Hydraulic Fluid Power. Andrea Vacca

Чтение книги онлайн.

Читать онлайн книгу Hydraulic Fluid Power - Andrea Vacca страница 33

Автор:
Жанр:
Серия:
Издательство:
Hydraulic Fluid Power - Andrea Vacca

Скачать книгу

that

rho 2 equals StartStartFraction rho 1 OverOver 1 minus StartFraction normal upper Delta p Over upper B Subscript l Baseline EndFraction EndEndFraction

      we have

upper Q 2 equals upper Q 1 left-parenthesis 1 minus StartFraction normal upper Delta p Over upper B EndFraction right-parenthesis equals 100 left-bracket l slash italic min right-bracket dot left-parenthesis 1 minus StartFraction 100 left-bracket italic b a r right-bracket Over 18 000 left-bracket italic b a r right-bracket EndFraction right-parenthesis equals 99.44 l slash italic min

      Due to the effect of the fluid compressibility, the volumetric flow rate at the pump outlet is lower than the volumetric flow rate at the inlet by 0.56%.

      In this case, a certain amount of dissolved air is present at the pump inlet, being p1 < pT = pSAT. The amount of air at the inlet port 1 can be evaluated as

upper V Subscript a i r comma r comma 1 Baseline equals upper V Subscript s a t Baseline left-parenthesis 1 minus StartFraction p 1 Over p Subscript s a t Baseline EndFraction right-parenthesis left-parenthesis StartFraction p Subscript s a t Baseline Over p 1 EndFraction right-parenthesis Superscript StartFraction 1 Over gamma EndFraction

      where psat = pT, considering the process as isothermal (γ = 1):

upper V Subscript a i r comma r comma 1 Baseline left-parenthesis percent-sign right-parenthesis equals 0.09 left-parenthesis 1 minus StartFraction 0.7 Over 1 EndFraction right-parenthesis left-parenthesis StartFraction 1 Over 0.7 EndFraction right-parenthesis equals 0.09 dot 0.429 equals 0.039

      Therefore, the density of the fluid at the inlet section is

StartLayout 1st Row 1st Column rho 1 2nd Column equals 3rd Column alpha Subscript g Baseline rho Subscript g Baseline plus left-parenthesis 1 minus alpha Subscript g Baseline right-parenthesis rho Subscript l Baseline equals StartFraction upper V Subscript g Baseline Over left-parenthesis upper V Subscript l Baseline plus upper V Subscript g Baseline right-parenthesis EndFraction dot rho Subscript g Baseline plus left-parenthesis 1 minus StartFraction upper V Subscript g Baseline Over left-parenthesis upper V Subscript l Baseline plus upper V Subscript g Baseline right-parenthesis EndFraction right-parenthesis rho Subscript l Baseline 2nd Row 1st Column Blank 2nd Column equals 3rd Column 0.0375 dot 1.225 left-bracket italic k g slash m cubed right-bracket plus left-parenthesis 1 minus 0.0375 right-parenthesis dot 870 left-bracket italic k g slash m cubed right-bracket equals 837.4 italic k g slash m cubed EndLayout

      In the above expression, it is considered that the density of the air at standard conditions is ρg = 1.225 kg/m3.

      The density at the pump outlet can be calculated considering that at high pressure (p2 = 100 bar) all the fluid is liquid:

rho 2 equals StartStartFraction rho Subscript upper T Baseline OverOver 1 minus StartFraction normal upper Delta p Over upper B EndFraction EndEndFraction equals StartStartFraction 870 left-bracket italic k g slash m cubed right-bracket OverOver 1 minus StartFraction 100 left-bracket italic b a r right-bracket Over 18 000 left-bracket italic b a r right-bracket EndFraction EndEndFraction equals 874.9 italic k g slash m cubed

      Therefore, from the expression

rho 1 upper Q 1 equals rho 2 upper Q 2

      we have

upper Q 2 equals upper Q 1 StartFraction rho 1 Over rho 2 EndFraction equals 100 left-bracket l slash min right-bracket dot StartFraction 837.4 left-bracket italic k g slash m cubed right-bracket Over 874.9 left-bracket italic k g slash m cubed right-bracket EndFraction equals 95.7 left-bracket l slash min right-bracket

      It is therefore possible to observe how, in this (gaseous) cavitation condition, the reduction in outlet flow is about 4.3%, much more pronounced with respect to the case (a), where there was no cavitation.

      A final remark can be made on the evaluation of the equivalent (or effective) bulk modulus. For the typical operating pressure of hydraulic control systems, the elasticity of the material is also not negligible. Consider again the case of Figure 2.12 while also including the elasticity of the walls according to the bulk modulus of the material (similar to the Young modulus definition):

      (2.33)upper B Subscript m a t Baseline equals minus upper V Subscript t o t Baseline left-parenthesis StartFraction normal upper Delta p Over normal upper Delta upper V Subscript m a t Baseline EndFraction right-parenthesis

      The equivalent bulk modulus for the system becomes

      (2.34)upper B Subscript t o t Baseline equals left-bracket StartFraction alpha Subscript g Baseline Over upper B Subscript g Baseline EndFraction plus StartFraction alpha Subscript v Baseline Over upper B Subscript v Baseline EndFraction plus StartFraction left-parenthesis 1 minus alpha Subscript g Baseline minus alpha Subscript v Baseline right-parenthesis Over upper B Subscript l Baseline EndFraction plus StartFraction 1 Over upper B Subscript m a t Baseline EndFraction right-bracket Superscript negative 1

      A hydraulic oil is subject to various forms of contamination:

       Solid contamination. The solid contamination is the most common and intuitive form of contamination; it affects the operation and life of all hydraulic circuits. The solid contamination is due to the presence of undesired solid particles (metallic, plastic, fibers of different types, etc.) within the hydraulic fluid. These particles can accelerate the wear of the hydraulic components or produce the blockage of small flow connections (such as those of small hydraulic orifices). Solid contamination can cause malfunctioning of the hydraulic system and can also lead to the catastrophic failure of some components, like pumps and motors.

       Liquid contamination. In general terms, liquid contamination refers to the presence of other liquids in the working fluid that can either be chemically aggressive to the hydraulic components or can deteriorate the properties of the hydraulic fluid. In the majority of the cases, the liquid contaminant is water. For example, water causes rusting in hydraulic components (which can be visible, for example, in the reservoir of the system), reduces the lubrication characteristics of the oil, and can cause unwanted reactions leading to the formation of alcohols, acids, or sludges. In addition, water has a higher vapor pressure values when compared with typical oils. Therefore, the presence of water can lead to instances of vapor cavitation that can cause instabilities and damages of the mechanical parts.

       Gas contamination. Gas contamination usually refers the presence of undissolved or entrained air in the hydraulic oil. As mentioned before, this can lead to the premature wear of certain hydraulic components,

Скачать книгу