{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,10,26]],"date-time":"2026-10-26T01:43:44Z","timestamp":1792979024296,"version":"4.5.0"},"reference-count":33,"publisher":"Wiley","issue":"14","license":[{"start":{"date-parts":[[2006,3,15]],"date-time":"2006-03-15T00:00:00Z","timestamp":1142380800000},"content-version":"vor","delay-in-days":34407,"URL":"http:\/\/onlinelibrary.wiley.com\/termsAndConditions#vor"}],"content-domain":{"domain":["onlinelibrary.wiley.com"],"crossmark-restriction":true},"short-container-title":["Annalen der Physik"],"published-print":{"date-parts":[[1912,1]]},"DOI":"10.1002\/andp.19123441404","type":"journal-article","created":{"date-parts":[[2007,5,29]],"date-time":"2007-05-29T21:52:16Z","timestamp":1180475536000},"page":"789-839","update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":1758,"title":["Zur Theorie der spezifischen W\u00e4rmen"],"prefix":"10.1002","volume":"344","author":[{"given":"P.","family":"Debye","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"311","published-online":{"date-parts":[[2006,3,15]]},"reference":[{"key":"e_1_2_1_1_2","doi-asserted-by":"publisher","DOI":"10.1002\/andp.19063270110"},{"key":"e_1_2_1_2_2","unstructured":"M.Planck W\u00e4rmestrahlung p.157. 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Paris"},{"key":"e_1_2_1_11_2","unstructured":"Vgl.M.Planck W\u00e4rmestrahlung Leipzig1906. p.161."},{"key":"e_1_2_1_12_2","unstructured":"Es sei noch bemerkt da\u00df es nach (13) keine Temperatur mehr geben kann f\u00fcr welche bei tiefen Temperaturen die Strahlungsenergie gr\u00f6\u00dfer w\u00e4re wie die Energie der Atome wie das sowohl nach der Einsteinschen wie nach derNernst\u2010LindemannschenFormel f\u00fcr alle K\u00f6rper der Fall ist es sei denn da\u00df K\u00f6rper existieren deren charakteristische Temperatur \u0398 gr\u00f6\u00dfer wie 135000\u00b0 w\u00e4re."},{"key":"e_1_2_1_13_2","unstructured":"Die Zahlenwerte wurden nicht neu gerechnet sondern den Tabellen vonB.Pollitzer: Die Berechnung chemischer Affinit\u00e4ten nach dem Nernstschen W\u00e4rmetheorem Stuttgart1912 p.165entnommen bzw. durch Interpolation zwischen den dort angegebenen Zahlen berechnet."},{"key":"e_1_2_1_14_2","unstructured":"Vgl. noch die Bemerkung auf p.805 \u00a7 3."},{"key":"e_1_2_1_15_2","doi-asserted-by":"crossref","unstructured":"W.Nernst\u2010Lindemann Zeitschr. f. Elektrochem.p.817.1911.","DOI":"10.1002\/bbpc.19110171809"},{"key":"e_1_2_1_16_2","unstructured":"Die KonstanteAzur Umrechnung vonCpaufCvscheint etwas zu niedrig gegriffen. Wir haben aber absichtlich keine \u00c4nderung an der vonNernstundLindemannangegebenen Zahl angebracht."},{"key":"e_1_2_1_17_2","unstructured":"Man braucht die Rechnungen nat\u00fcrlich nicht mehr wirklich auszuf\u00fchren sondern kann in der Tabelle des \u00a7 2 interpolieren. Um ganz sicher zu gehen haben wir in diesem Falle aber die Interpolation vermieden und neu gerechnet."},{"key":"e_1_2_1_18_2","unstructured":"Wir vernachl\u00e4ssigen dabei die Differenz zwischenCpundCv was bei den Temperaturen welche hier in Betracht kommen ohne weiteres zul\u00e4ssig ist."},{"key":"e_1_2_1_19_2","first-page":"41","volume":"38","author":"Paschen\u2010Gerlach","year":"1912","journal-title":"Ann. d. Phys."},{"key":"e_1_2_1_20_2","doi-asserted-by":"publisher","DOI":"10.1002\/andp.19113390110"},{"key":"e_1_2_1_21_2","first-page":"838","volume":"22","author":"Gr\u00fcneisen E.","year":"1907","journal-title":"Ann. d. Phys."},{"key":"e_1_2_1_21_3","first-page":"845","volume":"25","year":"1908","journal-title":"Ann. d. Phys."},{"key":"e_1_2_1_22_2","unstructured":"Vgl.A. E. H.Love Lehrbuch der Elektrizit\u00e4t. \u00dcbersetzung vonTimpe Leipzig1907. p.320und die dort angegebene Literatur."},{"key":"e_1_2_1_23_2","unstructured":"Vgl.A. E. H.Love l. c. p.123. Man bedenke da\u00df der dort definierte Kompressionsmodulkgleich dem reziproken Werte der Kompressibilit\u00e4txist."},{"key":"e_1_2_1_24_2","first-page":"61 ff.","volume":"30","author":"Debye P.","year":"1909","journal-title":"Ann. d. Phys."},{"key":"e_1_2_1_25_2","first-page":"64","volume":"30","author":"Debye P.","year":"1909","journal-title":"Ann. d. Phys."},{"key":"e_1_2_1_26_2","first-page":"179","volume":"1","author":"Maxwell J. C.","year":"1881","journal-title":"Treatise on electricity and magnetism, Oxford"},{"key":"e_1_2_1_27_2","doi-asserted-by":"publisher","DOI":"10.1007\/BF01450097"},{"key":"e_1_2_1_27_3","unstructured":"Die Formeln sind auch zusammengestellt beiE.Jahnkeu.F.Emde: Funktionentafeln Leipzig1909. p.102."},{"key":"e_1_2_1_27_4","unstructured":"\u00c4hnliche Rechnungen wie die unsrigen finden sich beiJ.Reudler Diss. Leiden1912 in welcher das elektromagnetische Feld in einer Kugel mit R\u00fccksicht auf die Jeanssche Ableitung des Strahlungsgesetzes untersucht wird."},{"key":"e_1_2_1_28_2","unstructured":"Vgl.P.Debye Math. 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