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An Introduction to the theory of statistics

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Bibliographic data

Contents: An Introduction to the theory of statistics

Monograph

Identifikator:
1028803699
URN:
urn:nbn:de:zbw-retromon-43559
Document type:
Monograph
Author:
Fisher, Irving http://d-nb.info/gnd/118533541
Brown, Harry Gunnison http://d-nb.info/gnd/123548152
Title:
Die Kaufkraft des Geldes
Place of publication:
Berlin
Publisher:
Druck und Verlag von Georg Reimer
Year of publication:
1916
Scope:
1 Online-Ressource (XX, 435 Seiten)
Digitisation:
2018
Collection:
Economics Books
Usage license:
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Chapter

Document type:
Monograph
Structure type:
Chapter
Title:
IV. Kapitel. Störung der Gleichung und der Kaufkraft in Perioden des Übergangs
Collection:
Economics Books

Contents

Table of contents

  • An Introduction to the theory of statistics
  • Title page
  • Part I. The theory of atributes
  • Part II. The theory of variables
  • Part III. Theory of sampling
  • Index

Full text

te THEORY OF STATISTICS. 
B were independent in the universe of (’s, and the corresponding 
differences for the frequencies (4B), (AC), and (BC). The four 
quantities in the brackets on the right represent, say, the four 
known associations, the bracket on the left the unknown association. 
Clearly, the relation is not of such a simple kind that the term on 
the left can be, in general, mentally evaluated. Hence in con- 
sidering the choice and number of associations to be actually 
tabulated, regard must be had to practical considerations rather 
than to theoretical relations. 
13. The particular case in which all the 2” —n +1 given associa- 
tions are zero is worth some special investigation. 
It follows, in the first place, that all other possible associations 
must be zero, z.e. that a state of complete independence, as we 
may term it, exists. Suppose, for instance, that we are given— 
(4)(B) _(4)(©) 
(4B) = 7 (40) = v 
_(B)C) _(4OXBO) _ (4)(B)(C) 
(BC) aN (4B0C) Tw (0) Ce 
Then it follows at once that we have also— 
AB)(BC) (4B)(AC) 
A450) = EENBC) (ABYC, 
ents a 
t.e. 4 and C are independent in the universe of B’s, and B and C 
in the universe of 4’s. Again, 
= (AE) _ DB) _ (A)XB)C) 
(4By)=(4B) - (4BC) = Sa 
_ AB) _ 4y)(By) 
re (r) 
Therefore 4 and B are independent in the universe of fs. 
Similarly, it may be shown that 4 and C' are independent in the 
universe of 8’s, B and C in the universe of a’s. 
In the next place it is evident from the above that relations of 
the general form (to write the equation symmetrically) 
“BO _(1) (#) (©) = 
N x. aN : 2 
must hold for every class-frequency. This relation is the general 
form of the equation of independence, (2) (d), Chap. III. (p. 26). 
14. It must be noted, however, that (8) is not a criterion for the 
56
	        

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Zur Geschichte Und Theorie Des Bergregals Und Der Bergbaufreiheit. J. Bielefelds Verlag, 1916.
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