Pressure difference in a bucket sitting in an elevator

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When a bucket filled with an incompressible fluid is in an elevator accelerating downwards, the pressure difference between two points separated by a vertical distance, delta h, is given by the equation ΔP = ρ(g - a)Δh. This accounts for the effective gravitational force being reduced by the elevator's downward acceleration, a. The analysis involves considering the forces acting on different layers of fluid within the bucket. The pressure at the bottom layer is influenced by the weight of the fluid above it and the acceleration of the elevator. Thus, the correct formulation reflects the modified gravitational effect due to the elevator's motion.
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if a bucket is on an elevator floor in a inconpressible fluid of density p. When the elevator is accelerating downards, what is the pressure difference between two points in a fluid, separated by a vertical distance of delta h.

I was thinking that it is p (g - a) delta h, since it should be taking away from g, but could it be g + a, or could the whole equation be pa delta h, p g delta h, or p g a delta h, because of the inconpressiblity and/or the possiblity of the pressure being the same, can i have some hints on this please, thanks.
 
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mikezietz said:
if a bucket is on an elevator floor in a inconpressible fluid of density p. When the elevator is accelerating downards, what is the pressure difference between two points in a fluid, separated by a vertical distance of delta h.

I was thinking that it is p (g - a) delta h, since it should be taking away from g, but could it be g + a, or could the whole equation be pa delta h, p g delta h, or p g a delta h, because of the inconpressiblity and/or the possiblity of the pressure being the same, can i have some hints on this please, thanks.
Think of the bucket of water in terms of three layers of water - just masses sitting on top of each other. The weight of the lowest mass is m_1g = \rho h_1Ag, the second is m_2g = \rho \triangle hAg and the uppermost is m_3g = \rho h_3 Ag where A is the area of the bucket (assume the bucket has vertical sides).

When the bucket is at rest, the top layer (m3) is exerting an downward force Fdn3 of m3g on m2.

At rest:

m_3g - F_{dn3} = m_3a = 0

When the bucket falls with acceleration a,

m_3g - F_{dn3} = m_3a
m_3(g - a) = F_{dn3}

Since m_3 = \rho h_3 A, the pressure (divide force by A) is: P = \rho h_3(g - a)

Do a similar analysis of the pressure on the bottom layer and you will see that the pressure difference is
\triangle P = \rho \triangle h (g-a)

AM
 
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