2.2.5Fluid Mechanics

Hydrostatics — pressure = ρgh, derivation

1,790 words8 min readdifficulty · medium

WHAT are we talking about?

WHY does it matter? Dams, submarines, blood pressure, barometers, buoyancy — every one of them lives or dies by how pressure changes with depth.


HOW: derive P=ρghP = \rho g h from scratch

We use only Newton's first law: a fluid at rest has zero net force on every piece of it.

Figure — Hydrostatics — pressure = ρgh, derivation

Step 1 — Choose the body. A vertical cylinder of fluid: area AA, height hh, top at the free surface (open to atmosphere), bottom at depth hh.

Why this step? A column makes the geometry simple — only top and bottom faces matter for vertical balance; the sides push horizontally and cancel.

Step 2 — Find the mass of the column. V=Ah,m=ρV=ρAhV = A h, \qquad m = \rho V = \rho A h

Why this step? Pressure is about weight, and weight needs mass; mass comes from density × volume.

Step 3 — Forces on the column (vertical only).

  • Weight pulling down: W=mg=ρAhgW = mg = \rho A h\, g
  • Atmosphere pushing down on the top: Ftop=P0AF_{\text{top}} = P_0 A
  • Fluid below pushing up on the bottom: Fbot=PAF_{\text{bot}} = P A (this is what we want)

Why this step? Each face feels pressure ×\times area. Sideways forces on the curved wall are horizontal and cancel by symmetry, so we ignore them.

Step 4 — Apply equilibrium (net force =0=0). Fbot=Ftop+WF_{\text{bot}} = F_{\text{top}} + W PA=P0A+ρAhgP A = P_0 A + \rho A h g

Why this step? The column is at rest \Rightarrow up-push balances (down-push + weight).

Step 5 — Divide by AA. P=P0+ρgh\boxed{P = P_0 + \rho g h}

The gauge (extra) pressure due to the fluid alone is: Pgauge=PP0=ρgh\boxed{P_{\text{gauge}} = P - P_0 = \rho g h}


Worked examples


Common mistakes (Steel-man + fix)


Recall Feynman: explain to a 12-year-old

Imagine a tall stack of pillows. If you lie at the bottom of the stack, lots of pillows squash you. Near the top, only a few do. Water is the same: the deeper you dive, the more water sits above you and squeezes you. Twice as deep \Rightarrow roughly twice the squeeze. And it doesn't matter if the pool is huge or tiny — only how deep you go counts, because only the water right above your head is pressing on you.


Flashcards

Hydrostatic pressure formula (gauge)
P=ρghP = \rho g h
What does each symbol mean in ρgh\rho g h?
ρ\rho = fluid density, gg = gravity, hh = vertical depth below surface
Absolute vs gauge pressure relation
Pabs=P0+ρghP_{abs} = P_0 + \rho g h; gauge =ρgh= \rho g h
Does pressure depend on container shape/area?
No — only on vertical depth hh (hydrostatic paradox)
Starting principle used to derive P=ρghP=\rho g h
Fluid at rest \Rightarrow net force on any column is zero (force balance)
Why do side forces drop out of the derivation?
They are horizontal and cancel by symmetry; only top/bottom faces give vertical force
Roughly how much depth of water adds 1 atmosphere?
About 10 m
SI unit of pressure
pascal, Pa=N/m2\text{Pa} = \text{N/m}^2
Height of mercury barometer at 1 atm
0.76m\approx 0.76\,\text{m} (760 mm Hg)
Convert 1g/cm31\,\text{g/cm}^3 to SI
1000kg/m31000\,\text{kg/m}^3
Why does pressure increase with depth (one line)?
More fluid weight sits above, spread over the same area

Connections

  • Pascal's Law — pressure applied to enclosed fluid transmits equally
  • Atmospheric Pressure & Barometer — measuring P0P_0 via ρgh\rho g h
  • Buoyancy & Archimedes' Principle — net upward force comes from pressure difference with depth
  • Manometers — read pressure differences as height differences
  • Bernoulli's Equation — adds motion; reduces to ρgh\rho g h when fluid is static
  • Density and Specific Gravity — supplies ρ\rho

Concept Map

deeper means more fluid above

Newton first law

weight W = rho A h g

cancel by symmetry

divide by A

subtract P0

depends only on depth

confirms

applies to

Fluid has weight

Pressure grows with depth

Imaginary fluid column area A depth h

Vertical force balance

Mass m = rho A h

Atmosphere pushes down P0 A

Fluid pushes up P A

Side forces horizontal

P = P0 + rho g h

Gauge pressure = rho g h

Hydrostatic paradox shape irrelevant

Dams submarines barometers buoyancy

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Dekho yaar, hydrostatics ka core idea bilkul simple hai: fluid jab rest pe hota hai, tab bhi uska weight hota hai. Jitna neeche jaoge, utna zyada paani tumhare upar baitha hota hai, aur wo dabaata hai. Isi liye depth badhne se pressure badhta hai. Formula P=ρghP = \rho g h ka matlab seedha hai — upar wale column ka weight, area pe spread kar do, bas wahi pressure hai.

Derivation samajhne ke liye ek imaginary column lo — area AA, height hh, top surface pe. Ye column rest pe hai, to upar ki taraf wala force neeche wale forces ko balance karega. Neeche se fluid push karta hai PAPA (upar), upar atmosphere push karta hai P0AP_0 A (neeche), aur weight ρAhg\rho A h g neeche. Balance karo: PA=P0A+ρAhgPA = P_0 A + \rho A h g. AA se divide karo, mil gaya P=P0+ρghP = P_0 + \rho g h. Side ke forces horizontal hote hain, cancel ho jaate hain — isliye unki tension mat lo.

Ek important baat: pressure sirf depth pe depend karta hai, container ke size ya shape pe nahi. Isko hydrostatic paradox kehte hain — chhoti patli tube aur badi tank, dono ka same depth pe bottom pressure same. Reason: jo extra paani hai badi tank mein, uska weight walls aur base sambhalte hain, ek point ke upar nahi aata.

Exam tip: agar "gauge" pressure pucha hai to sirf ρgh\rho g h likho; "absolute" pucha hai to P0P_0 add karo. Aur hh hamesha vertical depth hota hai, surface se seedha neeche — slant distance nahi. Density ko SI mein convert karna mat bhoolna (1g/cm3=1000kg/m31\,\text{g/cm}^3 = 1000\,\text{kg/m}^3). Bas itna pakka kar lo, ye topic full marks ka hai.

Go deeper — visual, from zero

Test yourself — Fluid Mechanics

Connections