Lecture I

GA 320/1919-12-23/p029 ·1919-12-23 · English MediumMedium alignmentSome paragraph re-numbering between this translation and the German original — the locus may slip by a paragraph or two.
Record: unknown. How this text was taken down (shorthand transcript, listeners' notes or manuscript) is not on record here. Unknown is not an assurance of a stenogram: check the edition's own notes before resting an argument on one word.

This in effect is what we always look for, when speaking of the World in terms of Physics. All physical research amounts to this: we follow up the centric forces to their centres; we try to find the points from which effects can issue, For this kind of effect in Nature, we are obliged to assume that there are centres, charged as it were with possibilities of action in certain directions. And we have sundry means of measuring these possibilities of action; we can express in stated measures, how strongly such a point or centre has the potentiality of working. Speaking in general terms, we call the measure of a force thus centred and concentrated a “potential” or “potential force”. In studying these effects of Nature we then have to trace the potentials of the centric forces,—so we may formulate it. We look for centres which we then investigate as sources of potential forces.

Read this passage in another edition
DEoriginalENEnglish
Raw JSON: /v1/steiner/en/ga/320/1919-12-23/p029.json
Cite: GA 320/1919-12-23/p029 · edition English