Theoretical Studies Concerning the Hydropulse
Theoretical Studies Concerning the Hydropulse
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In our eReader you can find the full English version of the book. Read Theoretical Studies Concerning the Hydropulse Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Theoretical Studies Concerning the Hydropulse
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To quickly assess the difficulty of the text, read a short excerpt:
82 . 069 1. 57 . 84 . 068 7 = 1. 1 '1 ~ ° V = 0. 5 ° f v^= . 01 V. = 3 1. 373 . 302 1. 366 . 301 7 = 1. 3 v^ = v„= . 416 v^= . 024 ^1 ~ -^ 1. 198 . 570 1. 188 . 566 CONFIDENTIAL 46 COMPIDENTIAL A3 the table shows, the approximate formula appears to be quite accurate over a wide range of parameter values.
In the following table a few conparlsons of exact and approximate values for the time of stroke dimensionless form, cf. Section 4) are given: T3 (in Cases Time of Stroke Tg Approximate Exact 7 ...= 1. 1 Vj^ = . 01 Vg = 0. 5 v;. O v; = 3 . 353 . 148 . 392 . 150 7 = 1. 3 v^ = . 024 V3 = . 416 v; = o vl=l . 319 . 248 . 370 • 259 As remarked above, the approximate formula for the time of t stroke becomes more accurate when the initial velocity (v.
in dimensionless form) increases.
As we have seen in the preceding section, our formula for I_ gives an upper bound for this quantity. The formula s for t_, as we have seen, furnishes a lower bound, and consequently the formula for P_ yields an upper bound.
What to read after Theoretical Studies Concerning the Hydropulse?
You can find similar books in the "Read Also" column, or choose other free books by James Johnston Stoker to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
82 . 069 1. 57 . 84 . 068 7 = 1. 1 '1 ~ ° V = 0. 5 ° f v^= . 01 V. = 3 1. 373 . 302 1. 366 . 301 7 = 1. 3 v^ = v„= . 416 v^= . 024 ^1 ~ -^ 1. 198 . 570 1. 188 . 566 CONFIDENTIAL 46 COMPIDENTIAL A3 the table shows, the approximate formula appears to be quite accurate over a wide range of parameter values.
In the following table a few conparlsons of exact and approximate values for the time of stroke dimensionless form, cf. Section 4) are given: T3 (in Cases Time of Stroke Tg Approximate Exact 7 ...= 1. 1 Vj^ = . 01 Vg = 0. 5 v;. O v; = 3 . 353 . 148 . 392 . 150 7 = 1. 3 v^ = . 024 V3 = . 416 v; = o vl=l . 319 . 248 . 370 • 259 As remarked above, the approximate formula for the time of t stroke becomes more accurate when the initial velocity (v.
in dimensionless form) increases.
As we have seen in the preceding section, our formula for I_ gives an upper bound for this quantity. The formula s for t_, as we have seen, furnishes a lower bound, and consequently the formula for P_ yields an upper bound.
What to read after Theoretical Studies Concerning the Hydropulse?
You can find similar books in the "Read Also" column, or choose other free books by James Johnston Stoker to read onlineMoreLess
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