The Magic of Floating
Imagine you are standing next to a calm lake, watching a wooden block float peacefully on the water.
It seems so simple, yet beneath the surface, a beautiful tug-of-war of physics is taking place.
On one hand, gravity is relentlessly pulling the block downward with a force equal to its weight, W=Mg.
On the other hand, the water is pushing back upward with a force we call buoyancy or upthrust, FB.
Under normal conditions, these two forces are in perfect harmony, keeping the block in a state of stable equilibrium.
But what happens if we suddenly cut the thread of gravity?
What if we take this entire setup—the beaker, the water, and the floating block—and drop it from a high tower, letting it fall freely?
Does the block sink? Does it shoot out of the water? Or does something even more fascinating happen?
Let's dive deep into the physics of free fall and fluid dynamics to find out.
The Physics of Upthrust
To understand what happens in free fall, we must first understand where upthrust actually comes from.
It is a common misconception that fluids simply "dislike" submerged objects and push them up.
In reality, upthrust is the result of a pressure difference.
Because of gravity, the pressure in a static fluid increases with depth.
This variation is mathematically described by the hydrostatic pressure gradient equation:
Here, ρL is the density of the liquid, h is the depth, and g is the acceleration due to gravity.
Because of this gradient, the pressure at the bottom of a submerged object is always greater than the pressure at its top.
This pressure difference creates a net upward force, which we call the buoyant force:
where Vi is the volume of the submerged portion of the body.
Notice how both equations are directly proportional to g.
This is our crucial clue!
Plunging into Free Fall
Now, let's release the entire system into a state of free fall.
As the beaker, liquid, and body plunge downwards, they accelerate at exactly the rate of gravity, a=g.
If we step inside the accelerating frame of reference of the beaker, we must use the concept of effective gravity (geff):
Since the system is falling freely, the downward acceleration of our frame is exactly equal to g.
Substituting a=g into our equation, we get:
In this freely falling frame, the effective gravity is exactly zero!
The entire system enters a state of complete weightlessness.
The Disappearing Pressure Gradient
Now, let's see what happens to our pressure gradient when geff=0.
Substituting this value back into our hydrostatic equation:
This is a profound realization!
Since the pressure gradient is zero, the pressure does not change with depth anymore.
The pressure is completely uniform and equal to the atmospheric pressure P0 at every single point in the liquid.
Without a pressure difference between the top and bottom of our submerged body, there is no longer any net upward force from the liquid.
We can also see this directly from Archimedes' formula by substituting geff=0:
Thus, the upthrust acting on the body during free fall is exactly zero.
This perfectly matches Option (a).
What Happens to the Floating Body?
Let's take a moment to appreciate the physical reality of this state.
Since the upthrust is zero, you might initially think the body should sink.
But remember, in this weightless environment, the effective gravity pulling the body down is also zero!
Both the downward gravitational pull and the upward buoyant force have completely vanished.
The net force acting on the body is exactly zero.
As a result, the body will simply remain in its original position relative to the liquid, suspended in a state of perfect weightlessness.
It won't sink, and it won't rise; it will just float effortlessly, as if suspended in deep space.