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  1. Zwischen scylla und charybdis.Adolf Meyer - 1936 - Acta Biotheoretica 1 (3):203-218.
    In comparing it with the mechanistic and vitalistic views, the author seeks to make clear the nature of holistic causality, referring toDonnan's equations as an example.Holistic causality is essentially dimensional simplification. A complex system which forms a whole must be described in the first instance autonomo-phenomenologically, and if possible mathematically. Thereafter it is simplified into other wholes of less dimensionality, through progressive elimination of its higher dimensions, and so on until there remain over constituents no longer showing „wholeness”. These are (...)
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  • Der feldbegriff in seiner anwendung auf Das problem der zellteilung.Alex Gurwitsch & Lydia Gurwitsch - 1936 - Acta Biotheoretica 2 (2):77-92.
    The authors show that in certain isolated tissues the mitotic processes continue during at least one hour. They are very strongly stimulated by heat and also by mitogenetic radiation. In the case of the cancer cells new mitoses are promoted in considerable number. A detailed analysis of both energy factors leads to the conclusion that they effect a disturbance of the unstable constellations of the elementary particles in the cell-body. Thus a certain degree of disorganisation of its plasma seems to (...)
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  • Die hypothese der keimgangmutationen.E. Ungerer - 1936 - Acta Biotheoretica 2 (1):23-58.
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  • (1 other version)Philosophie der Naturwissenschaften.Gerhart Saenger - 1938 - Philosophical Review 47:552.
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  • Zur kritik Des „holismus”.Hans Driesch - 1936 - Acta Biotheoretica 1 (3):185-202.
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  • Integral analysis and the phenomena of lifeDie Integralanalyse und die LebenserscheinungenL'Analyse intégrale et les phénomènes de la vie.F. G. Donnan - 1936 - Acta Biotheoretica 2 (1):1-11.
    Der Beschreibung der zeitlichen Entwicklung lebender Systeme kann eine reine Differentialanalyse nicht genügen. In solchen Fällen muss man sich an Stelle der gewöhnlichen Differentialgleichungen der integraldifferentiellen, bezw. der Integralgleichungen bedienen. Zur leichteren Veranschaulichung der mathematischen Darstellung betrachtet Verfasser zuerst diejenigen Systeme, deren innerer Zustand sich durch ein einziges Parameterc bestimmen lässt. Die zeitliche Entwicklung eines leblosen Systems dieser Klasse werde durch die Differentialgleichung $$\frac{{dc}}{{dt}} = kf...$$ dargestellt, wot=Zeit, undk eine Funktion der äusseren Parameterα, Β, γ. ist. Im Falle eines jeden (...)
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