{"id":{"repo_id":"greece","oai_identifier":"oai:10442/0822"},"canonical_url":"https://search.dev.ndltd.org/etd/greece/oai:10442/0822","repository":{"repo_id":"greece","name":"Greek National Archive of PhD Theses","base_url":"https://phdtheses.ekt.gr/eadd_oai/request"},"display":{"title":"ΜΕΛΕΤΗ ΤΗΣ ΚΑΤΑΝΟΜΗΣ ΥΔΡΟΓΟΝΟΥ ΣΕ ΛΕΠΤΑ ΥΜΕΝΙΑ ΔΥΟ ΣΤΡΩΜΑΤΩΝ ΔΙΑΦΟΡΕΤΙΚΩΝ ΜΕΤΑΛΛΩΝ","abstract":"THE RESONANCE AT E(15N)=6.39 MEV IN THE REACTION 1H(15N,ΑΓ)12C HAS BEEN EMPLOYED FOR THE DETERMINATION OF THE HYDROGEN DEPTH DISTRIBUTION IN SOME THIN FILMS OF METAL-HYDROGEN SYSTEMS ONTO A STAINLESS STEEL SUBSTRATE. THE INVESTIGATED FILMS WERE: THE SINGLE LAYER FILMS V-H AND TI-H AND THE THIN FILMS SANDWICHES (FILMS CONSISTING OF TWO THIN LAYERS OF DIFFERENT MATERIALS) TATI -H, TANB-H, NBTA-H AND TAV-H. THE PREPARATION OF THE SAMPLES BY MEANS OF UHV TECHNIQUE AND THEIRTREATMENT DURING THE LOADING PROCESS WITH HYDROGEN IS DESCRIBED. THE HYDROGEN TO METAL RATIOS IN THE TWO COMPONENTS OF EACH SANDWICH ARE QUANTITATIVE THE SAMPLES HAVE BEEN ANNEALED AT SEVERAL TEMPERATURES (IN THE RANGE BETWEEN 25 AND 400 C), AND AFTER COOLING DOWN TO ROOM TEMPERATURE THE PROFILE OF THE REMAINING HYDROGEN HAS BEEN MEASURED. THEORETICAL ANALYSIS OF THE YIELD DEDUCED FROM A RESONANCE REACTION IN THE CASES OF A SINGLE AND DOUBLE LAYER SAMPLE IS PRESENTED. AN EXPLANATION FOR THE HYDROGEN CONCENTRATION IN THE TWO LAYERS OF THE SANDWICHES BEFORE AND AFTER ANNEALING IS ATTEMPTED USING A SIMPLE STATISTICAL MODEL FORTHE CHEMICAL POTENTIAL OF H IN METALS.","abstract_html":"THE RESONANCE AT E(15N)=6.39 MEV IN THE REACTION 1H(15N,ΑΓ)12C HAS BEEN EMPLOYED FOR THE DETERMINATION OF THE HYDROGEN DEPTH DISTRIBUTION IN SOME THIN FILMS OF METAL-HYDROGEN SYSTEMS ONTO A STAINLESS STEEL SUBSTRATE. THE INVESTIGATED FILMS WERE: THE SINGLE LAYER FILMS V-H AND TI-H AND THE THIN FILMS SANDWICHES (FILMS CONSISTING OF TWO THIN LAYERS OF DIFFERENT MATERIALS) TATI -H, TANB-H, NBTA-H AND TAV-H. THE PREPARATION OF THE SAMPLES BY MEANS OF UHV TECHNIQUE AND THEIRTREATMENT DURING THE LOADING PROCESS WITH HYDROGEN IS DESCRIBED. THE HYDROGEN TO METAL RATIOS IN THE TWO COMPONENTS OF EACH SANDWICH ARE QUANTITATIVE THE SAMPLES HAVE BEEN ANNEALED AT SEVERAL TEMPERATURES (IN THE RANGE BETWEEN 25 AND 400 C), AND AFTER COOLING DOWN TO ROOM TEMPERATURE THE PROFILE OF THE REMAINING HYDROGEN HAS BEEN MEASURED. THEORETICAL ANALYSIS OF THE YIELD DEDUCED FROM A RESONANCE REACTION IN THE CASES OF A SINGLE AND DOUBLE LAYER SAMPLE IS PRESENTED. AN EXPLANATION FOR THE HYDROGEN CONCENTRATION IN THE TWO LAYERS OF THE SANDWICHES BEFORE AND AFTER ANNEALING IS ATTEMPTED USING A SIMPLE STATISTICAL MODEL FORTHE CHEMICAL POTENTIAL OF H IN METALS.","abstract_has_math":false,"creators":["Πηλακούτα, Μυροφόρα"],"institution":"Πανεπιστήμιο Πατρών","degree_name":null,"degree_level":null,"degree_discipline":null,"degree_department":null,"school":null,"contributors":[],"advisors":[],"committee_chairs":[],"committee_members":[],"year":1988,"date_issued":"1988","date_published":"1988","updated_at":"2026-07-24T02:25:27Z","subjects":["HYDROGEN CHEMICAL POTENTIAL","HYDROGEN DEPTH DISTRIBUTION","HYDROGEN DEPTH PROFILE WITH 15N-METHOD","HYDROGEN DEPTH PROFILE WITH I.B.M.","HYDROGEN DISTRIBUTION IN SANDWICH-FILMS","HYDROGEN PROFILE","HYDROGEN TECHNOLOGY","THERMODYNAMIC OF METAL HYDROGEN SYSTEM","ΑΝΑΛΥΣΗ ΚΑΤΑΝΟΜΗΣ ΥΔΡΟΓΟΝΟΥ","ΘΕΡΜΟΔΥΝΑΜΙΚΗ ΣΥΣΤΗΜΑΤΟΣ ΜΕΤΑΛΛΟ-ΥΔΡΟΓΟΝΟ","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥ","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥ ΜΕ ΜΕΘΟΔΟ -15Ν","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥΣΕ ΔΙΠΛΑ ΥΜΕΝΙΑ","ΠΡΟΣΔΙΟΡΙΣΜΟΣ ΣΥΓΚΕΝΤΡΩΣΕΩΝ ΥΔΡΟΓΟΝΟΥ","ΤΕΧΝΟΛΟΓΙΑ ΥΔΡΟΓΟΝΟΥ","ΧΗΜΙΚΟ ΔΥΝΑΜΙΚΟ ΥΔΡΟΓΟΝΟΥ","Φυσικές Επιστήμες","Natural Sciences","Φυσική","Physical Sciences"],"languages":["gre"],"rights":[],"rights_urls":[],"identifier_entries":[{"key":"dc:identifier","label":"Identifier","values":["10.12681/eadd/0822"],"render_values":[{"text":"10.12681/eadd/0822","href":"https://doi.org/10.12681/eadd/0822","code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/10442/hedi/0822","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:creator","label":"Author","values":["Πηλακούτα, Μυροφόρα"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["1988"]},{"key":"dc:publisher","label":"Institution","values":["Πανεπιστήμιο Πατρών","University of Patras"]},{"key":"dc:type","label":"Dc Type","values":["PhD Thesis"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["HYDROGEN CHEMICAL POTENTIAL","HYDROGEN DEPTH DISTRIBUTION","HYDROGEN DEPTH PROFILE WITH 15N-METHOD","HYDROGEN DEPTH PROFILE WITH I.B.M.","HYDROGEN DISTRIBUTION IN SANDWICH-FILMS","HYDROGEN PROFILE","HYDROGEN TECHNOLOGY","THERMODYNAMIC OF METAL HYDROGEN SYSTEM","ΑΝΑΛΥΣΗ ΚΑΤΑΝΟΜΗΣ ΥΔΡΟΓΟΝΟΥ","ΘΕΡΜΟΔΥΝΑΜΙΚΗ ΣΥΣΤΗΜΑΤΟΣ ΜΕΤΑΛΛΟ-ΥΔΡΟΓΟΝΟ","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥ","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥ ΜΕ ΜΕΘΟΔΟ -15Ν","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥΣΕ ΔΙΠΛΑ ΥΜΕΝΙΑ","ΠΡΟΣΔΙΟΡΙΣΜΟΣ ΣΥΓΚΕΝΤΡΩΣΕΩΝ ΥΔΡΟΓΟΝΟΥ","ΤΕΧΝΟΛΟΓΙΑ ΥΔΡΟΓΟΝΟΥ","ΧΗΜΙΚΟ ΔΥΝΑΜΙΚΟ ΥΔΡΟΓΟΝΟΥ","Φυσικές Επιστήμες","Natural Sciences","Φυσική","Physical Sciences"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["gre"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["10.12681/eadd/0822","http://hdl.handle.net/10442/hedi/0822"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["THE RESONANCE AT E(15N)=6.39 MEV IN THE REACTION 1H(15N,ΑΓ)12C HAS BEEN EMPLOYED FOR THE DETERMINATION OF THE HYDROGEN DEPTH DISTRIBUTION IN SOME THIN FILMS OF METAL-HYDROGEN SYSTEMS ONTO A STAINLESS STEEL SUBSTRATE. THE INVESTIGATED FILMS WERE: THE SINGLE LAYER FILMS V-H AND TI-H AND THE THIN FILMS SANDWICHES (FILMS CONSISTING OF TWO THIN LAYERS OF DIFFERENT MATERIALS) TATI -H, TANB-H, NBTA-H AND TAV-H. THE PREPARATION OF THE SAMPLES BY MEANS OF UHV TECHNIQUE AND THEIRTREATMENT DURING THE LOADING PROCESS WITH HYDROGEN IS DESCRIBED. THE HYDROGEN TO METAL RATIOS IN THE TWO COMPONENTS OF EACH SANDWICH ARE QUANTITATIVE THE SAMPLES HAVE BEEN ANNEALED AT SEVERAL TEMPERATURES (IN THE RANGE BETWEEN 25 AND 400 C), AND AFTER COOLING DOWN TO ROOM TEMPERATURE THE PROFILE OF THE REMAINING HYDROGEN HAS BEEN MEASURED. THEORETICAL ANALYSIS OF THE YIELD DEDUCED FROM A RESONANCE REACTION IN THE CASES OF A SINGLE AND DOUBLE LAYER SAMPLE IS PRESENTED. AN EXPLANATION FOR THE HYDROGEN CONCENTRATION IN THE TWO LAYERS OF THE SANDWICHES BEFORE AND AFTER ANNEALING IS ATTEMPTED USING A SIMPLE STATISTICAL MODEL FORTHE CHEMICAL POTENTIAL OF H IN METALS.","Ο ΣΥΝΤΟΝΙΣΜΟΣ ΣΤΗΝ ΕΝΕΡΓΕΙΑ Ε=6.385 MEV ΤΗΣ ΑΝΤΙΔΡΑΣΗΣ Η(15Ν,ΑΓ)12C ΧΡΗΣΙΜΟΠΟΙΗΘΗΚΕ ΓΙΑ ΤΟΝ ΚΑΘΟΡΙΣΜΟ ΤΗΣ ΚΑΤΑ ΒΑΘΟΣ ΚΑΤΑΝΟΜΗΣ ΤΟΥ ΥΔΡΟΓΟΝΟΥ ΣΕ ΜΕΡΙΚΑ ΛΕΠΤΑ ΥΜΕΝΙΑ ΣΥΣΤΗΜΑΤΩΝ ΜΕΤΑΛΛΟ -ΥΔΡΟΓΟΝΟ ΠΑΝΩ ΣΕ ΥΠΟΣΤΡΩΜΑ ΑΝΟΞΕΙΔΩΤΟΥ ΧΑΛΥΒΑ. ΤΑ ΥΜΕΝΙΑ ΠΟΥ ΜΕΛΕΤΗΘΗΚΑΝ ΗΣΑΝ: ΤΑ ΥΜΕΝΙΑ ΕΝΟΣ ΣΤΡΩΜΑΤΟΣ V-H ΚΑΙ TI-H ΚΑΙ ΤΑ ΛΕΠΤΑ ΥΜΕΝΙΑ ΔΥΟ ΣΤΡΩΜΑΤΩΝ ΔΙΑΦΟΡΕΤΙΚΩΝ ΜΕΤΑΛΛΩΝ TATI-H, TANB-H, NBTA-H ΚΑΙ TAV-H. ΠΕΡΙΓΡΑΦΕΤΑΙ Η ΠΑΡΑΣΚΕΥΗ ΤΩΝ ΔΕΙΓΜΑΤΩΝ ΠΟΥ ΕΓΙΝΕ ΜΕ ΤΕΧΝΙΚΗ ΥΠΕΡ ΥΨΗΛΟΥ ΚΕΝΟΥ ΚΑΘΩΣΚΑΙ Ο ΧΕΙΡΙΣΜΟΣ ΤΟΥΣ ΚΑΤΑ ΤΗΝ ΔΙΑΔΙΚΑΣΙΑ ΦΟΡΤΙΣΗΣ ΜΕ ΥΔΡΟΓΟΝΟ. ΚΑΘΟΡΙΖΕΤΑΙ ΠΟΣΟΤΙΚΑ Ο ΛΟΓΟΣ ΥΔΡΟΓΟΝΟΥ ΠΡΟΣ ΜΕΤΑΛΛΟ ΣΤΑ ΔΥΟ ΣΤΡΩΜΑΤΑ ΤΟΥ ΚΑΘΕ ΔΙΠΛΟΥ ΔΕΙΓΜΑΤΟΣ(SANDWICH SAMPLE) ΚΑΙ ΕΞΕΤΑΖΕΤΑΙ Η ΚΑΤΑΝΟΜΗ ΤΟΥ ΥΔΡΟΓΟΝΟΥ ΠΟΥ ΠΑΡΑΜΕΝΕΙ ΣΤΑ ΔΕΙΓΜΑΤΑ ΜΕΤΑ ΑΠΟ ΘΕΡΜΙΚΗ ΕΠΕΞΕΡΓΑΣΙΑ IN-SITU ΣΕ ΔΙΑΦΟΡΕΣ ΘΕΡΜΟΚΡΑΣΙΕΣ (ΠΕΡΙΟΧΗ 25 ΕΩΣ 400 C) ΚΑΙ ΨΗΞΗ ΣΤΗ ΘΕΡΜΟΚΡΑΣΙΑ ΠΕΡΙΒΑΛΛΟΝΤΟΣ. ΠΑΡΟΥΣΙΑΖΕΤΑΙ ΘΕΩΡΗΤΙΚΗ ΑΝΑΛΥΣΗ ΤΗΣ ΑΠΟΔΟΣΗΣ (YIELD) ΜΙΑΣ ΑΝΤΙΔΡΑΣΗΣ ΣΥΝΤΟΝΙΣΜΟΥ ΣΤΗΝ ΠΕΡΙΠΤΩΣΗ ΕΝΟΣ ΑΠΛΟΥ ΔΕΙΓΜΑΤΟΣ (ΜΟΝΟΥ ΥΜΕΝΙΟΥ) ΚΑΙ ΕΝΟΣ ΔΙΠΛΟΥ ΔΕΙΓΜΑΤΟΣ. ΧΡΗΣΙΜΟΠΟΙΩΝΤΑΣ ΕΝΑ ΑΠΛΟΣΤΑΤΙΣΤΙΚΟ ΜΟΝΤΕΛΟ ΓΙΑ ΤΟ ΧΗΜΙΚΟ ΔΥΝΑΜΙΚΟ ΤΟΥ Η ΣΤΑ ΜΕΤΑΛΛΑ, ΓΙΝΕΤΑΙ ΠΡΟΣΠΑΘΕΙΑ ΕΞΗΓΗΣΗΣ ΤΩΝ ΣΥΓΚΕΝΤΡΩΣΕΩΝ ΤΟΥ ΥΔΡΟΓΟΝΟΥ ΠΟΥ ΜΕΤΡΗΘΗΚΑΝ ΣΤΑ ΔΥΟ ΣΤΡΩΜΑΤΑ ΤΩΝ ΔΙΠΛΩΝ ΔΕΙΓΜΑΤΩΝ (ΥΜΕΝΙΩΝ ΔΥΟ ΣΤΡΩΜΑΤΩΝ ΔΙΑΦΟΡΕΤΙΚΩΝ ΥΛΙΚΩΝ) ΠΡΙΝ ΚΑΙ ΜΕΤΑ ΤΗ ΘΕΡΜΙΚΗ ΕΠΕΞΕΡΓΑΣΙΑ."]},{"key":"dc:title","label":"Title","values":["ΜΕΛΕΤΗ ΤΗΣ ΚΑΤΑΝΟΜΗΣ ΥΔΡΟΓΟΝΟΥ ΣΕ ΛΕΠΤΑ ΥΜΕΝΙΑ ΔΥΟ ΣΤΡΩΜΑΤΩΝ ΔΙΑΦΟΡΕΤΙΚΩΝ ΜΕΤΑΛΛΩΝ"]}]}],"canonical_facts":{"dc:creator":["Πηλακούτα, Μυροφόρα"],"dc:date":["1988"],"dc:description":["THE RESONANCE AT E(15N)=6.39 MEV IN THE REACTION 1H(15N,ΑΓ)12C HAS BEEN EMPLOYED FOR THE DETERMINATION OF THE HYDROGEN DEPTH DISTRIBUTION IN SOME THIN FILMS OF METAL-HYDROGEN SYSTEMS ONTO A STAINLESS STEEL SUBSTRATE. THE INVESTIGATED FILMS WERE: THE SINGLE LAYER FILMS V-H AND TI-H AND THE THIN FILMS SANDWICHES (FILMS CONSISTING OF TWO THIN LAYERS OF DIFFERENT MATERIALS) TATI -H, TANB-H, NBTA-H AND TAV-H. THE PREPARATION OF THE SAMPLES BY MEANS OF UHV TECHNIQUE AND THEIRTREATMENT DURING THE LOADING PROCESS WITH HYDROGEN IS DESCRIBED. THE HYDROGEN TO METAL RATIOS IN THE TWO COMPONENTS OF EACH SANDWICH ARE QUANTITATIVE THE SAMPLES HAVE BEEN ANNEALED AT SEVERAL TEMPERATURES (IN THE RANGE BETWEEN 25 AND 400 C), AND AFTER COOLING DOWN TO ROOM TEMPERATURE THE PROFILE OF THE REMAINING HYDROGEN HAS BEEN MEASURED. THEORETICAL ANALYSIS OF THE YIELD DEDUCED FROM A RESONANCE REACTION IN THE CASES OF A SINGLE AND DOUBLE LAYER SAMPLE IS PRESENTED. AN EXPLANATION FOR THE HYDROGEN CONCENTRATION IN THE TWO LAYERS OF THE SANDWICHES BEFORE AND AFTER ANNEALING IS ATTEMPTED USING A SIMPLE STATISTICAL MODEL FORTHE CHEMICAL POTENTIAL OF H IN METALS.","Ο ΣΥΝΤΟΝΙΣΜΟΣ ΣΤΗΝ ΕΝΕΡΓΕΙΑ Ε=6.385 MEV ΤΗΣ ΑΝΤΙΔΡΑΣΗΣ Η(15Ν,ΑΓ)12C ΧΡΗΣΙΜΟΠΟΙΗΘΗΚΕ ΓΙΑ ΤΟΝ ΚΑΘΟΡΙΣΜΟ ΤΗΣ ΚΑΤΑ ΒΑΘΟΣ ΚΑΤΑΝΟΜΗΣ ΤΟΥ ΥΔΡΟΓΟΝΟΥ ΣΕ ΜΕΡΙΚΑ ΛΕΠΤΑ ΥΜΕΝΙΑ ΣΥΣΤΗΜΑΤΩΝ ΜΕΤΑΛΛΟ -ΥΔΡΟΓΟΝΟ ΠΑΝΩ ΣΕ ΥΠΟΣΤΡΩΜΑ ΑΝΟΞΕΙΔΩΤΟΥ ΧΑΛΥΒΑ. ΤΑ ΥΜΕΝΙΑ ΠΟΥ ΜΕΛΕΤΗΘΗΚΑΝ ΗΣΑΝ: ΤΑ ΥΜΕΝΙΑ ΕΝΟΣ ΣΤΡΩΜΑΤΟΣ V-H ΚΑΙ TI-H ΚΑΙ ΤΑ ΛΕΠΤΑ ΥΜΕΝΙΑ ΔΥΟ ΣΤΡΩΜΑΤΩΝ ΔΙΑΦΟΡΕΤΙΚΩΝ ΜΕΤΑΛΛΩΝ TATI-H, TANB-H, NBTA-H ΚΑΙ TAV-H. ΠΕΡΙΓΡΑΦΕΤΑΙ Η ΠΑΡΑΣΚΕΥΗ ΤΩΝ ΔΕΙΓΜΑΤΩΝ ΠΟΥ ΕΓΙΝΕ ΜΕ ΤΕΧΝΙΚΗ ΥΠΕΡ ΥΨΗΛΟΥ ΚΕΝΟΥ ΚΑΘΩΣΚΑΙ Ο ΧΕΙΡΙΣΜΟΣ ΤΟΥΣ ΚΑΤΑ ΤΗΝ ΔΙΑΔΙΚΑΣΙΑ ΦΟΡΤΙΣΗΣ ΜΕ ΥΔΡΟΓΟΝΟ. ΚΑΘΟΡΙΖΕΤΑΙ ΠΟΣΟΤΙΚΑ Ο ΛΟΓΟΣ ΥΔΡΟΓΟΝΟΥ ΠΡΟΣ ΜΕΤΑΛΛΟ ΣΤΑ ΔΥΟ ΣΤΡΩΜΑΤΑ ΤΟΥ ΚΑΘΕ ΔΙΠΛΟΥ ΔΕΙΓΜΑΤΟΣ(SANDWICH SAMPLE) ΚΑΙ ΕΞΕΤΑΖΕΤΑΙ Η ΚΑΤΑΝΟΜΗ ΤΟΥ ΥΔΡΟΓΟΝΟΥ ΠΟΥ ΠΑΡΑΜΕΝΕΙ ΣΤΑ ΔΕΙΓΜΑΤΑ ΜΕΤΑ ΑΠΟ ΘΕΡΜΙΚΗ ΕΠΕΞΕΡΓΑΣΙΑ IN-SITU ΣΕ ΔΙΑΦΟΡΕΣ ΘΕΡΜΟΚΡΑΣΙΕΣ (ΠΕΡΙΟΧΗ 25 ΕΩΣ 400 C) ΚΑΙ ΨΗΞΗ ΣΤΗ ΘΕΡΜΟΚΡΑΣΙΑ ΠΕΡΙΒΑΛΛΟΝΤΟΣ. ΠΑΡΟΥΣΙΑΖΕΤΑΙ ΘΕΩΡΗΤΙΚΗ ΑΝΑΛΥΣΗ ΤΗΣ ΑΠΟΔΟΣΗΣ (YIELD) ΜΙΑΣ ΑΝΤΙΔΡΑΣΗΣ ΣΥΝΤΟΝΙΣΜΟΥ ΣΤΗΝ ΠΕΡΙΠΤΩΣΗ ΕΝΟΣ ΑΠΛΟΥ ΔΕΙΓΜΑΤΟΣ (ΜΟΝΟΥ ΥΜΕΝΙΟΥ) ΚΑΙ ΕΝΟΣ ΔΙΠΛΟΥ ΔΕΙΓΜΑΤΟΣ. ΧΡΗΣΙΜΟΠΟΙΩΝΤΑΣ ΕΝΑ ΑΠΛΟΣΤΑΤΙΣΤΙΚΟ ΜΟΝΤΕΛΟ ΓΙΑ ΤΟ ΧΗΜΙΚΟ ΔΥΝΑΜΙΚΟ ΤΟΥ Η ΣΤΑ ΜΕΤΑΛΛΑ, ΓΙΝΕΤΑΙ ΠΡΟΣΠΑΘΕΙΑ ΕΞΗΓΗΣΗΣ ΤΩΝ ΣΥΓΚΕΝΤΡΩΣΕΩΝ ΤΟΥ ΥΔΡΟΓΟΝΟΥ ΠΟΥ ΜΕΤΡΗΘΗΚΑΝ ΣΤΑ ΔΥΟ ΣΤΡΩΜΑΤΑ ΤΩΝ ΔΙΠΛΩΝ ΔΕΙΓΜΑΤΩΝ (ΥΜΕΝΙΩΝ ΔΥΟ ΣΤΡΩΜΑΤΩΝ ΔΙΑΦΟΡΕΤΙΚΩΝ ΥΛΙΚΩΝ) ΠΡΙΝ ΚΑΙ ΜΕΤΑ ΤΗ ΘΕΡΜΙΚΗ ΕΠΕΞΕΡΓΑΣΙΑ."],"dc:identifier":["10.12681/eadd/0822","http://hdl.handle.net/10442/hedi/0822"],"dc:language":["gre"],"dc:publisher":["Πανεπιστήμιο Πατρών","University of Patras"],"dc:subject":["HYDROGEN CHEMICAL POTENTIAL","HYDROGEN DEPTH DISTRIBUTION","HYDROGEN DEPTH PROFILE WITH 15N-METHOD","HYDROGEN DEPTH PROFILE WITH I.B.M.","HYDROGEN DISTRIBUTION IN SANDWICH-FILMS","HYDROGEN PROFILE","HYDROGEN TECHNOLOGY","THERMODYNAMIC OF METAL HYDROGEN SYSTEM","ΑΝΑΛΥΣΗ ΚΑΤΑΝΟΜΗΣ ΥΔΡΟΓΟΝΟΥ","ΘΕΡΜΟΔΥΝΑΜΙΚΗ ΣΥΣΤΗΜΑΤΟΣ ΜΕΤΑΛΛΟ-ΥΔΡΟΓΟΝΟ","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥ","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥ ΜΕ ΜΕΘΟΔΟ -15Ν","ΚΑΤΑΝΟΜΗ ΥΔΡΟΓΟΝΟΥΣΕ ΔΙΠΛΑ ΥΜΕΝΙΑ","ΠΡΟΣΔΙΟΡΙΣΜΟΣ ΣΥΓΚΕΝΤΡΩΣΕΩΝ ΥΔΡΟΓΟΝΟΥ","ΤΕΧΝΟΛΟΓΙΑ ΥΔΡΟΓΟΝΟΥ","ΧΗΜΙΚΟ ΔΥΝΑΜΙΚΟ ΥΔΡΟΓΟΝΟΥ","Φυσικές Επιστήμες","Natural Sciences","Φυσική","Physical Sciences"],"dc:title":["ΜΕΛΕΤΗ ΤΗΣ ΚΑΤΑΝΟΜΗΣ ΥΔΡΟΓΟΝΟΥ ΣΕ ΛΕΠΤΑ ΥΜΕΝΙΑ ΔΥΟ ΣΤΡΩΜΑΤΩΝ ΔΙΑΦΟΡΕΤΙΚΩΝ ΜΕΤΑΛΛΩΝ"],"dc:type":["PhD Thesis"]},"updated_at":"2026-07-24T02:25:27Z"}