialization of hydrogen fuel cell vehicles” http://www.wec.org/news/shell-gm-partner-to-make-hydrogen-fuel-cell-vehicles-a-reality.</p></sec><sec id="s2_8"><title>2.8. Shell predicts the end of the gas guzzler by 2070. The New Zealand Herald (2014)</title><p>Shell has released a report predicting the end of petrol-powered cars will be in 2070. The oil giant have compiled a 46-page report, using the progress in automotive fuel technology and economic scenarios as a basis for their prediction of all petrol cars becoming a thing of the past by 2070.</p><p>In the present paper are considered, in the light of a constructive critical analysis [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] of a number of data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref22">22</xref>] , some fundamental aspects—open questions, relevant to developing, may be, within several years time frame, of a key breakthrough technology of a compact and energy efficient hydrogen storage in hydrogenated graphite nanofibers (GNFs).</p></sec><sec id="s2_9"><title>2.9. The Northeastern University (NU) Group [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref8">8</xref>] Hydrogen Storage Activity</title><p>As was noted in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] (2002) by Maeland, whose two works were cited in [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref1">1</xref>] (1978) and Ref. [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] (1981) in it), at the 1996 fall meeting of the US Materials Research Society (MRS), held in Boston, Massachusetts, Rodriguez and Baker of Northeastern University (NU), Boston, presented a paper in which they claimed the development of a “super” hydrogen storage nanomaterial. The material, graphite nanofibers (GNFs), discovered by Baker back in 1972 was claimed to be capable of storing up to 30 liters of gaseous hydrogen (H<sub>2</sub>) per gram of nanofibers of the herringbone-like structure (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref50">50</xref>] (1996) and Ref. [<xref ref-type="bibr" rid="scirp.51724-ref51">51</xref>] (1997) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ), i.e. about 73 mass% (of the graphite-hydrogen system mass) corresponding to formula CH32. The graphite nanofibers (GNFs) were preparing by reacting hydrocarbons with carbon monoxide on catalytic particles of bi- or tri-metallic nickel or iron. Hydrogen uptakes were determined by exposing, in a system of known volume, a purified GNF bundle (batch-like) sample to molecular gaseous hydrogen at room temperature, and observing the drop in pressure over a 24 hour period from an initial value of 11.2 MPa [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref61">61</xref>] (1998) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ). Three of the herringbone-like structure samples, according to [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] , take up hydrogen to give the hydrogen adsorption data of 62 &#177; 5 mass% (but not 73 mass%, as it was declared in the earlier talks (1996, 1997)), two of the platelet-like structure samples take up hydrogen to give the hydrogen adsorption data of 46 and 54 mass%, and the tubular-like structure sample— 11 mass%. Four of the herringbone-like structure hydrogenated samples, according to [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] , released the most of the stored hydrogen (at room temperature for 5 - 10 min) to give the reversible hydrogen desorption data of 48 &#177; 5 mass%; the rest part of the stored hydrogen was released at higher temperatures (under temperature-pro- grammed desorption examination) to give the irreversible hydrogen desorption data of 14 &#177; 5 mass%. The results reported by Rodriguez and Baker immediately caused controversy. Michal Heben of the National Renewable Laboratory in Denver, Colorado, USA, pointed out that the highest ratio of hydrogen to carbon found in Nature is 4/1 (CH<sub>4</sub>) and corresponds to 25 mass% and expressed skepticism (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref51">51</xref>] (1997) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ) of the results and attempts to verify the results of Rodriguez and Baker. Ahn et al. (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref52">52</xref>] (1998) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ) measured hydrogen adsorption and desorption at 300 K on graphite nanofibers (GNFs) and reported that the absolute level of hydrogen desorption from these materials were typically less than 0.025 H/C (0.2 mass%) which is comparable to other forms of carbon. Jarvi et al. (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref53">53</xref>] (1999) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ) reported very low hydrogen storage capacity at 303 K, comparable to activated carbon, for graphite nanofibers (GNFs) prepared by catalytic decomposition of ethylene over nickel, iron, copper/nickel and alumina/magnesia catalysts and concluded that they were unlikely storage materials for hydrogen. However, they left the door open by stating that subtle processing effect might convert inactive materials into effective hydrogen sorbents (as has been recently shown in analytical studies [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] , and is considered in the present analytical study). As was also noted in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] , the announcement at the MRS meeting did not escape the automakers and Daimler-Chrysler began an evaluation study with the NU group of these “super” hydrogen storage materials. Later, however, Daimler-Chrysler ended their participation in the study. Then, Ford Motor Company was supporting the NU group (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref54">54</xref>] (1999) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ). The NU group was also supported by the DOE in USA (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref55">55</xref>] (1998) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ), but the support was terminated presumably because of the un-willingness of Rodriguez and Baker to share their GNF samples with other DOE laboratories for examination. More detailed description of the situation was done by Jennifer Babson, a freelance writer in Boston, who interviewed (in November 1997) Rodriguez and Baker; see two 10/25/97 articles from the Economist on hydrogen fuel. This un-willingness to submit samples to other investigations had continued to fuel the controversy and prompted Dr. Gary Sandrock, a well known expert in the field of hydrogen storage materials, to publically call on Rodriguez to submit samples to others for a “Real-Word Test” of her nanofiber materials (Ref. [<xref ref-type="bibr" rid="scirp.51724-ref56">56</xref>] (1998) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ). It, however, had not been done (so far as we know) up to 2005 [<xref ref-type="bibr" rid="scirp.51724-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref22">22</xref>] , despite the fact that Rodriguez and Baker were issued two related US patents of 1997 (“Storage of hydrogen in layered nanostructures”) [<xref ref-type="bibr" rid="scirp.51724-ref6">6</xref>] and 2000 (“Method for introducing hydrogen into layered nanostructures”) [<xref ref-type="bibr" rid="scirp.51724-ref7">7</xref>] and had thus secured protection for their process. As can be shown, the negative test-results [<xref ref-type="bibr" rid="scirp.51724-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref22">22</xref>] , with respect to [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] data (i.e., both for Rodriguez-Baker et al. data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref8">8</xref>] , and for Gupta et al. ones [<xref ref-type="bibr" rid="scirp.51724-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] ), could be caused by using in [<xref ref-type="bibr" rid="scirp.51724-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref22">22</xref>] the non-adequate GNF samples (including samples supplied for this test by Rodriguez and Baker themselves). The work of the NU group had been presented in a number of talks (Refs. [<xref ref-type="bibr" rid="scirp.51724-ref58">58</xref>]-[<xref ref-type="bibr" rid="scirp.51724-ref60">60</xref>] (1999) in [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] ) and in two yearly cited (up to nowadays) articles in the Journal of Physical Chemistry of 1998 [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] and 1999 [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] . Article [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] has been cited (from 1998) 168 times in Scopus; the most recent citing is in two articles of 2013 [<xref ref-type="bibr" rid="scirp.51724-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref24">24</xref>] . Article [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] has been cited (from 1999) 196 times in Scopus; the most recent citing is in two articles of 2013 [<xref ref-type="bibr" rid="scirp.51724-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref26">26</xref>] .</p><p>Unlike [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] (1998, 1999), the Gupta et al. papers [<xref ref-type="bibr" rid="scirp.51724-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] (2000-2004, 2006) have not been discussed and/or cited so much, despite of the situation that, as far as we know, only experimental results [<xref ref-type="bibr" rid="scirp.51724-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] confirm (and reproduce, in an essential degree) the extraordinary experimental data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref8">8</xref>] . And as far as we know, both authors [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref8">8</xref>] (1998-2000, 2005) and authors [<xref ref-type="bibr" rid="scirp.51724-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] (2000-2004, 2006) have never crossed out their extraordinary experimental results. Nevertheless, authors [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] (1998) had done some corrections (and/or modifications) in [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] (1999) of their original adsorption-desorption data. Baker (in [<xref ref-type="bibr" rid="scirp.51724-ref8">8</xref>] (2005)) had modified the reversible hydrogen adsorption-desorption data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] (for the herringbone-like structure GNF samples) up to value of “40% by mass of molecular hydrogen per gram of carbon” that corresponds to 29 mass% of hydrogen (of carbon-hydro- gen system mass), instead of 48 &#177; 5 mass% quantity declared in [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] . In article of Lueking et al. [<xref ref-type="bibr" rid="scirp.51724-ref27">27</xref>] (2004), where Rodriguez and Baker were co-authors, it was noted the quantity of 67 mass%, relevance to [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref6">6</xref>] data (for the herringbone-like structure GNF samples), and the quantity up to 40%, relevance to [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref7">7</xref>] data (for the herringbone-like structure GNF samples). The graphite nanofibers (GNFs) possessing a herringbone-like structure and a high degree of defects (dislocations) were found [<xref ref-type="bibr" rid="scirp.51724-ref27">27</xref>] to exhibit the best performance for hydrogen storage resulted in 3.8 mass% release after exposure at 69 bar and room temperature (for 10 h). This result is in contrary with data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref8">8</xref>] . But, as was stressed in [<xref ref-type="bibr" rid="scirp.51724-ref27">27</xref>] , the “herringbone” graphite nanofibers (GNFs) used in that investigation were produced from a different catalyst formulation than that used in [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] and [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] . Furthermore, as was also stressed in [<xref ref-type="bibr" rid="scirp.51724-ref27">27</xref>] , the hydrogenation adsorption/desorption protocol followed there was not the same as that used in [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] and [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] . It is necessary to emphasize that the extraordinary experimental results [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] have not been reproduced by other research teams worldwide [<xref ref-type="bibr" rid="scirp.51724-ref20">20</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref27">27</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref30">30</xref>] . But the rather known authors [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] (see, for instance, information about them in Scopus and/or ScienceDirect.com Internet programs) have not definitely crossed out their data (as far as we know). Some of these works [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] have been yearly cited (up to nowadays). On the other hand, the physics of such results [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] has been developed (in an essential degree) in analytical studies [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref31">31</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref33">33</xref>] . Therefore, there are serious reasons to assume (following to [<xref ref-type="bibr" rid="scirp.51724-ref34">34</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref35">35</xref>] ) that experimental works [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] have contained some “know-how” methodological and/or technological elements. It is under a consideration in the present analytical study.</p></sec></sec><sec id="s3"><title>3. Some Fundamental Open Questions of the Considered Problem</title><sec id="s3_1"><title>3.1. On Thermodynamic Stability and Related Characteristics of Some Hydrogenated Graphene Layers Nanostructures: Relevance to the Hydrogen Storage Problem</title><p>The analytical study [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] is devoted to consideration of the thermodynamic stability, and related thermodynamic characteristics of the following graphene layers systems: 1) double-side hydrogenated graphene of composition CH (theoretical graphene [<xref ref-type="bibr" rid="scirp.51724-ref36">36</xref>] (<xref ref-type="fig" rid="fig4">Figure 4</xref>)) and experimental graphene [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] ; 2) theoretical single-side hydrogenated graphene of composition CH; 3) theoretical single-side hydrogenated graphene of composition C<sub>2</sub>H (graphene); 4) experimental hydrogenated epitaxial graphene, bilayer graphene and a few layer graphene on SiO<sub>2</sub> or other substrates; 5) experimental and theoretical single-external side hydrogenated single-walled carbon nanotubes, and experimental hydrofullerene C<sub>60</sub>H<sub>36</sub>; 6) experimental single-internal side hydrogenated (up to C<sub>2</sub>H or CH composition) graphene nanoblisters with intercalated high pressure H<sub>2</sub> gas inside them, formed on a surface of highly oriented pyrolytic graphite or epitaxial graphene under the atomic hydrogen treatment; and 7) experimental hydrogenated graphite nanofibers—multigraphene with intercalated solid H<sub>2</sub> nanoregions of high density inside them [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] , relevant to solving the current problem of the hydrogen storage in fuel-cell-powered vehicles and other clean energy applications. It is expedient to note [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] that there are a number of fundamental open questions in this field to be further studied.</p><p>The <xref ref-type="fig" rid="fig4">Figure 4</xref> shows the diamond-like distorted hexagonal network with carbon in sp<sup>3</sup> hybridization [<xref ref-type="bibr" rid="scirp.51724-ref36">36</xref>] , the carbon atoms are shown in gray and the hydrogen atoms in white.</p></sec><sec id="s3_2"><title>3.2. Determination of thermodynamic characteristics of graphene hydrides</title><p>Some theoretical, experimental and semi-empirical results [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref36">36</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref41">41</xref>] of determination of thermodynamic characteristics of graphene hydrides, including determination of the energy of formation of graphene hydrides from graphene and atomic gaseous hydrogen, the energy of breaking-down of C-H sp<sup>3</sup>-bonds (∆H (C-H)) in graphene hydrides, the energy of formation of graphene hydrides from atomic gaseous carbon and atomic gaseous hydrogen, the energy of breaking-down of C-C sp<sup>3</sup>-bonds (∆H (C-C)) in graphene hydrides, and some other characteristics are considered (<xref ref-type="table" rid="table1">Table 1</xref>) from [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] .</p><p>The critical comparison of the theoretical and experimental quantities, resulting in determination of the errors of the theoretical evaluations, are also included in [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] . In the light of the analytical results [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] , two open questions formulated by K.S. Novoselov, A.K. Geim et al. (2009) [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] are considered, namely as:</p><p>1) Is the theoretical graphene (CH) [<xref ref-type="bibr" rid="scirp.51724-ref36">36</xref>] “the until-now-theoretical material”?</p><p>2) May the experimental hydrogenated graphene (CH) [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] have “a more complex hydrogen bonding than the one suggested by theory [<xref ref-type="bibr" rid="scirp.51724-ref36">36</xref>] ”?</p><p>Two other fundamental open questions [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] are also discussed, namely as:</p><p>3) Can hydrogenated graphene layers nanostructures (graphene hydrides) with a high energy of C-C sp<sup>3</sup>-bonds close to that for graphene exist?</p><p>4) Can a solid (or liquid) molecular hydrogen nanophase be intercalated into hydrogenated graphite nanofibers.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The theoretical graphene structure in chair configura- tion</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x9.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Analytical and other characteristics</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  ></th><th align="center" valign="middle"  colspan="5"  >Value/quantity (analytical: an.)</th></tr></thead><tr><td align="center" valign="middle" >∆H (C-H) (eV)</td><td align="center" valign="middle" >∆H (bind.) (eV)</td><td align="center" valign="middle" >∆H (C-C) (eV)</td><td align="center" valign="middle" >∆H (des.) (eV)</td><td align="center" valign="middle" >K<sup>0</sup> (des.) (s<sup>−1</sup>)</td></tr><tr><td align="center" valign="middle" >Graphene [<xref ref-type="bibr" rid="scirp.51724-ref36">36</xref>]</td><td align="center" valign="middle" >(2.5 &#177; 0.1) an.</td><td align="center" valign="middle" >6.56</td><td align="center" valign="middle" >(2.7) an.</td><td align="center" valign="middle" >(2.5) an.</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Graphene [<xref ref-type="bibr" rid="scirp.51724-ref39">39</xref>]</td><td align="center" valign="middle" >1.50</td><td align="center" valign="middle" >5.03</td><td align="center" valign="middle" >(2.35) an.</td><td align="center" valign="middle" >(1.5) an.</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Graphene [<xref ref-type="bibr" rid="scirp.51724-ref38">38</xref>] Graphene [<xref ref-type="bibr" rid="scirp.51724-ref38">38</xref>] an.</td><td align="center" valign="middle" >2.46 &#177; 0.17 2.46 &#177; 0.17</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >2.46 &#177; 0.17 2.46 &#177; 0.17</td><td align="center" valign="middle" >(2.1 &#177; 0.5) &#215; 10<sup>17</sup> 2.0 &#215; 10<sup>15</sup></td></tr><tr><td align="center" valign="middle" >Graphene membrane [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] an.</td><td align="center" valign="middle" >2.5 &#177; 0.1 2.6 &#177; 0.1</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >2.5 &#177; 0.1 2.6 &#177; 0.1</td><td align="center" valign="middle" >7 &#215; 10<sup>12</sup> 5 &#215; 10<sup>13</sup></td></tr><tr><td align="center" valign="middle" >Graphene epitaxial [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] an.</td><td align="center" valign="middle" >1.84 1.94</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.84 1.94</td><td align="center" valign="middle" >7 &#215; 10<sup>12</sup> 5 &#215; 10<sup>13</sup></td></tr><tr><td align="center" valign="middle" >Graphene epitaxial, TDS #1 [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] an.</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.6 &#177; 0.3</td><td align="center" valign="middle" >2 &#215; 10<sup>7</sup></td></tr><tr><td align="center" valign="middle" >Graphene epitaxial, TDS #2 [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] an.</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.6 &#177; 0.3</td><td align="center" valign="middle" >1 &#215; 10<sup>6</sup></td></tr><tr><td align="center" valign="middle" >Graphene epitaxial, TDS #3 [<xref ref-type="bibr" rid="scirp.51724-ref37">37</xref>] an.</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.23 &#177; 0.05</td><td align="center" valign="middle" >2.4</td></tr><tr><td align="center" valign="middle" >Graphene [<xref ref-type="bibr" rid="scirp.51724-ref39">39</xref>]</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >7.40</td><td align="center" valign="middle" >(4.93) an.</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Graphene<sup>*</sup> [<xref ref-type="bibr" rid="scirp.51724-ref31">31</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref33">33</xref>]</td><td align="center" valign="middle" >2.6</td><td align="center" valign="middle" >9.95</td><td align="center" valign="middle" >4.9</td><td align="center" valign="middle" >2.6</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Graphite [<xref ref-type="bibr" rid="scirp.51724-ref31">31</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref33">33</xref>]</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >7.41 &#177; 0.05</td><td align="center" valign="middle" >4.94 &#177; 0.03</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Diamond [<xref ref-type="bibr" rid="scirp.51724-ref31">31</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref33">33</xref>]</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >7.38 &#177; 0.04</td><td align="center" valign="middle" >3.69 &#177; 0.02</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Hydrofullerene C<sub>60</sub>H<sub>36</sub> [<xref ref-type="bibr" rid="scirp.51724-ref40">40</xref>]</td><td align="center" valign="middle" >2.64 &#177; 0.01</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Hydrogenated carbon nanotubes (C<sub>2</sub>H, [<xref ref-type="bibr" rid="scirp.51724-ref41">41</xref>] )</td><td align="center" valign="middle" >2.5 &#177; 0.2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap></sec><sec id="s3_3"><title>3.3. A treatment &amp; interpretation of some recent STM, STS, HREELS/LEED, PES, ARPS and Raman spectroscopy data on Hydrogen sorption with epitaxial grapheme</title><p>Herein, some results of the thermodynamic analysis [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] of the data [<xref ref-type="bibr" rid="scirp.51724-ref42">42</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref46">46</xref>] on hydrogen sorption with epitaxial graphene are presented in <xref ref-type="table" rid="table2">Table 2</xref>, <xref ref-type="table" rid="table3">Table 3</xref>. In the framework of the formal kinetics approximation of the first order rate reaction, the characteristic quantities for the processes [<xref ref-type="bibr" rid="scirp.51724-ref42">42</xref>] -[<xref ref-type="bibr" rid="scirp.51724-ref46">46</xref>] of hydrogen sorption (the rate constant (K (des.) = 1/0.63 (des.)), the activation energy (ΔH (des.)), the pre-exponential factor of the rate constant (K<sup>0</sup> (des.)) are determined.</p><p>Evaluation of the HREELS elastic peak FWHM of hydrogenated graphene on SiC substrate (SiC-D/ QFMLG-H) upon annealing is shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, where the uncertain annealing temperature is estimated to be 5%, error bars represent the σ variation of FWHM measured across the entire surface of several samples [<xref ref-type="bibr" rid="scirp.51724-ref44">44</xref>] .</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Analytical results (from [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] )</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Materials</th><th align="center" valign="middle"  colspan="3"  >Values/quantities</th></tr></thead><tr><td align="center" valign="middle" >ΔH (des.) (eV)</td><td align="center" valign="middle" >K<sup>0</sup> (des.) (s<sup>−1</sup>)</td><td align="center" valign="middle" >τ 0.63 (des.) 553 K (s)</td></tr><tr><td align="center" valign="middle" >Graphene flakes/SiO<sub>2</sub> [<xref ref-type="bibr" rid="scirp.51724-ref42">42</xref>]</td><td align="center" valign="middle" >0.11 &#177; 0.07</td><td align="center" valign="middle" >0.15</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >Graphene/Ni [<xref ref-type="bibr" rid="scirp.51724-ref43">43</xref>] HOPG [<xref ref-type="bibr" rid="scirp.51724-ref43">43</xref>]</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >130 130</td></tr><tr><td align="center" valign="middle" >(SiC-D/QFMLG-H) [<xref ref-type="bibr" rid="scirp.51724-ref44">44</xref>]</td><td align="center" valign="middle" >0.7 &#177; 0.2</td><td align="center" valign="middle" >9 &#215; 10<sup>2</sup></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >(SiC-D/QFMLG) [<xref ref-type="bibr" rid="scirp.51724-ref44">44</xref>]</td><td align="center" valign="middle" >2.0 &#177; 0.6</td><td align="center" valign="middle" >1 &#215; 10<sup>6</sup></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Some other analytical results (from [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] )</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Samples</th><th align="center" valign="middle"  colspan="4"  >Values/quantities (analytical: an.)</th></tr></thead><tr><td align="center" valign="middle" >ΔH (des.) I (eV)</td><td align="center" valign="middle" >K<sup>0</sup> (des.) I (s<sup>−1</sup>)</td><td align="center" valign="middle" >ΔH (des.) II (eV)</td><td align="center" valign="middle" >K<sup>0</sup> (des.) II (s<sup>−1</sup>)</td></tr><tr><td align="center" valign="middle" >1LG-15W (grapheme) [<xref ref-type="bibr" rid="scirp.51724-ref45">45</xref>]</td><td align="center" valign="middle" >0.6 &#177; 0.2</td><td align="center" valign="middle" >2 &#215; 10<sup>4</sup></td><td align="center" valign="middle" >0.19 &#177; 0.07</td><td align="center" valign="middle" >3 &#215; 10<sup>−2</sup></td></tr><tr><td align="center" valign="middle" >2LG-15W (bi-graphene) [<xref ref-type="bibr" rid="scirp.51724-ref45">45</xref>]</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.9 &#177; 0.3</td><td align="center" valign="middle" >1 &#215; 10<sup>3</sup></td></tr><tr><td align="center" valign="middle" >1LG-5W (grapheme) [<xref ref-type="bibr" rid="scirp.51724-ref45">45</xref>]</td><td align="center" valign="middle" >0.15 &#177; 0.04</td><td align="center" valign="middle" >2 &#215; 10<sup>−2</sup></td><td align="center" valign="middle" >0.31 &#177; 0.07</td><td align="center" valign="middle" >5 &#215; 10<sup>−1</sup></td></tr><tr><td align="center" valign="middle" >2LG-5W (bi-graphene) [<xref ref-type="bibr" rid="scirp.51724-ref45">45</xref>]</td><td align="center" valign="middle" >0.50 &#177; 0.15</td><td align="center" valign="middle" >2 &#215; 10<sup>3</sup></td><td align="center" valign="middle" >0.40 &#177; 0.15</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >HOPG [<xref ref-type="bibr" rid="scirp.51724-ref47">47</xref>] , TDS-peaks I, II</td><td align="center" valign="middle" >0.6 &#177; 0.2</td><td align="center" valign="middle" >1.5 &#215; 10<sup>4</sup></td><td align="center" valign="middle" >1.0 &#177; 0.3</td><td align="center" valign="middle" >2 &#215; 10<sup>6</sup></td></tr><tr><td align="center" valign="middle" >Graphene/SiC [<xref ref-type="bibr" rid="scirp.51724-ref46">46</xref>]</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3.6</td><td align="center" valign="middle" >2 &#215; 10<sup>14</sup></td></tr><tr><td align="center" valign="middle" >HOPG [<xref ref-type="bibr" rid="scirp.51724-ref48">48</xref>] , TDS-peaks I, II HOPG [<xref ref-type="bibr" rid="scirp.51724-ref48">48</xref>] , TDS-peak I</td><td align="center" valign="middle" >2.4 [<xref ref-type="bibr" rid="scirp.51724-ref48">48</xref>] (2.4 &#177; 0.5) an.</td><td align="center" valign="middle" >(2 &#215; 10<sup>10</sup>) an.</td><td align="center" valign="middle" >4.1 [<xref ref-type="bibr" rid="scirp.51724-ref48">48</xref>]</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >GNF [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref11">11</xref>] , TDS-peaks I, II</td><td align="center" valign="middle" >(2.4 &#177; 0.5) an.</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Evaluation of the HREELS elastic peak FWHM of hydrogenated graphene on SiC substrate upon annealing</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x10.png"/></fig><p>Some models (<xref ref-type="fig" rid="fig6">Figure 6</xref>) and characteristics [<xref ref-type="bibr" rid="scirp.51724-ref34">34</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref35">35</xref>] of hydrogen chemisorption on graphite (on the basal and edge planes) have been used for interpretation of the results of data [<xref ref-type="bibr" rid="scirp.51724-ref42">42</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref46">46</xref>] treatment, in relation with the hydrogen storage problem. Schemes of some theoretical models of chemisorption of atomic hydrogen on graphite on the basal and edge planes [<xref ref-type="bibr" rid="scirp.51724-ref34">34</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref35">35</xref>] are presented in <xref ref-type="fig" rid="fig6">Figure 6</xref>.</p><p>As it is shown in [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] , there are a number of fundamental open questions also in this field to be further studied.</p></sec><sec id="s3_4"><title>3.4. On the physics of intercalation of hydrogen into surface graphene-like nanoblisters in pyrolytic graphite and epitaxial grapheme</title><p>In the light of the analytical results [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] , the physics of the spontaneous process ( [<xref ref-type="bibr" rid="scirp.51724-ref47">47</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref50">50</xref>] and others) of intercalation of gaseous molecular hydrogen of a high pressure into nanoblisters—the surface nano-size bulges with monolayer graphene-like “walls”, those being formed (at definite conditions of hydrogenation in atomic gaseous hydrogen) on a surface of highly oriented pyrolytic graphite (<xref ref-type="fig" rid="fig7">Figure 7</xref>, <xref ref-type="fig" rid="fig8">Figure 8</xref>) and epitaxial graphene (<xref ref-type="fig" rid="fig9">Figure 9</xref>, <xref ref-type="fig" rid="fig1">Figure 1</xref>0). A fundamental open question [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref51">51</xref>] namely as “Can gaseous atomic hydrogen</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Schemes of some theoretical models of chemisorption of atomic hydrogen on graphite on the basal and edge planes</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x11.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> High resolution STM images of the untreated HOPG sample taken from varios areas of: (a) 60.8 &#215; 60.8 nm; (b) 10.9 &#215; 10.9 nm; (c) AFM image (area of 1 &#215; 1 nm); (d) Surface height profile obtained from the AFM image reported in (c)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x12.png"/></fig><p>penetrate through a perfect graphene monolayer?” is also discussed.</p><p>On <xref ref-type="fig" rid="fig7">Figure 7</xref> there are STM images of the untreated HOPG sample [<xref ref-type="bibr" rid="scirp.51724-ref49">49</xref>] (under ambient conditions) taken from areas of (a) 60.8 &#215; 60.8 nm and (b) 10.9 &#215; 10.9 nm (high resolution image of the square in image (a)). (c). AFM image (area of 1 &#215; 1 nm) of the HOPG sample subjected to atomic hydrogen dose (D) of 1.8 &#215; 10<sup>16</sup> H<sup>0</sup>/cm<sup>2</sup>. (d) Surface height profile obtained from the AFM image reported in (c). The STM tunnel V<sub>bias</sub> and current are 50 - 100 mV and 1 - 1.5 mA, respectively.</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows a hydrogen storage efficiency of HOPG samples [<xref ref-type="bibr" rid="scirp.51724-ref49">49</xref>] , desorbed molecular hydrogen (Q) versus dose (D) of atomic hydrogen exposure (<xref ref-type="fig" rid="fig8">Figure 8</xref>(a)) and STM image for 600 &#215; 600 nm area of the HOPG sample subjected to atomic hydrogen dose of 1.8 &#215; 10<sup>16</sup> H<sup>0</sup>/cm<sup>2</sup>, followed by hydrogen thermal desorption (<xref ref-type="fig" rid="fig8">Figure 8</xref>(b)).</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> (a) Desorbed molecular hydrogen (Q) versus dose (D) of atomic hydrogen exposure; (b) STM image for 600 &#215; 600 nm area of the HOPG sample subjected to atomic hydrogen dose followed by hydrogen thermal desorption</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x13.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> (a) STM image of hydrogenated graphene; (b) The same image as in (a) with inverted color scheme</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x14.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> (a) STM image of the graphene surface after extended hydrogen exposure; (b) Large graphene area recovered from hydrogenation by annealing to 1073 K</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x15.png"/></fig><p><xref ref-type="fig" rid="fig9">Figure 9</xref>(a) presents a scanning tunneling microscopy (STM) image of hydrogenated graphene [<xref ref-type="bibr" rid="scirp.51724-ref50">50</xref>] . The bright protrusions visible in the image are atomic hydrogen adsorbate structures identified as A = ortho-dimers, B = para-dimers, C = elongated dimers, D = monomers (imaging parameters: V<sub>t</sub> = −0.245 V<sub>t</sub>, I<sub>t</sub> = −0.26 nA). There is inset in (a): ortho- and para-dimer configuration on the graphene lattice (A and B, respectively). <xref ref-type="fig" rid="fig9">Figure 9</xref>(b) shows the same image as in <xref ref-type="fig" rid="fig9">Figure 9</xref>(a) but with inverted color scheme, giving emphasis to preferential hydrogen adsorption along the 6 &#215; 6 modulation on the SiC (0001)—(1 &#215; 10 surface). Hydrogen dose at T<sub>beam</sub> = 1600 K, t = 5 s, F = 10<sup>12</sup> - 10<sup>13</sup> atoms/cm<sup>2</sup>&#183;s.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>0(a) presents the STM image of the graphene surface after extended hydrogen exposure [<xref ref-type="bibr" rid="scirp.51724-ref50">50</xref>] . The bright protrusions visible in the image are atomic hydrogen clusters (imaging parameters: V<sub>t</sub> = −0.36 V, I<sub>t</sub> = −0.32 nA). Hydrogen dose at T = 1600 K, t = 90 s, F = 10<sup>12</sup> - 10<sup>13</sup> atoms/cm<sup>2</sup>&#183;s. <xref ref-type="fig" rid="fig1">Figure 1</xref>0(b) exibit a large graphene area recovered from hydrogenation by annealing to 1073 K (imaging parameters: V<sub>t</sub> = −0.38 V, I<sub>t</sub> = −0.41 nA).</p><p>Authors of [<xref ref-type="bibr" rid="scirp.51724-ref51">51</xref>] noted that their test calculations show that the barrier for the penetration of a hydrogen atom through the six-membered ring of graphene is larger than 2.0 eV. Thus, they believe that it is almost impossible for a hydrogen atom to pass through the six-membered ring of graphene at room temperature (from a private communication with H.G. Xiang and M.-H. Whangbo). On the other hand, in the light of analysis [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] of a number of recent experimental studies, there is a real possibility that a hydrogen atom can pass through the graphene network at room temperature. This is the case of existing relevant defects in graphene, i.e., grain boundaries (particularly, the triple junctions of them) and/or vacancies.</p></sec><sec id="s3_5"><title>3.5. On the physics of the elastic &amp; plastic deformation of graphene (graphene-like) walls in hydrogenated graphite nanofibers</title><p>Herein, some results of the thermodynamic analysis [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] of the unique (extraordinary) data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] are considered. Mechanical behavior (the elastic and plastic deformation (<xref ref-type="fig" rid="fig1">Figure 1</xref>1, <xref ref-type="fig" rid="fig1">Figure 1</xref>2)) of the graphene (graphene-like) walls in graphite nanofibers (GNFs) under definite hydrogenation conditions are analyzed and interpreted, relevance to the hydrogen storage problem. There are a number of fundamental open questions also in this field to be further studied. Here, <xref ref-type="fig" rid="fig1">Figure 1</xref>1 shows an increase in GNF width due to H<sub>2</sub>O adsorption [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] .</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>2 shows the TEM of the dehydrogenated GNFs, by [<xref ref-type="bibr" rid="scirp.51724-ref11">11</xref>] .</p><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Increase in GNF width due to H<sub>2</sub>O adsorption</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x16.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> TEM of the dehydrogenated GNF</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-2201025x17.png"/></fig></sec><sec id="s3_6"><title>3.6. On the physics of engineering of “super” hydrogen storage Carbonaceous nanomaterials, in the light of analysis of the Rodriguez-Baker extraordinary data and some others</title><p>Herein, in the light of a constructive critical analysis (including the analytical results [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] ) of a complete set of the extraordinary experimental (nobody reproduced up to nowadays) data [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] and some related ones [<xref ref-type="bibr" rid="scirp.51724-ref52">52</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref53">53</xref>], the physical fundamentals of developing of a key breakthrough technology of a compact and energy efficient hydrogen storage in hydrogenated graphite nanofibers (<xref ref-type="fig" rid="fig1">Figure 1</xref>2, 1, 2) are considered. As far as we know, both authors [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref8">8</xref>] (1998-2005) and authors [<xref ref-type="bibr" rid="scirp.51724-ref9">9</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] (2000-2006) have never crossed out their extraordinary non-reproduced experimental results. On the other hand, article [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] has been cited (within 1998-2013) 168 times in Scopus, and article [<xref ref-type="bibr" rid="scirp.51724-ref5">5</xref>] —196 times. But, as far as we know, nobody has analyzed and interpreted a complete set of [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] data. As is shown in the present study, the most recent negative test-results [<xref ref-type="bibr" rid="scirp.51724-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref23">23</xref>] , with respect to [<xref ref-type="bibr" rid="scirp.51724-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref12">12</xref>] data can be caused by using in [<xref ref-type="bibr" rid="scirp.51724-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref22">22</xref>] the non-adequate GNF samples (including samples and regimes supplied for this test by Rodriguez and Baker themselves). Some ethical aspects of this long-term situation are discussed, as well.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>1) As is shown in this work, in the light of analysis [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] , there are a number of fundamental open questions, relevance to developing of a key breakthrough technology of a compact and energy efficient hydrogen storage in hydrogenated graphite nanofibers (<xref ref-type="fig" rid="fig1">Figure 1</xref>, <xref ref-type="fig" rid="fig2">Figure 2</xref>), to be further studied.</p><p>2) These fundamental open questions [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref31">31</xref>] - [<xref ref-type="bibr" rid="scirp.51724-ref33">33</xref>] may be solved within several years, i.e., within the necessary time frame (<xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>3) A constructive open discussion and, may be, a related international cooperation on solving the above considered open questions seems expedient, relevant to the promotion of further developments, particularly in the developing of basic grounds of a possible break-through in nanotechnology for hydrogen on-board storage and other clean energy applications [<xref ref-type="bibr" rid="scirp.51724-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51724-ref3">3</xref>] .</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work has been supported by the RFBR (Project #14-08-91376 CT) and the TUBITAK (Project # 213M523).</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.51724-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Zuettel, A. 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