The Magic of Squeezing
Understanding Bulk Modulus
Imagine holding a sponge ball in your hand and squeezing it from all directions. What happens? The ball shrinks uniformly, its volume decreases, and you feel a resistive force pushing back against your fingers. This simple, everyday experience is the gateway to one of the most fundamental concepts in the physics of materials: Bulk Modulus.
In this problem, we are asked to find the Bulk Modulus of a medium whose pressure is increased from 1.01×105 Pa to 1.165×105 Pa, causing its volume to contract by 10%. Let us embark on a journey to understand how materials respond to being squeezed from all sides, and how we can mathematically quantify this resistance.
The Physics of Volumetric Stress and Strain
When we apply a force uniformly over the entire surface of an object, we are applying pressure. This uniform pressure is called volumetric stress or bulk stress. Unlike tensile stress, which pulls an object along a single axis, or shear stress, which slides layers of an object past each other, volumetric stress acts in three dimensions simultaneously.
How does the material respond? It undergoes volumetric strain, which is defined as the fractional change in volume:
Here, ΔV is the change in volume, and V is the original volume. Because a positive increase in pressure always leads to a decrease in volume, the change in volume ΔV is negative. To keep our physical constant positive, we define the Bulk Modulus (B) with a negative sign:
This elegant formula tells us that Bulk Modulus is simply the ratio of the change in pressure to the fractional change in volume. It is a direct measure of how incompressible a substance is. A massive Bulk Modulus, like that of steel or diamond, means it takes an enormous amount of pressure to cause even a tiny change in volume. A small Bulk Modulus, like that of air or water, means the substance is much easier to compress.
Step-by-Step Execution
Breaking Down the Math
Let us look at the numbers given to us. The initial pressure of our medium is:
And the final pressure is:
To find the volumetric stress, we calculate the change in pressure, ΔP:
ΔP=P2−P1=1.165×105−1.01×105
ΔP=(1.165−1.01)×105=0.155×105 Pa
This is the extra pressure squeezing our medium.
Now, let us address the volumetric strain. The problem states that the volume changes by 10%. This means the fractional change in volume is:
Substituting these values into our Bulk Modulus formula, we get:
Notice how the two negative signs cancel out beautifully, leaving us with a positive value for the Bulk Modulus:
B=0.100.155×105=1.55×105 Pa
And there we have it! The Bulk Modulus of the medium is 1.55×105 Pa, which corresponds perfectly to Option (d).
Deep Physical Insights
Compressibility and Beyond
Why is Bulk Modulus so important? It is the key to understanding sound waves traveling through fluids, the behavior of deep-sea submersibles, and even the stability of stars!
There is another closely related concept called Compressibility (K), which is simply the reciprocal of the Bulk Modulus:
While Bulk Modulus measures a material's resistance to compression, compressibility measures how easy it is to compress. Gases have extremely high compressibility (and low bulk modulus), while solids and liquids have very low compressibility (and high bulk modulus).
In our problem, the temperature was kept constant, which means we calculated the isothermal bulk modulus. If the compression had happened so quickly that no heat could escape, we would have calculated the adiabatic bulk modulus, which is always larger because the rising temperature of the compressed material adds an extra thermal pressure resisting the squeeze. Physics is full of these beautiful, interconnected layers!