
By Khinchin A.
Read Online or Download A course of mathematical analysis PDF
Similar geometry books
Contact Geometry and Linear Differential Equations
The purpose of the sequence is to offer new and critical advancements in natural and utilized arithmetic. good validated locally over twenty years, it bargains a wide library of arithmetic together with a number of vital classics. The volumes offer thorough and unique expositions of the tools and concepts necessary to the subjects in query.
This paintings covers the lawsuits of the NSF-CBMS convention on 'Spectral difficulties in Geometry and mathematics' held on the college of Iowa. The important speaker used to be Peter Sarnak, who has been a imperative contributor to advancements during this box. the amount methods the subject from the geometric, actual, and quantity theoretic issues of view.
- The Pythagorean Theorem: A 4,000-Year History
- Elementary geometry from an advanced standpoint
- Origami 3: Third International Meeting of Origami Science, Mathematics, and Education Sponsored by Origami USA
- Space, Time and Geometry
- Geometry of Non-Linear Differential Equations, Backlund Transformations, and Solitons, Part B
Additional resources for A course of mathematical analysis
Example text
Since the vector eo and the curve p(t) were arbitrarily chosen, the leaves of the foliation Al> passing through the points p(O) and p(I), are parallel, and subsequently each of them is autoparallel. Using the same method, one easily prove the theorem for the leaves of the foliation A2. 59) imply that e;, = e (eDlt=t= d(e; + e~) + (e{ + e4)w~ = 0, and a vector tangent to a leaf F3 of the third foliation is defined by the condition e~ + e~ = 0, then the previous statement also valid for the third foliation A3 .
101 ) 36 1. , a ",J°kl . = a",J,°kl - . 101), satisfy the following conditions: *i ~[jkll _ - 0 , *i ~jkl *i *i + ~jkl + gjkl = 0. 103) The tensors ~;kl are covariant derivatives of the torsion tensor a~k with respect to the middle connection f (see Problem 19). Consider the following identity: which can be easily verified. 104) This is the desired decomposition of the curvature tensor b~kl. Thus, the curvature tensor b~kl is represented as the sum of the summands of three types: the first is expressed in terms of the torsion tensor, the second is expressed in terms of the covariant derivatives of the torsion tensor with respect to the middle * and the third does not depend on the torsion tensor.
A",J,°kl - . 101), satisfy the following conditions: *i ~[jkll _ - 0 , *i ~jkl *i *i + ~jkl + gjkl = 0. 103) The tensors ~;kl are covariant derivatives of the torsion tensor a~k with respect to the middle connection f (see Problem 19). Consider the following identity: which can be easily verified. 104) This is the desired decomposition of the curvature tensor b~kl. Thus, the curvature tensor b~kl is represented as the sum of the summands of three types: the first is expressed in terms of the torsion tensor, the second is expressed in terms of the covariant derivatives of the torsion tensor with respect to the middle * and the third does not depend on the torsion tensor.