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2. Our efforts in “proving the basic properties of fluids have so far been limited to the case of blocks. In this problem, wNow consider the shape below For this shape, you can assume that the pressure on the near parallelogram face and the far para

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2. A The pressure en botten face - Sgh where, Sis density. force on bottom face - P.A - 9gh lew) - Sglwh. D. Arg. pressure on

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