2.2.6Fluid Mechanics

Pascal's law — pressure transmits equally

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WHAT is Pascal's Law?

Two ideas hide inside this one sentence:

  1. Same pressure everywhere on a level — in static fluid at one height, pressure is equal in all directions and at all points on that level.
  2. Changes transmit fully — if you raise the pressure at one point by Δp\Delta p, every point rises by the same Δp\Delta p.

WHY is it true? (Derivation from first principles)

Setup: Take a tiny wedge-shaped fluid element (a triangular prism) of thickness, inside a static fluid. Let the three faces have pressures pxp_x (on the vertical face), pyp_y (on the horizontal face), pnp_n (on the slanted face). The element is so small we can ignore gravity (volume 0\to 0 faster than area).

Let the slanted face make angle θ\theta, with areas:

  • vertical face area =dAx= dA_x
  • horizontal face area =dAy= dA_y
  • slant face area =dAn= dA_n

Geometry of the wedge gives: dAx=dAnsinθ,dAy=dAncosθdA_x = dA_n \sin\theta, \qquad dA_y = dA_n \cos\theta

Horizontal balance (x): pressure force on vertical face = horizontal component of force on slant face pxdAx=pndAnsinθp_x\,dA_x = p_n\,dA_n \sin\theta

Why this step? Pressure pushes perpendicular into a surface; only the horizontal component of the slant-face force opposes the vertical-face force.

Substitute dAx=dAnsinθdA_x = dA_n\sin\theta: pxdAnsinθ=pndAnsinθ    px=pnp_x\,dA_n\sin\theta = p_n\,dA_n\sin\theta \;\Rightarrow\; \boxed{p_x = p_n}

Vertical balance (y): similarly pydAy=pndAncosθ    py=pnp_y\,dA_y = p_n\,dA_n\cos\theta \;\Rightarrow\; p_y = p_n

Therefore: px=py=pn\boxed{p_x = p_y = p_n}

Now the transmission part. Recall the hydrostatic relation (from a fluid column of height hh): p=p0+ρghp = p_0 + \rho g h

If we increase the external/applied pressure p0p0+Δpp_0 \to p_0 + \Delta p, then at every depth hh: pnew=(p0+Δp)+ρgh=pold+Δpp_{\text{new}} = (p_0 + \Delta p) + \rho g h = p_{\text{old}} + \Delta p

The ρgh\rho g h term is unchanged (same fluid, same heights), so the increase Δp\Delta p is identical at every point. That is Pascal's law.


Figure — Pascal's law — pressure transmits equally

HOW to use it — worked examples


Common mistakes (steel-manned)


Flashcards

Pascal's law in one sentence
A pressure change applied to an enclosed incompressible fluid is transmitted undiminished to every part of the fluid and the container walls.
Why is pressure equal in all directions at a point in a static fluid?
Because a tiny wedge element in equilibrium has zero net force; the wedge geometry forces px=py=pnp_x=p_y=p_n.
Hydraulic press force relation
F2=F1A2/A1F_2 = F_1\,A_2/A_1 (since p1=p2p_1=p_2).
Why does a tiny force lift a big load in a hydraulic lift?
Same pressure acts over a larger area; force = pressure × area, and A2/A1A_2/A_1 is large.
Does the hydraulic press give free energy?
No — F1d1=F2d2F_1 d_1 = F_2 d_2; you trade distance for force.
If you raise surface pressure by Δp\Delta p, how much does pressure rise at depth hh?
By exactly Δp\Delta p (the ρgh\rho g h term is unchanged).
Two conditions for Pascal's law
Fluid must be enclosed (confined) and incompressible.
For pistons radii 1 cm and 10 cm, mechanical advantage?
(10/1)2=100(10/1)^2 = 100.

Recall Feynman: explain to a 12-year-old

Imagine a balloon completely full of water with no air. If you poke it with your finger on one side, the whole balloon bulges everywhere — not just where you pushed. Water can't get squashed, so your push has to go somewhere, and it pushes equally on every bit of the rubber. A car lift uses this trick: you press a skinny straw of water, and that same push spreads onto a fat platform. A small push on a small spot becomes a giant push on a big spot — but you have to push your skinny straw down a loooong way to lift the car just a little. Nothing is free; you just swap "how hard" for "how far."


Connections

  • Hydrostatic pressure — p = p0 + ρgh — supplies the ρgh\rho g h term we held constant.
  • Pressure — force per unit area — basic definition p=F/Ap=F/A used in the press.
  • Hydraulic systems — brakes, lifts, jacks — direct engineering application.
  • Archimedes' principle — buoyancy — also relies on isotropic fluid pressure.
  • Conservation of energy in machines — explains why the press isn't a free-energy device.
  • Incompressibility & continuity equation — why A1d1=A2d2A_1 d_1 = A_2 d_2.

Concept Map

net force zero

force balance

foundation for

add delta p to p0

proves transmission

applied to

two pistons

pressure acts

component balance

same pressure bigger area

Static equilibrium no flow

Tiny wedge element

Pressure isotropic px=py=pn

Pascal's Law

Hydrostatic p=p0+rho g h

Delta p same at every depth

Hydraulic machine

Small push lifts big load

Perpendicular into surface

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Pascal's law ka core idea bahut simple hai: agar fluid band (enclosed) aur incompressible ho, aur tum kahin bhi pressure badhao (Δp\Delta p), to woh badhaav fluid ke har point par aur deewaron par exactly same transmit ho jaata hai — kahin bhi kam nahi hota. Iska proof ek chhote se wedge (triangle) fluid element se aata hai: static fluid mein woh element rest pe hai, net force zero, isliye px=py=pnp_x=p_y=p_n — yaani ek point par pressure har direction mein barabar hota hai.

Sabse useful application hai hydraulic lift / press. Do piston connected by fluid: pressure dono jagah equal, to F1/A1=F2/A2F_1/A_1 = F_2/A_2. Matlab chhote piston (chhota area) par thoda force lagao, bade piston par area A2/A1A_2/A_1 guna zyada force milta hai. Isiliye garage mein car uthane ke liye sirf thodi si mehnat lagti hai.

Lekin yaad rakho — free energy nahi milti! Bada piston thoda hi upar uthta hai, chhota piston bahut neeche jaata hai, kyunki fluid incompressible hai: A1d1=A2d2A_1 d_1 = A_2 d_2. Isliye work same rehta hai: F1d1=F2d2F_1 d_1 = F_2 d_2. Tum sirf "force" aur "distance" ka trade kar rahe ho.

Exam tip: jab bhi enclosed fluid mein dabaav ka question aaye, pehle socho "pressure equal hai dono pistons par", phir F=pAF=pA laga do. Aur ρgh\rho g h wala term tabhi add karo jab dono pistons alag height pe hon — warna ignore.

Go deeper — visual, from zero

Test yourself — Fluid Mechanics

Connections