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Class 11 Physics · NCERT Chapter 9

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Mechanical Properties of Fluids Class 11 Physics Notes

Complete, exam-ready notes on the mechanical properties of fluids: pressure and its variation with depth, Pascal's law and hydraulic machines, Archimedes' principle, streamline and turbulent flow, the equation of continuity, Bernoulli's principle and its applications, viscosity and Stokes' law, and surface tension and capillary rise — every NCERT topic with MCQs, mark-wise questions and solved numericals for CBSE, JEE and NEET.

Chapter:Mechanical Properties of FluidsClass:Class 11Subject:PhysicsBoard:CBSEExams:CBSE · JEE · NEET
10 Key Formulas3 Solved Examples40 Practice MCQs
DWritten byDeep Narayan
Updated
Key Concept Summary

State Bernoulli's principle and write its equation.

For an incompressible, non-viscous fluid in steady flow, the total mechanical energy per unit volume is constant along a streamline: P + ½ρv² + ρgh = constant. Where the speed of the fluid is higher, the pressure is lower.

01

Pressure and Its Variation with Depth

Definition

Pressure

Pressure is the normal force acting per unit area: P = F/a. Its SI unit is the pascal (1 Pa = 1 N m⁻²). In a fluid at rest, pressure is the same in all directions about any point and acts normally to any surface.

Pressure at a depth h below the free surface

The pressure at any point in a fluid at rest equals the atmospheric pressure P₀ plus ρgh, where ρ is the fluid density, g the gravitational acceleration and h the depth below the free surface. Hence pressure increases uniformly with depth and is the same in all directions at a given depth.

  • The pressure does not depend on the shape of the container — only on depth.
  • Two vessels of different shapes connected at the bottom reach the same liquid level.
  • Gauge pressure = P − P_atm = ρgh; the manometer and barometer work on this principle.

Why dams are thicker at the bottom

Because pressure increases with depth, the walls of a dam experience the greatest force at the bottom and are therefore built thicker there.

MCQ Questions

Q1
The SI unit of pressure is —
Q2
Pressure at a depth h in a liquid of density ρ is —
Q3
The pressure at a point inside a liquid at rest —
Q4
Gauge pressure is —

1 Mark Questions

  1. 1
    Define pressure. Write its SI unit.
  2. 2
    Write the expression for pressure at a depth h in a liquid.
  3. 3
    Define gauge pressure.

2 Mark Questions

  1. 1
    Find the pressure at a depth of 10 m below the surface of water. (ρ = 1000 kg m⁻³, g = 10 m/s², atmospheric pressure = 10⁵ Pa.)
  2. 2
    Why is a dam wall thicker at the bottom than at the top?
  3. 3
    Distinguish between absolute pressure and gauge pressure.

3 Mark Questions

  1. 1
    Derive an expression for the pressure at a depth h inside a liquid at rest, taking atmospheric pressure into account.
  2. 2
    A rectangular tank is filled with water up to a height of 2 m. Find the total force on a wall of dimensions 2 m × 3 m due to the water. (ρ = 1000 kg m⁻³, g = 10 m/s².)
02

Pascal's Law and Hydraulic Machines

Definition

Pascal's law

For a fluid at rest, the pressure at any point within the fluid and at the walls of its container is transmitted undiminished in all directions. A change in pressure applied to an enclosed fluid is transmitted equally to every part of the fluid and the walls of its container.

Hydraulic amplification by Pascal's law

The hydraulic lift, hydraulic press and hydraulic brakes all exploit Pascal's law. A small force F₁ applied on a small piston of area A₁ produces the same pressure throughout, giving a much larger force F₂ on a large piston of area A₂, since F₂ = F₁(A₂/A₁). The mechanical advantage is the ratio of the areas.

  • Hydraulic brakes use Pascal's law to transmit the driver's pedal force to all four wheels.
  • A small input force can lift a heavy car on a hydraulic lift.
  • The principle works because liquids are nearly incompressible.

Big area, big force

The larger the ratio of the piston areas A₂/A₁, the greater the force amplification. Work is conserved — the small piston moves a larger distance while the large piston moves a smaller one.

MCQ Questions

Q1
Pascal's law is valid for —
Q2
A hydraulic lift multiplies force in proportion to the —
Q3
Hydraulic machines work because liquids are —
Q4
If the area of the output piston is five times that of the input piston, a force of 50 N produces an output force of —

1 Mark Questions

  1. 1
    State Pascal's law.
  2. 2
    Name two machines that work on Pascal's law.
  3. 3
    Write the formula for the force amplification in a hydraulic press.

2 Mark Questions

  1. 1
    A hydraulic lift has pistons of areas 10 cm² and 200 cm². What force is needed on the small piston to lift a car of weight 2000 N?
  2. 2
    Explain the working of hydraulic brakes using Pascal's law.
  3. 3
    State Pascal's law and explain why it is the basis of the hydraulic press.

3 Mark Questions

  1. 1
    State and explain Pascal's law, and derive the force amplification in a hydraulic lift.
  2. 2
    The small piston of a hydraulic press has a diameter of 2 cm and the large piston a diameter of 20 cm. If a force of 10 N is applied to the small piston, find the force on the large piston.
03

Archimedes' Principle and Floatation

Definition

Archimedes' principle

A body wholly or partially immersed in a fluid experiences an upward buoyant force equal to the weight of the fluid displaced by it. The buoyant force acts through the centre of buoyancy and depends only on the volume of fluid displaced.

Buoyant force

For floatation, the weight of the floating body equals the weight of the fluid displaced. A body sinks if its density exceeds that of the fluid and floats if its density is lower. This is why a steel ship floats — its average density (including the air inside) is less than water.

  • The fraction of a floating body submerged equals the ratio of its density to the fluid's density.
  • A hydrometer measures the density of a liquid by the depth it sinks.
  • An iceberg floats with about 90% of its volume submerged because ice is slightly less dense than water.

The ship that floats

A solid block of steel sinks because its density exceeds water's. But shaped as a hollow hull, its average density is less than water, so the buoyant force matches its weight and it floats.

MCQ Questions

Q1
The buoyant force on a body immersed in a fluid equals —
Q2
A body floats if its average density is —
Q3
The fraction of a floating body submerged is —
Q4
An iceberg floats because —

1 Mark Questions

  1. 1
    State Archimedes' principle.
  2. 2
    What is the condition for a body to float?
  3. 3
    State the condition for a body to sink in a liquid.

2 Mark Questions

  1. 1
    A body of volume 2 × 10⁻³ m³ is fully immersed in water. Find the buoyant force on it. (ρ = 1000 kg m⁻³, g = 10 m/s².)
  2. 2
    Explain why a solid steel ball sinks in water but a steel ship floats.
  3. 3
    A body floats with one quarter of its volume above water. Find the ratio of its density to that of water.

3 Mark Questions

  1. 1
    State Archimedes' principle and use it to show the condition for floatation.
  2. 2
    A cube of side 5 cm floats in water with 60% of its volume submerged. Find the density of the cube. (ρ_water = 1000 kg m⁻³.)
04

Equation of Continuity and Bernoulli's Principle

Definition

Equation of continuity

For an incompressible fluid in steady flow, the mass flowing past any cross-section per unit time is constant. Since density is constant, A₁v₁ = A₂v₂ — the product of area and speed is constant. Where the tube narrows, the fluid speeds up.

Equation of continuity (volume flow rate)
Definition

Bernoulli's principle

For an incompressible, non-viscous fluid flowing steadily, the sum of the pressure energy, kinetic energy per unit volume and potential energy per unit volume is constant along a streamline: P + ½ρv² + ρgh = constant. It is a statement of energy conservation for fluid flow.

Bernoulli's equation

The most important consequence is that where the fluid speed is higher, the pressure is lower. This explains the lift on an aeroplane wing (faster air over the top, lower pressure), the working of a venturi meter, the atomiser and blow, and the curved flight of a spinning ball (Magnus effect).

Assumptions of Bernoulli's equation

Bernoulli's equation holds only for steady, incompressible, non-viscous (frictionless) flow. Real viscous fluids dissipate energy, so the equation is an idealisation.

MCQ Questions

Q1
For an incompressible fluid in steady flow, A₁v₁ = A₂v₂ is the —
Q2
Where the cross-section of a pipe narrows, the speed of an incompressible fluid —
Q3
Bernoulli's principle states that where fluid speed is higher, the pressure is —
Q4
The lift on an aeroplane wing is explained by —

1 Mark Questions

  1. 1
    State the equation of continuity for an incompressible fluid.
  2. 2
    Write Bernoulli's equation for a horizontal pipe.
  3. 3
    State Bernoulli's principle.

2 Mark Questions

  1. 1
    Water flows in a pipe of area 40 cm² at 2 m/s. Find the speed in a section of the pipe of area 10 cm².
  2. 2
    State and explain Bernoulli's principle, and give one application.
  3. 3
    Derive the equation of continuity for an incompressible fluid.

3 Mark Questions

  1. 1
    Derive Bernoulli's equation for the steady flow of an ideal incompressible fluid and state the assumptions made.
  2. 2
    Water flows through a horizontal pipe of cross-section 30 cm² where its speed is 2 m/s and pressure 2 × 10⁵ Pa. In a narrower section of area 10 cm² the speed rises; find the pressure there. (ρ = 1000 kg m⁻³.)
05

Viscosity and Stokes' Law

Definition

Viscosity

Viscosity is the property of a fluid by which it resists relative motion between its layers — it is the internal friction of a fluid. The viscous force between two layers separated by distance dy and moving with velocity difference dv is F = ηA(dv/dy), where η is the coefficient of viscosity.

Viscous force (Newton's law of viscosity)

The SI unit of viscosity is the poiseuille (Pa s); the cgs unit is the poise. Viscosity of liquids decreases with temperature, while that of gases increases. Honey is far more viscous than water.

Definition

Stokes' law

When a sphere of radius r falls through a viscous fluid with terminal velocity vₜ, the viscous drag opposing its motion is F = 6πηrvₜ. The terminal velocity is vₜ = (2/9)(r²/η)(ρ_sphere − ρ_fluid)g.

Stokes' law and terminal velocity

Why does a parachute fall steadily?

As a body falls through a fluid, the viscous drag grows with speed until it balances the weight. From then on the body falls at a constant terminal velocity — no further acceleration.

MCQ Questions

Q1
The property of a fluid that resists relative motion between its layers is called —
Q2
The SI unit of coefficient of viscosity is —
Q3
Stokes' law for a falling sphere gives the viscous force as —
Q4
Terminal velocity is the constant speed at which —

1 Mark Questions

  1. 1
    Define viscosity.
  2. 2
    State Stokes' law.
  3. 3
    Define terminal velocity.

2 Mark Questions

  1. 1
    A sphere of radius 1 mm falls through water of viscosity 0.001 Pa s at a terminal velocity of 2 cm/s. Find the viscous force on it.
  2. 2
    Why does the viscosity of liquids decrease with temperature but that of gases increase?
  3. 3
    Explain how a parachute achieves a constant terminal velocity.

3 Mark Questions

  1. 1
    State Stokes' law and derive an expression for the terminal velocity of a sphere falling through a viscous fluid.
  2. 2
    A rain drop of radius 0.1 mm falls through air with viscosity 1.8 × 10⁻⁵ Pa s. Estimate its terminal velocity. (ρ_water = 1000 kg m⁻³, ρ_air ≈ 0, g = 10 m/s².)
06

Surface Tension and Capillarity

Definition

Surface tension

Surface tension is the property of a liquid surface by which it behaves like a stretched elastic membrane, tending to minimise its area. It is the force per unit length acting along the free surface: S = F/L. Its SI unit is N m⁻¹.

Surface tension and capillary rise

Surface tension arises because molecules at the surface have fewer neighbours and hence higher potential energy — the liquid pulls them inward. It explains why a needle floats on water, why drops are spherical, and the rise (or fall) of a liquid in a narrow capillary tube: h = 2S cosθ/(ρgr). Water rises in a glass tube because it wets it (θ < 90°).

  • Small liquid drops and soap bubbles are spherical because a sphere has minimum surface area.
  • Surface tension decreases with temperature.
  • Capillary rise is greater in narrower tubes.

Narrower tube, higher rise

The height of liquid rise in a capillary tube is inversely proportional to the radius (h ∝ 1/r). A thinner tube pulls the liquid higher — think of a wick drawing up oil.

MCQ Questions

Q1
Surface tension is the —
Q2
The SI unit of surface tension is —
Q3
A small liquid drop is spherical because —
Q4
In a capillary tube, the height of liquid rise is —

1 Mark Questions

  1. 1
    Define surface tension. Write its SI unit.
  2. 2
    Write the expression for the capillary rise of a liquid.
  3. 3
    Why are small liquid drops spherical?

2 Mark Questions

  1. 1
    Water rises to 4 cm in a capillary tube of radius 0.5 mm. Find the surface tension of water. (ρ = 1000 kg m⁻³, cosθ ≈ 1, g = 10 m/s².)
  2. 2
    Explain why a needle can float on the surface of water although steel is denser than water.
  3. 3
    State the factors on which the capillary rise of a liquid depends.

3 Mark Questions

  1. 1
    Explain the phenomenon of surface tension and derive the ascent of a liquid in a capillary tube.
  2. 2
    A liquid of surface tension 0.072 N m⁻¹ rises to 2 cm in a capillary tube of radius 0.36 mm. Find the density of the liquid. (cosθ = 1, g = 10 m/s².)
07

NCERT Exercise Questions

From the textbook

All NCERT questions for this chapter — NCERT Physics Part II, Chapter 9 (Mechanical Properties of Fluids). Questions keep their NCERT numbering so you can match them to the book.

Exercises (NCERT Q9.1–Q9.20)

  • 9.1) Explain why (a) The blood pressure in humans is greater at the feet than at the brain (b) Atmospheric pressure at a height of about 6 km decreases to nearly half of its value at the sea level, though the height of the atmosphere is more than 100 km (c) Hydrostatic pressure is a scalar quantity even though pressure is force divided by area.
  • 9.2) Explain why (a) The angle of contact of mercury with glass is obtuse, while that of water with glass is acute. (b) Water on a clean glass surface tends to spread out while mercury on the same surface tends to form drops. (Put differently, water wets glass while mercury does not.) (c) Surface tension of a liquid is independent of the area of the surface (d) Water with detergent dissolved in it should have small angles of contact. (e) A drop of liquid under no external forces is always spherical in shape.
  • 9.3) Fill in the blanks using the word(s) from the list appended with each statement: (a) Surface tension of liquids generally ... with temperatures (increases / decreases) (b) Viscosity of gases ... with temperature, whereas viscosity of liquids ... with temperature (increases / decreases) (c) For solids with elastic modulus of rigidity, the shearing force is proportional to ..., while for fluids it is proportional to ... (shear strain / rate of shear strain) (d) For a fluid in a steady flow, the increase in flow speed at a constriction follows (conservation of mass / Bernoulli's principle) (e) For the model of a plane in a wind tunnel, turbulence occurs at a ... speed for turbulence for an actual plane (greater / smaller)
  • 9.4) Explain why (a) To keep a piece of paper horizontal, you should blow over, not under, it (b) When we try to close a water tap with our fingers, fast jets of water gush through the openings between our fingers (c) The size of the needle of a syringe controls flow rate better than the thumb pressure exerted by a doctor while administering an injection (d) A fluid flowing out of a small hole in a vessel results in a backward thrust on the vessel (e) A spinning cricket ball in air does not follow a parabolic trajectory.
  • 9.5) A 50 kg girl wearing high heel shoes balances on a single heel. The heel is circular with a diameter 1.0 cm. What is the pressure exerted by the heel on the horizontal floor?
  • 9.6) Toricelli's barometer used mercury. Pascal duplicated it using French wine of density 984 kg m⁻³. Determine the height of the wine column for normal atmospheric pressure.
  • 9.7) A vertical off-shore structure is built to withstand a maximum stress of 10⁹ Pa. Is the structure suitable for putting up on top of an oil well in the ocean? Take the depth of the ocean to be roughly 3 km, and ignore ocean currents.
  • 9.8) A hydraulic automobile lift is designed to lift cars with a maximum mass of 3000 kg. The area of cross-section of the piston carrying the load is 425 cm². What maximum pressure would the smaller piston have to bear?
  • 9.9) A U-tube contains water and methylated spirit separated by mercury. The mercury columns in the two arms are in level with 10.0 cm of water in one arm and 12.5 cm of spirit in the other. What is the specific gravity of spirit?
  • 9.10) In the previous problem, if 15.0 cm of water and spirit each are further poured into the respective arms of the tube, what is the difference in the levels of mercury in the two arms? (Specific gravity of mercury = 13.6)
  • 9.11) Can Bernoulli's equation be used to describe the flow of water through a rapid in a river? Explain.
  • 9.12) Does it matter if one uses gauge instead of absolute pressures in applying Bernoulli's equation? Explain.
  • 9.13) Glycerine flows steadily through a horizontal tube of length 1.5 m and radius 1.0 cm. If the amount of glycerine collected per second at one end is 4.0 × 10⁻³ kg s⁻¹, what is the pressure difference between the two ends of the tube? (Density of glycerine = 1.3 × 10³ kg m⁻³ and viscosity of glycerine = 0.83 Pa s). [You may also like to check if the assumption of laminar flow in the tube is correct].
  • 9.14) In a test experiment on a model aeroplane in a wind tunnel, the flow speeds on the upper and lower surfaces of the wing are 70 m s⁻¹ and 63 m s⁻¹ respectively. What is the lift on the wing if its area is 2.5 m²? Take the density of air to be 1.3 kg m⁻³.
  • 9.15) Figures 9.20(a) and (b) refer to the steady flow of a (non-viscous) liquid. Which of the two figures is incorrect? Why?
  • 9.16) The cylindrical tube of a spray pump has a cross-section of 8.0 cm² one end of which has 40 fine holes each of diameter 1.0 mm. If the liquid flow inside the tube is 1.5 m min⁻¹, what is the speed of ejection of the liquid through the holes?
  • 9.17) A U-shaped wire is dipped in a soap solution, and removed. The thin soap film formed between the wire and the light slider supports a weight of 1.5 × 10⁻² N (which includes the small weight of the slider). The length of the slider is 30 cm. What is the surface tension of the film?
  • 9.18) Figure 9.21 (a) shows a thin liquid film supporting a small weight = 4.5 × 10⁻² N. What is the weight supported by a film of the same liquid at the same temperature in Fig. (b) and (c)? Explain your answer physically.
  • 9.19) What is the pressure inside the drop of mercury of radius 3.00 mm at room temperature? Surface tension of mercury at that temperature (20 °C) is 4.65 × 10⁻¹ N m⁻¹. The atmospheric pressure is 1.01 × 10⁵ Pa. Also give the excess pressure inside the drop.
  • 9.20) What is the excess pressure inside a bubble of soap solution of radius 5.00 mm, given that the surface tension of soap solution at the temperature (20 °C) is 2.50 × 10⁻² N m⁻¹? If an air bubble of the same dimension were formed at depth of 40.0 cm inside a container containing the soap solution (of relative density 1.20), what would be the pressure inside the bubble? (1 atmospheric pressure is 1.01 × 10⁵ Pa).

Answers at a glance

  1. 1
    Q9.1 → (a) P = hρg and the feet lie below a taller blood column (b) air density halves by 6 km; the tenuous upper air adds little pressure (c) hydrostatic pressure acts in all directions, so it is a scalar.
  2. 2
    Q9.2 → (a) weak adhesion of mercury versus strong adhesion of water to glass (b) cohesive mercury forms drops, adhesive water spreads (c) it is a per-unit-length force (d) small θ gives fast capillary rise (e) a sphere minimizes surface area.
  3. 3
    Q9.3 → (a) decreases (b) increases; decreases (c) shear strain; rate of shear strain (d) conservation of mass (e) greater.
  4. 4
    Q9.4 → (a) faster air above lowers pressure (b) continuity: smaller area, higher speed (c) the needle area, not the thumb, controls rate (d) reaction to the momentum of the jet (e) the Magnus/Bernoulli sideways force curves the flight.
  5. 5
    Q9.5 → Pressure = 6.24 × 10⁶ N m⁻².
  6. 6
    Q9.6 → The wine column would be 10.5 m high.
  7. 7
    Q9.7 → Yes: ocean pressure at 3 km is only 2.94 × 10⁷ Pa, well below 10⁹ Pa.
  8. 8
    Q9.8 → Maximum pressure on the smaller piston = 6.917 × 10⁵ Pa.
  9. 9
    Q9.9 → Specific gravity of spirit = 0.8.
  10. 10
    Q9.10 → The mercury levels differ by about 0.22 cm.
  11. 11
    Q9.11 → No — a rapid is turbulent flow, and Bernoulli's equation requires streamline flow.
  12. 12
    Q9.12 → No — the atmospheric term cancels; gauge and absolute pressures give the same difference.
  13. 13
    Q9.13 → Pressure difference = 9.8 × 10² Pa; Reynolds number ≈ 0.3, so the flow is laminar.
  14. 14
    Q9.14 → Lift ≈ 1.51 × 10³ N.
  15. 15
    Q9.15 → Figure (a) is incorrect — pressure (and hence the liquid level) falls at the high-speed constriction.
  16. 16
    Q9.16 → Speed of ejection ≈ 0.64 m s⁻¹.
  17. 17
    Q9.17 → Surface tension = 2.5 × 10⁻² N m⁻¹.
  18. 18
    Q9.18 → Figures (b) and (c) also support 4.5 × 10⁻² N, the same liquid and slider length giving the same force.
  19. 19
    Q9.19 → Excess pressure = 310 Pa; total pressure inside ≈ 1.01 × 10⁵ Pa.
  20. 20
    Q9.20 → Soap bubble excess = 20 Pa; air bubble at 40 cm depth: total pressure ≈ 1.06 × 10⁵ Pa.
08

CBSE Pattern Questions

How CBSE asks this chapter

Physics board paper structure: Section A (MCQ/VSA 1M), Section B (2M), Section C (3M), Section D (5M). Mechanical Properties of Fluids typically carries ~7 marks: 1-mark MCQs on Pascal's law, buoyancy or surface tension, a 2-mark numerical on pressure, a 3-mark derivation of Bernoulli's equation or excess pressure, and a 5-mark question on viscosity/terminal velocity or capillary rise.

MCQ Questions

Q1
Pascal's law states that pressure applied to an enclosed fluid is transmitted
Q2
The pressure at a depth h in a liquid of density ρ is
Q3
The upward buoyant force on a body equals
Q4
The excess pressure inside a spherical soap bubble of radius R and surface tension T is

1 Mark Questions

  1. 1
    State Pascal's law for fluids at rest.
  2. 2
    Define the buoyant force and state Archimedes' principle.
  3. 3
    Define surface tension and give its SI unit.
  4. 4
    State Bernoulli's theorem for a streamline flow of an ideal fluid.

2 Mark Questions

  1. 1
    A submarine is at a depth of 20 m in water of density 1000 kg/m³. Find the pressure on it (g = 10 m/s², P₀ = 10⁵ Pa). (Ans: P = P₀ + ρgh = 3 × 10⁵ Pa)
  2. 2
    Water flows in a horizontal pipe that narrows from 4 cm² to 1 cm². If the speed in the narrow part is 8 m/s, find the speed in the wide part. (Ans: v₁A₁ = v₂A₂ ⇒ v₁ = 2 m/s)
  3. 3
    A drop of water of radius 1 mm falls with terminal velocity in air. If the viscosity of air is 1.8 × 10⁻⁵ Pa s and effective density is 1000 kg/m³, state the balance of forces. (Ans: 6πrv = (4/3)πr³ρg)

3 Mark Questions

  1. 1
    Derive Bernoulli's equation P + ½ρv² + ρgh = constant for a streamline flow and state the assumptions made.
  2. 2
    Derive the expression for the excess pressure inside a liquid drop and inside a soap bubble. (Ans: 2T/r; 4T/r)
  3. 3
    Explain Stokes' law and derive the expression for the terminal velocity of a sphere falling in a viscous fluid. (Ans: vt = 2r²(ρ − σ)g/(9η))

5 Mark Questions

  1. 1
    Describe the phenomenon of capillarity, derive the expression for the height of a liquid column in a capillary tube, and explain its dependence on radius and angle of contact. (Ans: h = 2T cos θ/(rρg))
  2. 2
    Derive the equation of continuity and Bernoulli's equation, and explain with the help of a diagram how the venturi meter and the atomizer work on Bernoulli's principle.
09

PDF: Assignments & Tests

Printable study material

Free downloadable PDFs for Mechanical Properties of Fluids — two topic-wise assignments covering every concept of the chapter, and two full CBSE-pattern tests (each 90 minutes, 40 marks) mirroring the board paper. No signup required.

Free PDF Downloads & Assignments

No Signup Required

Practice path: complete Assignment 1 first (topic-by-topic), then Assignment 2 (mixed difficulty with full solutions), then attempt the timed tests.

Mechanical Properties of Fluids Assignment 1 — Topic-wise Questions

Covers all six topics: pressure and its variation with depth; Pascal's law and hydraulic machines; Archimedes' principle and floatation; the equation of continuity and Bernoulli's principle; viscosity and Stokes' law; and surface tension and capillarity. Arranged topic by topic.

mechanical-properties-of-fluids-class-11-notes-assignment-1.pdf
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Mechanical Properties of Fluids Assignment 2 — Challenge + Integrated Problems

Higher-difficulty set with multi-topic integration problems (depth pressure, hydraulic lifts, buoyancy, continuity and Bernoulli, Stokes' law, capillary rise) and full worked answers. Includes an answer key.

mechanical-properties-of-fluids-class-11-notes-assignment-2.pdf
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Mechanical Properties of Fluids Test 1 — CBSE Pattern (90 min, 40 marks)

Full board-pattern test: Section A (MCQ/VSA 1M × 10), Section B (2M × 4), Section C (3M × 4), Section D (5M × 2) = 40 marks. Time: 90 minutes. Includes answer key.

mechanical-properties-of-fluids-class-11-notes-test-1-cbse.pdf
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Mechanical Properties of Fluids Test 2 — CBSE Pattern (90 min, 40 marks)

Second full paper with different questions, same 40-mark / 90-minute blueprint. Includes answer key.

mechanical-properties-of-fluids-class-11-notes-test-2-cbse.pdf
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Quick Revision

Key formulas at a glance

Memorise these equations — direct application numericals and derivations in CBSE & JEE frequently hinge on these.

Pressure with depth

Pascal's law

Buoyant force

Equation of continuity

Bernoulli's equation

Viscous force

Stokes' law

Terminal velocity

Surface tension

Capillary rise

Exam Strategy

How this chapter is asked

High-yield question patterns observed across CBSE boards, JEE Main & Advanced, and NEET.

  • Pressure increases with depth: P = P₀ + ρgh.
  • Pascal's law: pressure transmitted undiminished in a fluid at rest.
  • Buoyant force = weight of displaced fluid; float if average density less than the fluid.
  • Continuity: A₁v₁ = A₂v₂.
  • Bernoulli: P + ½ρv² + ρgh = constant; higher speed → lower pressure.
  • Stokes' law F = 6πηrv; terminal velocity ∝ r².
  • Surface tension S = F/L; capillary rise h = 2S cosθ/(ρgr).

Practice Numericals

Step-by-step worked examples

Standard exam-level problems solved with clear conceptual breakdowns.

1

Pressure at depth

Problem StatementFind the pressure at a depth of 20 m in a lake. (ρ = 1000 kg m⁻³, g = 10 m/s², atmospheric pressure = 1.01 × 10⁵ Pa.)

Step-by-Step Solution

  1. 1P = P₀ + ρgh = 1.01 × 10⁵ + 1000 × 10 × 20.
  2. 2P = 1.01 × 10⁵ + 2 × 10⁵ = 3.01 × 10⁵ Pa.

Final Answer

3.01 × 10⁵ Pa

2

Hydraulic lift force

Problem StatementA hydraulic lift has pistons of areas 25 cm² and 500 cm². What force on the small piston will lift a car of weight 10000 N?

Step-by-Step Solution

  1. 1Pascal's law: F₁/A₁ = F₂/A₂.
  2. 2F₁ = F₂ × A₁/A₂ = 10000 × 25/500 = 10000 × 0.05 = 500 N.

Final Answer

500 N

3

Bernoulli pressure in a narrow pipe

Problem StatementWater flows in a horizontal pipe of area 20 cm² at 2 m/s with pressure 2 × 10⁵ Pa. In a section of area 10 cm², find the pressure. (ρ = 1000 kg m⁻³.)

Step-by-Step Solution

  1. 1Continuity: A₁v₁ = A₂v₂ → v₂ = v₁ × A₁/A₂ = 2 × 20/10 = 4 m/s.
  2. 2Bernoulli (horizontal, h same): P₁ + ½ρv₁² = P₂ + ½ρv₂².
  3. 3P₂ = P₁ + ½ρ(v₁² − v₂²) = 2×10⁵ + ½×1000×(4 − 16) = 2×10⁵ − 6000 = 1.94×10⁵ Pa.

Final Answer

1.94 × 10⁵ Pa

FAQ

Frequently asked questions

Why does pressure in a liquid increase with depth?

At a greater depth the liquid above exerts a larger weight, so the pressure rises by ρgh. This is why dams are built thicker at the bottom and divers feel increased pressure as they go deeper.

How does a hydraulic lift lift a heavy car with a small force?

By Pascal's law, the pressure applied on a small piston is transmitted undiminished to a much larger piston. Since pressure = force/area, the larger area produces a larger force: F₂ = F₁(A₂/A₁).

Why can a steel ship float even though steel is denser than water?

A solid block of steel sinks, but a ship's hollow hull has a large volume and low average density (including the air inside). Its weight equals the buoyant force (weight of displaced water), so it floats.

What is the physical meaning of the equation of continuity?

It expresses conservation of mass in steady flow: the same mass must pass every cross-section per second. For an incompressible fluid this becomes A₁v₁ = A₂v₂ — narrower pipes force the fluid to flow faster.

Why does a liquid climb higher in a thinner capillary tube?

Capillary rise is h = 2S cosθ/(ρgr). Since the rise is inversely proportional to the radius r, a narrower tube holds the liquid column higher — the effect behind wicks drawing up oil and water soaking into paper.

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