Setup: Take a tiny wedge-shaped fluid element (a triangular prism) of thickness, inside a static fluid. Let the three faces have pressures px (on the vertical face), py (on the horizontal face), pn (on the slanted face). The element is so small we can ignore gravity (volume →0 faster than area).
Let the slanted face make angle θ, with areas:
vertical face area =dAx
horizontal face area =dAy
slant face area =dAn
Geometry of the wedge gives:
dAx=dAnsinθ,dAy=dAncosθ
Horizontal balance (x): pressure force on vertical face = horizontal component of force on slant face
pxdAx=pndAnsinθ
Why this step? Pressure pushes perpendicular into a surface; only the horizontal component of the slant-face force opposes the vertical-face force.
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=pn.
Hydraulic press force relation
F2=F1A2/A1 (since p1=p2).
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/A1 is large.
Does the hydraulic press give free energy?
No — F1d1=F2d2; you trade distance for force.
If you raise surface pressure by Δp, how much does pressure rise at depth h?
By exactly Δp (the ρgh 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.
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."
Pascal's law ka core idea bahut simple hai: agar fluid band (enclosed) aur incompressible ho, aur tum kahin bhi pressure badhao (Δp), 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=pn — 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/A2. Matlab chhote piston (chhota area) par thoda force lagao, bade piston par area A2/A1 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=A2d2. Isliye work same rehta hai: F1d1=F2d2. 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=pA laga do. Aur ρgh wala term tabhi add karo jab dono pistons alag height pe hon — warna ignore.