Mechanical Properties of Fluids

Physics · Class 11

Lesson 12 of 12 · 19 min

Chapter review

Watch a class

The whole chapter on YouTube

Complete chapter walkthrough with NCERT coverage

Prashant Kirad 11th & 12th · Hinglish · Whole chapter · Open on YouTube

Whole-chapter one-shot revision

Next Toppers - 11th Science · Hinglish · Whole chapter · Open on YouTube

Loading the full lesson

Must-know facts

22 facts

  1. 1Pressure P = F/A (normal force); scalar; unit Pa = N m⁻²; dimensions [ML⁻¹T⁻²].
  2. 21 atm = 1.013 × 10⁵ Pa (1.01 × 10⁵ in the summary); 1 bar = 10⁵ Pa; 1 torr = 1 mm of Hg = 133 Pa.
  3. 3Density of water at 4 °C = 1.0 × 10³ kg m⁻³; relative density is a pure number.
  4. 4Pascal's law: equal pressure at equal heights in a fluid at rest; applied pressure is transmitted undiminished to every point.
  5. 5P = P_a + ρgh; gauge pressure P − P_a = ρgh; container shape does not matter (hydrostatic paradox).
  6. 6Barometer: P_a = ρgh, about 76 cm of mercury at sea level.
  7. 7Hydraulic lift: F₂ = F₁A₂/A₁, mechanical advantage A₂/A₁; distances A₁L₁ = A₂L₂.
  8. 8Syringes 1.0 cm and 3.0 cm diameter: 10 N becomes 90 N; 6.0 cm in gives 0.67 cm out.
  9. 9Streamlines never cross in steady flow; above a critical speed flow turns turbulent.
  10. 10Continuity: Av = constant for an incompressible fluid (conservation of mass).
  11. 11Bernoulli: P + ½ρv² + ρgh = constant along a streamline (energy conservation, ideal fluid, steady flow).
  12. 12Torricelli: v = √(2gh) from an open tank, the free-fall speed.
  13. 13Magnus effect: a spinning ball gets lift because air moves faster on one side than the other.
  14. 14Aircraft example: ΔP = 6.5 × 10³ N m⁻², upper-surface air only about 8% faster.
  15. 15η = (F/A)/(v/l); unit Pa s = N s m⁻² = poiseuille; dimensions [ML⁻¹T⁻¹].
  16. 16Liquid viscosity falls with temperature; gas viscosity rises.
  17. 17Stokes: F = 6πηav; terminal velocity v_t = 2a²(ρ − σ)g/(9η) ∝ a².
  18. 18Surface tension S = F/l per surface = surface energy per unit area; unit N m⁻¹ = J m⁻²; water 0.0727 N m⁻¹ at 20 °C.
  19. 19Surface tension usually falls with temperature.
  20. 20Angle of contact: acute for water-glass (wets), obtuse for mercury-glass (does not wet); S_la cos θ + S_sl = S_sa.
  21. 21Excess pressure: drop or air bubble in a liquid 2S/r; soap bubble in air 4S/r.
  22. 22Capillary rise h = 2S cos θ/(ρga); 2.98 cm for water in a 0.05 cm-radius tube; mercury is depressed.

Common traps

Where marks are lost

Treating pressure as a vector because force is a vector.

Only the normal component of force enters P = F/A; pressure has no direction and acts equally every way at a point.

Using absolute pressure where gauge pressure is asked, or the other way round.

Gauge = absolute − atmospheric = ρgh. A submarine window with 1 atm inside feels only the gauge pressure.

Thinking a wider container gives a larger pressure at the bottom.

P = P_a + ρgh depends only on depth, not on area or shape: the hydrostatic paradox.

Using the diameter ratio instead of its square in a hydraulic lift.

Force scales with area, so with (d₂/d₁)²: diameters 1 : 3 give forces 1 : 9.

Believing a hydraulic lift gives work for free.

The large piston moves A₁/A₂ as far, so F₁L₁ = F₂L₂ for an ideal lift.

Expecting higher pressure where a pipe narrows.

Speed rises in the narrow part (Av = constant), so by Bernoulli the pressure there is lower.

Applying Bernoulli's equation to turbulent or viscous flow.

It holds only for steady, incompressible, non-viscous flow along a streamline.

Saying the viscosity of air falls when it is heated.

Liquids get less viscous when hot; gases get more viscous.

Using 2S/r for a soap bubble in air.

A soap film has two surfaces: 4S/r. A drop, or an air bubble inside a liquid, has one: 2S/r.

Using the tube's diameter for a in h = 2S cos θ/(ρga).

a is the radius of the capillary.

Formulas

16 to know

Pressure

P = F/A; P = lim ΔF/ΔA as ΔA → 0

Normal force only; scalar.

Density

ρ = m/V

Relative density = ρ/ρ_water(4 °C).

Pressure with depth

P₂ − P₁ = ρgh; P = P_a + ρgh

Gauge pressure = ρgh.

Barometer

P_a = ρ_Hg g h

h ≈ 76 cm at sea level.

Hydraulic lift

F₂ = F₁A₂/A₁; A₁L₁ = A₂L₂

Mechanical advantage A₂/A₁.

Continuity

A₁v₁ = A₂v₂ (Av = constant)

Incompressible steady flow; Av is the volume flow rate.

Bernoulli's equation

P + ½ρv² + ρgh = constant

Along a streamline; ideal fluid.

Speed of efflux

v = √[2gh + 2(P − P_a)/ρ]; open tank v = √(2gh)

Torricelli's law.

Lift on a wing

ΔP × A = weight; ΔP = ½ρ(v₂² − v₁²)

(v₂ − v₁)/v_av = ΔP/(ρv_av²).

Coefficient of viscosity

η = (F/A)/(v/l) = Fl/(vA)

Pa s; [ML⁻¹T⁻¹].

Stokes' law

F = 6πηav

Sphere of radius a at speed v.

Terminal velocity

v_t = 2a²(ρ − σ)g/(9η)

ρ sphere, σ fluid.

Surface tension

S = F/2l (film with two surfaces); S_la = W/2l

N m⁻¹ = J m⁻².

Angle of contact

S_la cos θ + S_sl = S_sa

θ acute: wets; θ obtuse: does not wet.

Excess pressure

drop or cavity: 2S/r; soap bubble: 4S/r

Concave side at higher pressure.

Capillary rise

h = 2S cos θ/(ρga)

a = tube radius; negative h (depression) when θ > 90°.

Key terms

16 terms

Fluid
A substance that can flow: a liquid or a gas.
Pressure
Normal force per unit area; a scalar measured in pascals.
Relative density
Density of a substance divided by the density of water at 4 °C.
Gauge pressure
Pressure above atmospheric pressure, P − P_a.
Hydrostatic paradox
Differently shaped connected vessels fill to the same level because only depth sets the pressure.
Torr
Pressure of 1 mm of mercury, 133 Pa.
Steady flow
Flow in which the velocity at each fixed point does not change with time.
Streamline
The path of a fluid particle in steady flow; its tangent gives the local velocity.
Turbulent flow
Unsteady, irregular flow that sets in above the critical speed.
Equation of continuity
Av = constant: conservation of mass for an incompressible fluid.
Magnus effect
Sideways or upward force on a spinning ball moving through a fluid.
Viscosity
Internal friction between layers of a fluid in relative motion.
Terminal velocity
Constant speed of a body falling through a fluid when drag and buoyancy balance its weight.
Surface tension
Force per unit length, or energy per unit area, of a liquid's interface.
Angle of contact
Angle inside the liquid between the liquid surface and the solid at their line of contact.
Capillary rise
The climb of a wetting liquid in a narrow tube, driven by surface tension.
Test yourself: 10 questionsExam-style questions on Mechanical Properties of Fluids, with full solutions.Start
Chapter review | Mechanical Properties of Fluids | Lumi Learn