Height Of Mercury In A Mercury Barometer In An Accelerating Frame I am currently in high school and I came across a physics problem that asked to find whether the height of the mercury in a mercury barometer would change when it is kept in an elevator that accelerating upwards with a magnitude of 'a'.
Here is how I approached the problem(demonstrated in the image file attached):
1)In the frame of the elevator, the acceleration due to gravity would be (g+a) downwards
2)I assumed the Mass of the air column above the liquid mercury exposed to the atmosphere to be 'M'
3)I assumed the area of the mercury in the container exposed to the atmosphere to be 'A'.
4)I assumed that a vacuum exists in the space between the tube and the mercury.


*I assumed the density of mercury to be 'rho'

After you read my attempt at solving the problem, you see that at the end I get an equation for 'h' is not a function of either g or a. So that must imply that the height of the mercury inside the elevator accelerating upwards must be the same as in the case where the elevator was not accelerating.
But after checking various solutions on the internet, which propose that the height of the mercury changes, I am confused and not able to determine what I assumed wrong or where I made a mistake.
I would appreciate if someone could clarify my conceptual doubt.
(P.S I do not know how to write mathematical equations in PhysicsStackExchange so please excuse any distastefulness in my handwriting or illustration skills)


 A: Your expression for $P_B$ is correct, but your expression for $P_A$ is incorrect. When you write
$\displaystyle P_A=\frac{M(g+a)}{A}$
you are implicitly assuming that the whole mass $M$ of the atmosphere above the open area of mercury (all the way to the top of the atmosphere) is being accelerated. This is not true. Only the small amount of air in the lift is being accelerated, and its mass is negligible compared to the much larger mass $M$. You should have
$\displaystyle P_A=\frac{Mg}{A}$
On the other hand, all of the mercury is being accelerated, so we do have to include the acceleration when calculating the pressure of the column of mercury, as you have done in your expression for $P_B$:
$\displaystyle P_B = \rho (g+a)h$
Equating $P_A$ and $P_B$ now gives
$ \displaystyle \Rightarrow \frac {Mg}{A} = \rho(g+a)h
\\ \displaystyle \Rightarrow h = \frac{Mg}{A\rho (g+a)}$
We can also write $\frac{Mg}{A}$ as atmospheric pressure$P_{atm}$, so we have
$\displaystyle h=\frac{P_{atm}}{\rho (g+a)}$
As you can see, the height $h$ of the mercury column now depends on the acceleration $a$, and it decreases as $a$ increases.
A: This is response to a comment from @Archit Chhajed requesting my answer.
Any object of mass $m$ in the elevator experiences an inertial (fictitious) force $-ma$ downward where $a$ is the acceleration of the elevator upward.  The total force on each object is $-m(g + a)$ downward where $g$ is the acceleration of gravity.  The weight of each object is increased from $mg$ to $m(g + a)$.  There are three objects in the elevator to be considered: the air in the elevator (not the total atmosphere), the mercury exposed to the air in the elevator, and the mercury in the tube.  The increase in the pressure from the air in the elevator on the mecury exposed to the air is very small due to the small mass of air; use the ideal gas law to calculate the small mass: $PV = nRT$ where $P$ is pressure, $V$ volume of the elevator, $n$ moles of air (convert this to mass of air), $R$ the universal gas constant, and $T$ temperature.  So the increase in the pressure from the air in the elevator is very small.  Both the mercury exposed to the air and the mercury in the tube increase in weight. (It is as if with the elevator at rest the mercury is replaced by a denser liquid, except for the accelerating elevator the density is not increased, but the effective acceleration of gravity is increased from $g$ to $g + a$).  As others (e.g. @gandalf16) have explained, the increase in weight of the mercury in the tube decreases the height of the mercury in the tube, neglecting the small change in air pressure.  That is, the air pressure pushes a heavier liquid less-far up the tube.  The level of the mercury outside the tube increases as the level of mercury inside the tube decreases. (I have neglected the small vapor pressure of mercury in the open space at the top of the tube; that is, I have assumed a vacuum in the open space at the top of the closed-ended tube.)
Hope this helps.
