- #1
Alexanddros81
- 177
- 4
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.
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.