Steam Tables (Table 3. Vapor, page 18)

                       

                                     differences in flow pattern and general behavior,

having significantly different physical characteristics.

= (e_ji + w_ij) A_j,                                                 combustion or evaporation,

             e_ji = ½ (u_j,i + u_i,j),                   w_ij = ½ (u_j,i - u_i,j).

the e_ji and w_ij were constants and so small that their products < 0

                                                                                   

                                                                                         1   2            1   2 

                                                                                    e₁ A_j A_j  = e_jk  A_k A_j 

Steam Tables (Table 3. Vapor, page 16)

                        INTRODUCTORY CONCEPT

CHAPTER I

            If               science like fluid

If                                         passes through

If for every                                      between

            Love: A

be replaced by                         A & B

                                                                            of A₁, A₂, A₃, we must have

                                                                                               BODY FORCES.

                                                                    point of the body

                        F is                                                      Likewise a body originally

                                                                    are apt to lead to a false conclusions.

                                                                        l is multiply connected,

Steam Tables (Table 3. Vapor, page 14)

(a)   Air, (2) hydrogen, (c) uranium hexafluoride, (d) mercury vapor

1.     Body (or volume) force; that is;

   Let a body    be

                                                                                                if we neglect   

                                                                                    product of A’ and B’, we have

It is a matter of experience                                                                     be

                                                                                                 A    we have

                                                                                                         we must

            , the word “heat” in

                                    fluids.

                                                                                    shows that we must have

                                                                                                  PERFECT FLUIDS.

                                                                                               into the tank.

Steam Tables (Table 2. Saturation: Pressures, page 12)

His help was invaluable.                                 ANALYSIS OF STRAIN

                             In order that the solution of the problem may exist,

                                                      We introduce the definition of the unstrained or

                                                            we may consider a mixed boundary-value problems

                        Thus, the boundary is made up of two circles

   Consider a pair of harmonic

Steam Tables (Table 2. Saturation: Pressures, page 10)

 

                                                           Mathematische Annalen, vol. 75 (1914) pp. 497-544;

                                                1. Introduction

the rigid body motion

                                    (due to Wx alone)

                                                                        J in                 

                                                                              A and L. Föppl have disucussed

elasticians,

                                   

 

Paris,

            Boundary-value problems of elasticity:

                               Berlin,    present age might well turn out to be the period of transition

London,

            in 1941 and 1942 in the Program of Advanced Instruction and

                                                                        (10)

                                    the stress-strain relations can be found experimentally,

                              

Steam Tables (Table 1. Saturation: Temperatures)

                                                                  

 

                                                                                    The basics concepts,

the examples which they permit to be worked out often provide

                                                            A clue to the nature of this

                                                                                                COMPRESSIBLE FLOW

                                    GOVERNING RELATIONS

                                                   Changes from one point to another.

                                                                                    In an intangible yet real way.

Sylvia                         

                        Frictionless.

                                                                                           May thus be transferred to

                        Ralph A.                                                                                          Bruce

                                                            Young Peter,

            Since it expresses the obvious fact

                                                            Later we shall identify this type of interaction

Finally, but by no means least,

                           I must express a word

                                                                                    I hope that I have not failed

                       

                                                                                                            April 4, 1953

                                                                                                        Arlington, Mass.

                                                                 - Continued

Steam Tables: Vapor, Liquid and Solid Relations (Preface)

Welcome to "Altered Book Pages" blog! Here, I'll post my works and doodling on old book pages.
 
The first post is from "Steam Tables: Vapor, Liquid and Solid Relations." I used physics and mathematical information to develop a theory on relationships. Following the order of a book from the face page, content, preface, chapter I, II and III and appendix and so forth, I created a number of different levels of narratives in this work. Texts on the bottom of each page flow from page to page, while the imagery of fluids spill over, leak into and cut through to create another level of narratives.  Texts and altered images from two books, "The Dynamics and Thermodynamics of Compressible Fluid Flow" (1953) and "Mathematical Theory of Elasticity" (1946), are combined onto pages from "Steam Tables" (1969). It is best to see the whole work as an installation.

Below: texts from one of these pages. Images are at the bottom. Here, I'll post the first four pages.

a relief map of the flow field in which the vertical elevation is

                                                                               Measurement of work

                                                                                        from condition 1 to condition 2

                                                                        the heat “received” by Q,

w=pAc

a more or less

            Work.

                                                                                                   WORK RECEIVED.

                                                between two

                                                                           100°F,                                  may be computed

                                                                                    the amount of heat rejected by

            =0.

                                                                              the shock becomes vanishingly small.

                                                            Superposition (a) and (b),

                                                                        RECOGNITION OF WORK

P2-P1=                                                                            (that is, div F=Ñ2j=0).

                                                F=Ñj

            forces are prescribed

P2 is

                        a perpetual motion machine

                                                The machine experiences different histories.

between two heat reservoirs

                        throat and test section.

                                    EQUALITY OF TEMPERATURE

            EQUAL-TEMPERATURE PROCESS.                         it is useless to speak of such things

                                                                                                                                    p=p(x,y, z)

(107)

TEMPERATURE.  The concept of inequality