Conservation and Innovation : Helmholtz's Struggle with Energy ...

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Teichmann, Jurgen. "L'influenza di A.Volta in Germania." Quaderni del Giornale di Fisica 3 (1979): . Theobald, David. The Concept of Energy. London: Spon, 1966. Thomson,W. and Tait, P.G. Treatise on Natural Philosophy. Oxford, 1867. Truesdell, Clifford. The Tragicomic History of Thermodynamics. 1822-1854. New York: Springer,1980. Turner, Steven. "Hermann von Helmholtz." In DSB 6 ,1973. Pp.241-53. Weber, Wilhelm. "Elektrodynamische Maassbestimmungen über ein allgemeines Grundgesetz der Elektrischen Wirkung." 1846. In Werke 6 vols. Berlin, 1892-4. Vol.3, pp.25-214. Weber, Wilhelm. "Elektrodynamische Maassbestimmungen" In Pogg Ann 73 (1848): 193. Tr. in Taylor's Scientific Memoirs 5 (1852): 489-529. Weber, Wilhelm. "Elektrodynamische Maassbestimmungen, insbesonder uuber das Prinzip der Erhaltung der Energie." 1871. In Werke 6 vols. Berlin, 1892-4. Vol.4. Pp. 247-99. Tr. in Phil Mag 43 (1872): 1-20 and 119-49. Williams, Peirce. "Kant, Naturphilosophie and Scientific Method." In Foundations of Scientific Method: The Nineteenth Century. Ronald Giere and Richard Westfall (eds). Bloomington: Indiana U.P., 1973. Pp.3-22. Winters, Stephen. "Hermann von Helmholtz's Discovery of Force Conservation." Dissertation. The John Hopkins University, 1985. Wise, Norton. "W.Thomson's Mathematical Route to Energy Conservation: a Case Study of the Role of Mathematics in Concept Formation." In HSPS 10 (1979) : 49-83. Wise, Norton. "German Concepts of Force, Energy and the Electromagnetic Ether: 1845-1880" In Conceptions of Ether. G.N. Cantor and M.J.S.Hodge eds. Cambridge : Cambridge U.P., 1981. Pp.269-307. Wise, Norton and Smith, Crosbie. "Measurement, Work and Industry in Lord Kelvin's Britain." In HSPS 17 (1986): 147-73 Wise, Norton and Smith, Crosbie. Energy and Empire: William Thomson, Lord Kelvin, 1824-1907. Cambridge University Press. Harper, 1960. Whittaker, E. A History of the Theories of Aether and Electricity 2nd ed. New York: Wolff,Stefan."Clausius' way to the kinetic theory-the beginnings of theoretical physics in Germany." Forthcoming. Woodruff, A.E. "The Contributions of H.v.Helmholtz to Electrodynamics." In Isis 59 (1968): 300-11.
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Page 1 and 2:
Fabio Bevilacqua Conservation and I
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different formulations 4 and priori
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and interesting results, despite th
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principle of correlation is express
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principle to the existing empirical
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the origin and meaning of the princ
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Whether physiological research, apa
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In a discussion on the origins of a
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his "Wärme" that one of the differ
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generate a determined equivalent of
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"Bericht", despite the application
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experiments in the most disparate b
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The premise reveals that the struct
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intelligible if it can be referred
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elevant consequence of the deductio
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Needless to say the plan was to be
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and from here that the direction an
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since Leonardo 113; the "ad nihilum
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But unfortunately for the whole str
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The principle of conservation of vi
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different from the one joining the
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"The equality that exists between e
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In virtue of its limitations to New
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Helmholtz, while asserting that lig
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the temperature of 1 Kg of water ca
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In his search for a mechanical equi
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had already been achieved in the Be
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approach is discussed at length and
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and unaware of Green's results190,
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potential function 201. It is worth
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and judged unreliable, despite prov
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The relevance of the first question
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principle taking this potential int
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Finally we get to the real conclusi
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conservation 234, on the theory of
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for the mechanical equivalent of he
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The controversy started with some r
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where μ are immovable masses, m th
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demonstration criticised by Clausiu
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directions that join them and whose
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quotes 288 and criticises a proposi
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motion to all natural forces, the k
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measure this expenditure and compar
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" ...the quantity of force in natur
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forces is constant: but it relates
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experiences in general laws of unli
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"a series of important and difficul
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the Discontinuous Movements of Flui
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methodology. Dühring claimed the c
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The first history of the conservati
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while in Britain for the above talk
Page 103 and 104: apply it to acoustics (1859), hydro
Page 105 and 106: magnetic intensity. Maxwell realize
Page 107 and 108: and the electrostatic In modern not
Page 109 and 110: of conservation of energy: it is re
Page 111 and 112: efuted. But again in 1881 Helmholtz
Page 113 and 114: But was important here is that desp
Page 115 and 116: The second (1892-94), follows the i
Page 117 and 118: while the electromagnetic and the s
Page 119 and 120: can modify its specific theoric for
Page 121 and 122: considered relevant. In Poincarè
Page 123 and 124: meaning left is: "There is somethin
Page 125 and 126: interpretations at the beginning of
Page 127 and 128: while fighting metaphisicians, he w
Page 129 and 130: literature 456. There is an intrins
Page 131 and 132: assertion is surprising: it has lon
Page 133 and 134: Kant was a Naturphilosophe 480. The
Page 135 and 136: condition that work done by the for
Page 137 and 138: histories cites these (Hirn's) arti
Page 139 and 140: ) the experimental determinations o
Page 141 and 142: force principle 522. Elkana tried t
Page 143 and 144: Blüh, Otto. "The Value of Inspirat
Page 145 and 146: Graetz, L. "Das Mechanische Wärme
Page 147 and 148: Helmholtz, Hermann. "Bericht über
Page 149 and 150: Helmholtz, Hermann. Wissenschaftlic
Page 151 and 152: Madison: Wisconsin U.P., 1959. Pp.
Page 153: Poincarè, Henry. Electricité et O
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