I want to understand this equation - Fluid Mechanics

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Understanding the coefficient of compressibility or bulk modulus of elasticity (κ) in fluid mechanics requires familiarity with partial derivatives and finite difference approximations. Equation (2-12) represents κ in terms of volume and pressure changes, while equation (2-13) provides a finite change approximation. To grasp these concepts, one should review the definitions and calculations of derivatives, particularly in the context of fluid properties. Additionally, exploring how finite differences relate to derivatives will aid in understanding the transition from equation (2-12) to equation (2-13). A solid foundation in calculus and fluid mechanics principles is essential for a comprehensive understanding.
Alexanddros81
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Hi all!
I have started reading Fluid Mechanics at my own pace (no university study)
and really I would like to grasp the ideas behind it.

So I have Fluid Mechanics by Cengel - 4th edition.
At page 45 the coefficient of compressibility or bulk modulus of elasticity (κ) is introduced.

##κ = V(\frac {\partial P} {\partial V})_T = ρ(\frac {\partial P} {\partial ρ})_T## (Pa) (2-12)

It can also be expressed approximately in terms of finite changes as

##κ = - \frac {ΔP} {ΔV/V} = \frac {ΔP} {Δρ/ρ}## (T = constant) (2-13)

I want to understand equation (2-12) and how it gets equation (2-13).
Obviously I would need to revise partial derivatives.
What else would I need to Know in order to understand these equations?
Your insight would be appreciated.
 
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Eqns. 13 is the finite difference approximation to Eqn. 2-12. Do you know how to approximate derivatives of a function using finite differences?
 
Chestermiller said:
Eqns. 13 is the finite difference approximation to Eqn. 2-12. Do you know how to approximate derivatives of a function using finite differences?

I don't know. What should I be looking at?
 
Alexanddros81 said:
I don't know. What should I be looking at?
What is the definition of the derivative of f(x) with respect to x?
 
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