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7 Questions around this concept.
When a liquid is subjected to horizontal acceleration:
A closed rectangular tank is completely filled with water and is accelerated horizontally with an acceleration towards right. Pressure is-
(i) maximum at, and (ii) minimum at-
An object of uniform density is allowed to float in water kept in a beaker. The object has triangular cross-section as shown in the figure. If the water pressure measured at three point A, B and C below the object are PA, PB and PC respectively. Then-
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A cylindrical tank contains water upto a height H. If the tank is accelerated with acceleration a, then pressure at the point A is P1. If the tank is accelerated downwards with acceleration a the pressure at A is P2 then-
Case I- When Acceleration in the vertical direction
When the liquid container is moving with constant acceleration in an upward direction
Consider a cylindrical element of height h and Area A as shown in the below figure.
The force on the top face of the element =
The force on the bottom face of the element =
If a is the acceleration of the liquid then
We can write
Where m is the mass of the element of the liquid and which is given by
Where =density of liquid
So using this we get
When the liquid container is moving with constant acceleration in a downward direction
I. constant downward acceleration (a< g)
So for the below figure is given by
And Pressure at point A is given as
II. constant downward acceleration (a=g)
The pressure became zero everywhere when a=g
III. constant downward acceleration (a> g)
In this case, the fluid occupies the upper part of the container as shown in the figure.
Case II- When Acceleration in Horizontal direction
If a liquid in the tank is moving on a horizontal surface with some constant acceleration a
Then the free surface of the liquid takes the shape as shown by the dotted line in the figure.
Now consider a cylindrical element of length l and cross-section area A
So the force on the left face of the cylinder is
While force on the right face of the cylinder is
And we can also write
And the mass of the element of the liquid and which is given by
Where =density of liquid
So using Newton's second law for the element
So we can say that
The free surface of the liquid makes an angle with horizontal
Or the free surface of the liquid orient itself perpendicular to the direction of net effective gravity.
So for the below figure, we can say that
Pressure will vary in the horizontal direction.
And the Pressure gradient in the x-direction is given as
Where -ve sign indicates pressure increases in a direction opposite to the direction of acceleration.
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