FLD-16
Bulk modulus
K = − Δp / (ΔV/V). How hard a fluid is to compress.
Governing equation
where
- \Delta p
- Pressure rise (MPa)
- \Delta V/V
- Volumetric strain (—)
- K
- Bulk modulus (GPa)
The figure, part by part
Each numbered marker wears the color of its card. Hover a card to light the marker. Tap a marker to jump to that card. The slider walks a red point along the curve; Animate drawing traces it like a pen.
Governing law — red
Domain of the variable — blue
Response curve — green
Rate of change — amber
Lecture brief
Historical brief
Bernoulli, Navier–Stokes, Reynolds (1883) and Stokes drag made continuum flow a dimensionless craft. The sheets compute head, drag, Re and a pedagogical NS snapshot. This sheet (FLD-16 — Bulk modulus) is the form associated with Bulk modulus. Working symbols: , . Water is near 2.2 GPa. The definition is the isothermal or adiabatic derivative −v(∂p/∂v).
Purpose
Live realistic example
In symbols
Calculator
Inputs
Outputs
- Bulk modulus K2.22 GPa
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Free library
Full libraryFree PDF / open book
- University Physics Vol. 1 (mechanics, waves)OpenStax · CC BY · Free PDF / open book
- College Physics 2eOpenStax · CC BY · Free PDF / open book
- LibreTexts PhysicsLibreTexts · CC · Free PDF / open book
- SI Brochure (BIPM)BIPM · Free PDF / open book
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Narration of this film
A piston, a tiny volume shrink, a large Δp.
Water is near 2.2 GPa. The definition is the isothermal or adiabatic derivative −v(∂p/∂v).
Watch on YouTube