Page 250 - Introduction to Naval Architecture
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PROPULSION                          255

         correctly scaled pressure as is done in a special depressurised tomng tank
         facility at MARIN in the Netherlands. The tank is 240 m long, 18m wide
         with a water depth of 8 m. The pressure in the air above the water can
         be reduced to 0.03 bar. The more usual approach is to use a cavitation
         tunnel

         Cavitation number
                               2
        The value (p 0 - p v)/pV  or (p 0 - p^)/\pV^ is called the cavitation
         number. Water contains dissolved air and at low pressures this air will
         come out of solution and below a certain pressure, the vapour pressure
         of water, water vapour forms. Hence, as the pressure on the propeller
         blade drops, bubbles form. This phenomenon is called cavitation and
         will occur at a cavitation number given by:

             cavitation number, <j = (p a - e)/\pV*

         where e is water vapour pressure.
           The actual velocity experienced, and the value of p 0, vary with
         position on the blade. For a standard, a representative velocity is taken
         as speed of advance of the propeller through the water and p 0 is taken
         at the centre of the propeller hub. For a local cavitation number the
         actual velocity at the point concerned, including rotational velocity and
         any wake effects, and the corresponding p 0 for the depth of the point
         at the time must be taken. Blade elements experience different
         cavitation numbers as the propeller rotates and cavitation can come
         and go.

         Occurrence and effects of cavitation
         Since cavitation number reduces with increasing velocity cavitation is
         most likely to occur towards the blade tips where the rotational
        component of velocity is highest. It can also occur near the roots, where
         the blade joins the hub, as the angle of incidence can be high there.
        The greatest pressure reduction on the back of the blade occurs
        between the mid-chord and the leading edge so bubbles are likely to
        form there first. They will then be swept towards the trailing edge and
        as they enter a region of higher pressure they will collapse. The collapse
        of the bubbles generates very high local forces and these can damage
        the blade material causing it to be 'eaten away'. This phenomenon is
        called erosion.
          Water temperature, dissolved air or other gases, and the presence of
        nuclei to provide an initiation point for bubbles, all affect the pressure at
        which cavitation first occurs. Face cavitation usually appears first near the
        leading edge of the section. It results from an effective negative angle of
        incidence where the wake velocity is low. This face cavitation disappears
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