Topics
5📖 1. Chapter Overview
Overview
Mechanical Properties of Fluids studies liquids and gases at rest and in motion. Fluids cannot sustain shear stress at rest, so they flow and exert pressure normally on surfaces. The chapter begins with pressure in fluids, hydrostatic pressure and Pascal's law, which explains hydraulic lift and hydraulic press. Moving fluids are described using streamline flow, turbulent flow, continuity equation and Bernoulli's principle. Real fluids show viscosity, leading to drag, terminal velocity and Reynolds number. At the liquid surface, molecular forces produce surface tension, surface energy, capillary rise or fall and excess pressure in drops and soap bubbles. For NEET, this chapter is formula-rich, application-based and highly scoring.
- 1Pressure in a fluid at rest is the same in all directions at the same point.
- 2Fluid pressure depends on depth, density and gravity, not on container shape.
- 3In streamline flow through a narrow region, speed increases and pressure generally decreases.
- 4Bernoulli's principle is valid for ideal, incompressible, non-viscous and steady flow.
- 5Terminal velocity occurs when net force on a falling body in fluid becomes zero.
- 6Surface tension makes liquid surfaces behave like stretched membranes.
- 7NEET frequently asks hydraulic lift, continuity, Bernoulli applications, terminal velocity and capillarity formulas.
Continuity
A down means v up: smaller area gives larger speed.
Bernoulli
Fast fluid has low pressure at the same height.
Daily Life Example
Hydraulic brakes use Pascal's law, perfume atomizers use Bernoulli's principle, and capillary action helps water rise in plants.
NEET Quick Check
If a pipe area becomes one-third, fluid speed becomes three times for steady incompressible flow.
Using Bernoulli Everywhere
Bernoulli's equation in this form applies only to ideal, incompressible, non-viscous, steady flow along a streamline.
Confusing Viscosity and Surface Tension
Viscosity is internal resistance to flow, while surface tension acts at the free surface of a liquid.
Ignoring Atmospheric Pressure
Absolute pressure includes atmospheric pressure, while gauge pressure excludes it.
Pressure is the normal force acting per unit area.
Variables
P=Pressure
F=Normal force
A=Area
Pressure at depth h below the free surface of a liquid open to atmosphere.
Variables
P=Pressure at depth
P0=Pressure at free surface
ρ=Density of liquid
g=Acceleration due to gravity
h=Depth
For steady incompressible flow, volume flow rate remains constant.
Variables
A1, A2=Cross-sectional areas
v1, v2=Fluid speeds
💧 2. Pressure & Pascal's Law
Overview
Pressure is the normal force acting per unit area. In a fluid at rest, pressure at a point acts equally in all directions and always normal to any surface. Hydrostatic pressure increases with depth because lower layers support the weight of fluid above them. At depth h below an open surface, pressure is P = P0 + ρgh, where P0 is atmospheric pressure. Pascal's law states that pressure applied to an enclosed incompressible fluid is transmitted equally and undiminished throughout the fluid. This explains hydraulic lift and hydraulic press, where a small force on a small piston produces a large force on a larger piston. The machine multiplies force, not energy.
- 1Pressure is scalar although force is vector.
- 2Fluid pressure at rest depends on depth, fluid density and gravity.
- 3Pressure does not depend on container shape or base area alone.
- 4In hydraulic lift, the larger piston gives larger force because pressure is same but area is larger.
- 5The smaller piston moves a greater distance, so ideal work input equals work output.
- 6Pressure always acts normal to the surface of an object immersed in a fluid.
Hydrostatic Pressure
Deeper means more liquid above, so pressure increases.
Hydraulic Machines
Same pressure plus bigger area gives bigger force.
Solved Example: Pressure at Depth
At 4 m depth in water, gauge pressure = ρgh = 1000 × 10 × 4 = 4 × 10^4 Pa.
Solved Example: Hydraulic Lift
If A2 = 25A1 and F1 = 80 N, then F2 = F1(A2/A1) = 80 × 25 = 2000 N.
Thinking Hydraulic Lift Creates Energy
A hydraulic lift multiplies force, but the larger piston moves a smaller distance, so energy is conserved ideally.
Using Total Liquid Volume
Pressure at depth depends on height of liquid column, not total volume of liquid.
Confusing Gauge and Absolute Pressure
Gauge pressure is ρgh, while absolute pressure is P0 + ρgh.
Pressure is normal force per unit area.
Variables
P=Pressure
F=Normal force
A=Area
Absolute pressure at depth h in a liquid open to atmosphere.
Variables
P0=Atmospheric pressure or pressure at free surface
ρ=Density of liquid
g=Acceleration due to gravity
h=Depth below free surface
Excess pressure over atmospheric pressure at depth h.
Variables
Pg=Gauge pressure
ρgh=Pressure due to liquid column
🌊 3. Fluid Flow
Overview
Fluid flow describes the motion of liquids and gases. In streamline flow, each fluid particle follows a smooth path, and the velocity of fluid at a point remains constant with time. In turbulent flow, the motion is irregular, chaotic and contains eddies. The equation of continuity is based on conservation of mass. For steady incompressible flow, the volume of fluid crossing every cross-section per second is the same, so A1v1 = A2v2. Thus, fluid moves faster through narrow sections and slower through wider sections. The volume flow rate is Q = Av. Ideal fluid assumptions include incompressible, non-viscous, steady and irrotational flow, which are important before applying Bernoulli's principle.
- 1Continuity equation comes from conservation of mass.
- 2For incompressible fluid, density remains constant.
- 3If streamlines crossed, a fluid particle at one point would have two velocities, which is impossible.
- 4Flow rate has SI unit m³ s^-1.
- 5Turbulence is more likely at high speed, large pipe diameter or low viscosity.
- 6Continuity is often used together with Bernoulli equation in NEET.
Continuity Shortcut
Area × velocity is constant: small area means large velocity.
Streamlines
Streamlines do not cross because one point cannot have two flow directions.
Numerical Problem
Water flows through area 8 cm² at 3 m/s and then through area 2 cm². Using A1v1 = A2v2, v2 = 8×3/2 = 12 m/s.
Real-Life Example
When you partially close the mouth of a water hose, water comes out faster because the exit area decreases.
Using A1v1 = A2v2 for Compressible Gas Blindly
This simple form assumes incompressible flow with constant density.
Thinking Flow Rate Depends Only on Speed
Flow rate depends on both area and speed: Q = Av.
Confusing Turbulent Flow with Fast Streamline Flow
High speed may cause turbulence, but streamline flow can still be fast under suitable conditions.
Volume of fluid crossing a cross-section per unit time.
Variables
Q=Volume flow rate
A=Area of cross-section
v=Fluid speed
For incompressible steady flow, flow rate remains constant along the pipe.
Variables
A1, A2=Cross-sectional areas
v1, v2=Speeds of fluid at those sections
✈️ 4. Bernoulli's Principle
Overview
Bernoulli's principle is the conservation of mechanical energy for ideal fluid flow. For steady, incompressible, non-viscous flow along a streamline, the sum P + 1/2ρv² + ρgh remains constant. These terms represent pressure energy, kinetic energy and potential energy per unit volume. At the same height, when fluid speed increases, pressure decreases. This pressure-velocity relationship explains many applications: a venturimeter measures flow speed using pressure difference, airplane wings produce lift due to pressure difference, and atomizers and carburetors use fast air to reduce pressure and draw liquid into the air stream. NEET frequently asks direct formulas and conceptual applications.
- 1Bernoulli's equation is applied along a streamline.
- 2Pressure energy per unit volume is P.
- 3Kinetic energy per unit volume is 1/2ρv².
- 4Potential energy per unit volume is ρgh.
- 5Continuity equation is often needed before applying Bernoulli.
- 6Bernoulli does not account for viscous energy loss in real fluids.
- 7A pressure difference can create lift or suction-like effects.
Bernoulli Shortcut
Same height: speed up means pressure down.
Venturimeter
Narrow throat is the fast-low-pressure zone.
Numerical Example
Water speed changes from 2 m/s to 6 m/s at same height. Pressure drop = 1/2ρ(36 - 4) = 1/2×1000×32 = 16000 Pa.
Application Example
In a perfume atomizer, fast air over the tube lowers pressure and pulls liquid perfume upward into the air stream.
Applying Bernoulli Between Any Two Random Points
Use Bernoulli along the same streamline in ideal steady flow.
Ignoring Height Term
If two points are at different heights, include ρgh.
Assuming Bernoulli Explains All Lift Alone
For NEET, Bernoulli pressure difference is enough, but real aerodynamic lift also involves flow direction and Newton's laws.
Total mechanical energy per unit volume remains constant along a streamline for ideal flow.
Variables
P=Pressure
ρ=Fluid density
v=Fluid speed
h=Height
Simplified Bernoulli equation when height difference is negligible.
Variables
P1, P2=Pressures at two points
v1, v2=Speeds at two points
At the same height, pressure falls where speed rises.
Variables
P1 - P2=Pressure difference
v2² - v1²=Difference of squared speeds
🧪 5. Viscosity & Stokes' Law
Overview
Viscosity is the internal friction of a fluid that opposes relative motion between its layers. A more viscous fluid, such as honey, flows slowly compared with water. The coefficient of viscosity, η, measures the viscous nature of a fluid. When a small spherical body moves slowly through a viscous fluid, it experiences viscous drag given by Stokes' law: F = 6πηrv. As a sphere falls through a fluid, its speed increases until weight is balanced by buoyant force and viscous drag. Then acceleration becomes zero and it moves with terminal velocity. Reynolds number predicts whether fluid flow is streamline or turbulent. These ideas are important in raindrops, sedimentation, blood flow and oil flow.
- 1Viscosity arises due to relative motion between fluid layers.
- 2Liquids generally become less viscous when temperature increases.
- 3Gases generally become more viscous when temperature increases.
- 4Stokes' law is valid for small spherical bodies moving slowly in viscous fluid.
- 5Terminal velocity is proportional to r² for a small sphere.
- 6Higher viscosity lowers terminal velocity.
- 7Reynolds number is dimensionless.
Viscosity
Viscosity is fluid friction: honey has more, water has less.
Terminal Velocity
Terminal means final constant speed: weight is balanced by upward forces.
Stokes' Law
Remember 6πηrv: six-pi-eta-radius-velocity.
Numerical Example
If radius of a small sphere is doubled, terminal velocity becomes four times, assuming all other factors remain constant.
Application Example
Small raindrops fall slowly because viscous drag becomes comparable to their weight and they reach terminal velocity.
Applying Stokes' Law to Any Shape
Stokes' law in this form is for small spherical bodies moving slowly through viscous fluid.
Thinking Terminal Velocity Means No Forces
Forces still act, but net force is zero.
Forgetting Radius Squared in Terminal Velocity
Terminal velocity of a sphere is proportional to r², not r.
Viscous force between fluid layers is proportional to area and velocity gradient.
Variables
F=Viscous force
η=Coefficient of viscosity
A=Area of fluid layer
dv/dx=Velocity gradient perpendicular to flow
Viscous drag on a small sphere moving slowly through a viscous fluid.
Variables
F=Viscous drag force
η=Coefficient of viscosity
r=Radius of sphere
v=Speed of sphere
💦 6. Surface Tension & Capillarity
Overview
Surface tension is the property of a liquid surface by which it behaves like a stretched elastic membrane. It arises because molecules at the surface experience unbalanced cohesive forces. Surface tension is defined as force per unit length or surface energy per unit area. It explains spherical drops, floating needles, soap bubbles and insects walking on water. The angle of contact decides whether a liquid wets a solid surface. In a narrow capillary tube, liquid may rise or fall depending on adhesive and cohesive forces. Water rises in glass because angle of contact is acute, while mercury falls because its angle is obtuse. Curved liquid surfaces create excess pressure inside drops and bubbles, which is very important for NEET.
- 1Surface tension decreases with increase in temperature.
- 2Soap solution has lower surface tension than pure water.
- 3A liquid drop tends to be spherical to minimize surface area.
- 4Surface energy increases when surface area increases.
- 5Capillary action depends on surface tension, angle of contact, density and tube radius.
- 6A soap bubble has two surfaces, so its excess pressure is twice that of a liquid drop of same radius.
- 7For capillary fall, cosθ is negative because angle of contact is greater than 90 degrees.
Drop vs Bubble
Drop has one surface: 2S/R. Soap bubble has two surfaces: 4S/R.
Capillary Formula
Rise is high when tube is thin: h is inversely proportional to r.
Wetting
Water wets glass and rises; mercury avoids glass and falls.
Solved Example: Capillary Rise
If capillary radius is reduced to half, h = 2S cosθ/(ρgr) becomes double.
Solved Example: Bubble Pressure
For a soap bubble of radius R and surface tension S, excess pressure inside is 4S/R because it has two surfaces.
Everyday Application
Detergents reduce surface tension of water, helping it spread and enter small spaces in cloth for better cleaning.
Using Soap Bubble Formula for Liquid Drop
Liquid drop has one surface, so excess pressure is 2S/R, not 4S/R.
Forgetting cosθ in Capillary Rise
The sign of cosθ decides rise or fall.
Thinking Surface Tension Increases with Temperature
Surface tension generally decreases when temperature increases.
Surface tension is force acting per unit length along the liquid surface.
Variables
S=Surface tension
F=Surface force
l=Length of line over which force acts
Work required to increase surface area of a liquid by ΔA.
Variables
S=Surface tension
ΔA=Increase in surface area
Height of rise or fall of liquid in a capillary tube.
Variables
h=Capillary rise or fall
S=Surface tension
θ=Angle of contact
ρ=Density of liquid
r=Radius of capillary tube
Formula Sheet
10Pressure is the normal force acting per unit area.
Variables
P=Pressure
F=Normal force
A=Area
Pressure at depth h below the free surface of a liquid open to atmosphere.
Variables
P=Pressure at depth
P0=Pressure at free surface
ρ=Density of liquid
g=Acceleration due to gravity
h=Depth
For steady incompressible flow, volume flow rate remains constant.
Variables
A1, A2=Cross-sectional areas
v1, v2=Fluid speeds
Energy conservation per unit volume for ideal fluid flow along a streamline.
Variables
P=Pressure energy per unit volume
1/2ρv²=Kinetic energy per unit volume
ρgh=Potential energy per unit volume
Surface tension is force per unit length acting along a liquid surface.
Variables
S=Surface tension
F=Surface force
l=Length over which force acts
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NEET PYQs — Mechanical Properties of Fluids
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Water rises to height $h$ in a capillary tube. If the length of capillary tube above the surface of water is made less than $h$, then:
The cylindrical tube of a spray pump has radius $R$, one end of which has fine holes, each of radius $r$. If the speed of the liquid in the tube is $V$, the speed of ejection of the liquid through the holes is:
The heart of a man pumps $5$ litres of blood through the arteries per minute at a pressure of $150\,\text{mm}$ of mercury. If the density of mercury is $13.6\times10^3\,\text{kg/m}^{3}$ and $g=10\,\text{m/s}^{2}$, then the power of heart in watt is:
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