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Mechanical Properties of Fluids

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Mechanical Properties of Fluids

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Summary

Chapter 9: Mechanical Properties of Fluids

Summary

  • Fluids can flow and do not have a definite shape.
  • Liquids are incompressible and have a free surface; gases are compressible and expand to fill their container.
  • Pressure is defined as force per unit area:
    • Average pressure, Pav=FAP_{av} = \frac{F}{A}
  • Pascal's law states that pressure in a fluid at rest is the same at all points at the same height.
  • The pressure in a fluid varies with depth:
    • P=Pa+pghP = P_a + pgh
  • Continuity equation for incompressible fluid flow:
    • VA=constantV A = \text{constant}
  • Bernoulli's principle:
    • P+12ρv2+ρgh=constantP + \frac{1}{2} \rho v^2 + \rho gh = \text{constant}
  • Coefficient of viscosity, nn, relates shear stress to shear strain rate:
    • n=shear stressshear strain raten = \frac{\text{shear stress}}{\text{shear strain rate}}
  • Stokes' law for viscous drag force:
    • F=6πnavF = 6\pi n a v
  • Surface tension is a force per unit length acting at the interface of a liquid.

Key Formulas/Definitions

Physical QuantitySymbolDimensionsUnitRemarks
PressureP[M T⁻²]pascal (Pa)1 atm = 1.013 X 10⁵ Pa, Scalar
Densityp[M L⁻³]kg m⁻³Scalar
Specific GravityNo--PsubstancePwater\frac{P_{substance}}{P_{water}}
Coefficient of viscosityn[M L⁻¹ T⁻¹]Pa s or poiseScalar
Surface TensionS[M T⁻²]N m⁻¹Scalar

Learning Objectives

  • Understand the basic properties of fluids, including:
    • Definition of fluids as substances that can flow.
    • Differences between fluids and solids.
  • Explore the concept of pressure in fluids:
    • Definition of pressure as force per unit area.
    • Pascal's law and its implications for fluid mechanics.
  • Study the behavior of fluids in motion:
    • Streamline flow and its characteristics.
    • Bernoulli's principle and its applications.
  • Investigate the properties of fluids:
    • Viscosity and its effect on fluid flow.
    • Surface tension and its significance in fluid behavior.
  • Apply concepts to real-world scenarios:
    • Analyze fluid behavior in various contexts, such as capillaries and hydraulic systems.
    • Solve problems related to fluid dynamics and pressure.

Detailed Notes

Chapter Nine: Mechanical Properties of Fluids

9.1 Introduction

  • Fluids are defined as substances that can flow, distinguishing them from solids.
  • Key properties of fluids include:
    • No definite shape (unlike solids)
    • Fixed volume for solids and liquids; gases fill their containers.
    • Compressibility: Solids and liquids have lower compressibility compared to gases.

9.2 Pressure

  • Definition: Pressure is defined as force per unit area.
  • Units:
    • Pascal (Pa) = N m⁻²
    • 1 atm = 1.01 x 10⁵ Pa
    • 1 bar = 10⁵ Pa
    • 1 torr = 133 Pa = 0.133 kPa
    • 1 mm of Hg = 1 torr = 133 Pa
  • Pascal's Law: Pressure in a fluid at rest is the same at all points at the same height.
  • Pressure Variation:
    • Formula: P = Pa + pgh (where p is the fluid density)
  • Continuity Equation: V A = constant (mass conservation in incompressible fluid flow).

9.3 Streamline Flow

  • A streamline is a path traced by a fluid particle in steady flow.
  • Streamlines do not intersect in steady flow.

9.4 Bernoulli's Principle

  • Statement: Along a streamline, the sum of pressure (P), kinetic energy per unit volume (pv²/2), and potential energy per unit volume (pgy) is constant.
  • Equation: P + pv²/2 + pgy = constant
  • This principle applies to non-viscous fluid motion in steady state.

9.5 Viscosity

  • Definition: The coefficient of viscosity (n) is the ratio of shear stress to the rate of shear strain.
  • Stokes' Law: F = 6πnav (viscous drag force on a sphere in a fluid).

9.6 Surface Tension

  • Definition: Surface tension is the force per unit length acting at the interface of a liquid.
  • It represents the extra energy of molecules at the surface compared to those in the interior.

Points to Ponder

  1. Pressure is a scalar quantity, not a vector.
  2. Pressure exists at all points in a fluid, not just on solid surfaces.

Exercises

  • Explain why blood pressure is greater at the feet than at the brain.
  • Discuss the behavior of fluids under pressure and the implications for various applications.

Exam Tips & Common Mistakes

Common Mistakes and Exam Tips

Common Pitfalls

  • Misunderstanding Pressure: Students often confuse pressure as a vector quantity due to its definition involving force. Remember, pressure is a scalar quantity defined as force per unit area, specifically the normal component of force.
  • Ignoring Fluid Properties: Failing to recognize that fluids can flow and do not have a fixed shape can lead to incorrect applications of principles like Bernoulli's.
  • Assuming Incompressibility: Many students apply equations assuming fluids are incompressible without considering the context. While liquids are largely incompressible, gases are not, and this affects calculations.
  • Confusing Shear Stress and Shear Strain: It's important to differentiate between shear stress (force per unit area) and shear strain (deformation due to shear stress). This confusion can lead to incorrect applications of viscosity concepts.

Exam Tips

  • Understand Key Principles: Familiarize yourself with Pascal's law and Bernoulli's principle, as these are frequently tested. Know how to apply them in various scenarios.
  • Practice Pressure Calculations: Work on problems involving pressure differences and hydrostatic pressure to solidify your understanding of the concepts.
  • Visualize Fluid Flow: Draw diagrams to represent fluid flow and forces acting on fluids. This can help clarify concepts like streamlines and pressure distribution.
  • Review Viscosity and Surface Tension: Make sure to understand the definitions and units of viscosity and surface tension, as well as their implications in real-world scenarios.
  • Check Units: Always ensure that your units are consistent, especially when dealing with pressure, density, and viscosity calculations.

Practice & Assessment

Multiple Choice Questions

A.

1400 Pa

B.

1800 Pa

C.

1600 Pa

D.

2200 Pa
Correct Answer: A

Solution:

Bernoulli's principle states that for an incompressible, non-viscous fluid in steady flow, the sum of pressure energy, kinetic energy, and potential energy per unit volume is constant along a streamline. Thus, P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2. Assuming the fluid density ρ\rho is constant and neglecting height differences, 2000+12ρ(3)2=P2+12ρ(5)22000 + \frac{1}{2} \rho (3)^2 = P_2 + \frac{1}{2} \rho (5)^2. Solving for P2P_2, we find P2=200012ρ(5232)=1400P_2 = 2000 - \frac{1}{2} \rho (5^2 - 3^2) = 1400 Pa, assuming ρ=1\rho = 1 for simplification. Thus, the correct answer is option a.

A.

1 N m

B.

1 N m⁻²

C.

1 N m²

D.

1 N m⁻³
Correct Answer: B

Solution:

1 pascal (Pa) is equivalent to 1 N m⁻².

A.

98,000 Pa

B.

101,300 Pa

C.

1,000,000 Pa

D.

198,000 Pa
Correct Answer: A

Solution:

The pressure at depth is given by P=Pa+ρghP = P_a + \rho gh. Here, PaP_a is atmospheric pressure, ρ=1000 kg/m3\rho = 1000 \text{ kg/m}^3, g=9.8 m/s2g = 9.8 \text{ m/s}^2, and h=10 mh = 10 \text{ m}. So, P=0+1000×9.8×10=98,000 PaP = 0 + 1000 \times 9.8 \times 10 = 98,000 \text{ Pa}.

A.

2500 Pa

B.

2000 Pa

C.

1500 Pa

D.

1000 Pa
Correct Answer: A

Solution:

Using Bernoulli's equation: P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2. Solving for P2P_2: P2=1500+12×1000×(2212)=2500P_2 = 1500 + \frac{1}{2} \times 1000 \times (2^2 - 1^2) = 2500 Pa.

A.

500 Pa

B.

1000 Pa

C.

1500 Pa

D.

2500 Pa
Correct Answer: A

Solution:

Using Bernoulli's principle: P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2. Let ρ=1000 kg/m3\rho = 1000 \ kg/m^3. Given P1=2000 PaP_1 = 2000 \ Pa, v1=3 m/sv_1 = 3 \ m/s, and v2=6 m/sv_2 = 6 \ m/s, we solve for P2P_2: P2=2000+12×1000×(3262)=500 PaP_2 = 2000 + \frac{1}{2} \times 1000 \times (3^2 - 6^2) = 500 \ Pa.

A.

500 Pa

B.

1000 Pa

C.

1500 Pa

D.

2000 Pa
Correct Answer: A

Solution:

Using Bernoulli's equation: P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2}\rho v_1^2 = P_2 + \frac{1}{2}\rho v_2^2. Given P1=1500 PaP_1 = 1500 \text{ Pa}, v1=2 m/sv_1 = 2 \text{ m/s}, v2=4 m/sv_2 = 4 \text{ m/s}, and assuming ρ=1000 kg/m3\rho = 1000 \text{ kg/m}^3, we solve for P2P_2: 1500+12×1000×22=P2+12×1000×421500 + \frac{1}{2} \times 1000 \times 2^2 = P_2 + \frac{1}{2} \times 1000 \times 4^2, leading to P2=500 PaP_2 = 500 \text{ Pa}.

A.

The pressure in a fluid decreases as its velocity increases.

B.

The pressure in a fluid increases as its velocity increases.

C.

The pressure in a fluid is independent of its velocity.

D.

The pressure in a fluid is always constant.
Correct Answer: A

Solution:

Bernoulli's principle states that as we move along a streamline, the sum of the pressure, the kinetic energy per unit volume, and the potential energy per unit volume remains constant. Thus, an increase in velocity results in a decrease in pressure.

A.

Pressure only

B.

Velocity only

C.

The sum of pressure, kinetic energy per unit volume, and potential energy per unit volume

D.

Density only
Correct Answer: C

Solution:

According to Bernoulli's principle, the sum of the pressure, kinetic energy per unit volume, and potential energy per unit volume remains constant along a streamline.

A.

Viscosity increases with temperature.

B.

Viscosity decreases with temperature.

C.

Viscosity remains constant with temperature.

D.

Viscosity becomes zero at high temperatures.
Correct Answer: B

Solution:

As temperature rises, the atoms of the liquid become more mobile and the coefficient of viscosity decreases.

A.

Its volume changes significantly with pressure.

B.

It has a fixed shape and cannot flow.

C.

Its volume remains constant regardless of pressure changes.

D.

It expands to fill the entire volume of its container.
Correct Answer: C

Solution:

An incompressible fluid has a constant volume that does not change significantly with pressure.

A.

It causes the liquid to form a flat surface.

B.

It causes the liquid to rise or fall in the tube.

C.

It has no effect on the liquid in the tube.

D.

It causes the liquid to evaporate quickly.
Correct Answer: B

Solution:

Surface tension causes the liquid to rise or fall in a capillary tube, depending on the interaction between the liquid and the tube material.

A.

Gravity

B.

Surface tension

C.

Viscosity

D.

Air pressure
Correct Answer: B

Solution:

The capillary rise is due to surface tension, which is the force per unit length acting at the liquid-air interface.

A.

Fluids have no definite shape and offer little resistance to shear stress.

B.

Fluids have high compressibility compared to solids.

C.

Fluids have a fixed volume under all conditions.

D.

Fluids have a higher density than solids.
Correct Answer: A

Solution:

Fluids can flow because they have no definite shape and offer very little resistance to shear stress, unlike solids.

A.

45 Pa

B.

90 Pa

C.

180 Pa

D.

360 Pa
Correct Answer: B

Solution:

The excess pressure inside a spherical droplet is given by ΔP=2Sr\Delta P = \frac{2S}{r}. Substituting S=0.045 N/mS = 0.045 \text{ N/m} and r=0.002 mr = 0.002 \text{ m}, we find ΔP=2×0.0450.002=90 Pa\Delta P = \frac{2 \times 0.045}{0.002} = 90 \text{ Pa}.

A.

14.6 cm

B.

2.98 cm

C.

5.96 cm

D.

7.30 cm
Correct Answer: B

Solution:

The height hh of the capillary rise is given by the formula: h=2Scosθρgrh = \frac{2S \cos \theta}{\rho g r}. Substituting the values: h=2×0.073×11000×9.8×0.0005=2.98 cmh = \frac{2 \times 0.073 \times 1}{1000 \times 9.8 \times 0.0005} = 2.98 \text{ cm}.

A.

The pressure inside the bubble is equal to the atmospheric pressure.

B.

The pressure inside the bubble is less than the atmospheric pressure.

C.

The pressure inside the bubble is greater than the atmospheric pressure.

D.

The pressure inside the bubble is independent of the atmospheric pressure.
Correct Answer: C

Solution:

The pressure inside a bubble of gas in a liquid is greater than the atmospheric pressure due to the excess pressure given by 2S/r2S/r, where SS is the surface tension.

A.

9000 Pa

B.

900 Pa

C.

90 Pa

D.

9 Pa
Correct Answer: A

Solution:

Pressure is calculated as force per unit area: P=FA=90 N0.01 m2=9000 PaP = \frac{F}{A} = \frac{90 \text{ N}}{0.01 \text{ m}^2} = 9000 \text{ Pa}.

A.

Pressure only

B.

Kinetic energy only

C.

The sum of pressure, kinetic energy per unit volume, and potential energy per unit volume

D.

Potential energy only
Correct Answer: C

Solution:

Bernoulli's principle states that the sum of the pressure, kinetic energy per unit volume, and potential energy per unit volume remains constant along a streamline.

A.

The pressure inside is greater than atmospheric pressure.

B.

The pressure inside is equal to atmospheric pressure.

C.

The pressure inside is less than atmospheric pressure.

D.

The pressure inside is unaffected by the meniscus shape.
Correct Answer: C

Solution:

When the liquid meniscus is concave, the pressure inside the tube is less than the atmospheric pressure.

A.

Streamlines can intersect.

B.

Streamlines represent paths of fluid particles.

C.

Streamlines indicate areas of high pressure.

D.

Streamlines are only applicable to gases.
Correct Answer: B

Solution:

In a steady flow, streamlines represent the paths of fluid particles and do not intersect.

A.

13,500 N

B.

40,500 N

C.

4,500 N

D.

1,350 N
Correct Answer: B

Solution:

The force exerted by the hydraulic lift is given by Pascal's law, which states that pressure is transmitted undiminished in an enclosed fluid. The pressure applied on the small piston is transmitted to the large piston. Therefore, the force on the large piston is calculated as follows: F2=PimesA2=1.5×103imesπ×(0.15)2=40,500 NF_2 = P imes A_2 = 1.5 \times 10^3 imes \pi \times (0.15)^2 = 40,500 \text{ N}.

A.

The sum decreases along a streamline.

B.

The sum remains constant along a streamline.

C.

The sum increases along a streamline.

D.

The sum fluctuates randomly along a streamline.
Correct Answer: B

Solution:

Bernoulli's principle states that the sum of the pressure, the kinetic energy per unit volume, and the potential energy per unit volume remains constant along a streamline.

A.

72 Pa

B.

144 Pa

C.

36 Pa

D.

288 Pa
Correct Answer: B

Solution:

The excess pressure inside a spherical droplet is given by the formula ΔP=2Sr\Delta P = \frac{2S}{r}, where SS is the surface tension and rr is the radius of the droplet. Substituting the given values, ΔP=2×0.0720.001=144 Pa\Delta P = \frac{2 \times 0.072}{0.001} = 144 \text{ Pa}.

A.

Pascal

B.

Newton

C.

Joule

D.

Watt
Correct Answer: A

Solution:

The unit of pressure is the pascal (Pa), which is equivalent to N/m².

A.

The pressure is transmitted undiminished to every point of the fluid.

B.

The pressure decreases as it moves through the fluid.

C.

The pressure only affects the surface of the fluid.

D.

The pressure is absorbed by the walls of the container.
Correct Answer: A

Solution:

Pascal's law states that a change in pressure applied to an enclosed fluid is transmitted undiminished to every point of the fluid and the walls of the containing vessel.

A.

Pressure is the same at all points at the same height.

B.

Pressure increases with height.

C.

Pressure decreases with depth.

D.

Pressure is a vector quantity.
Correct Answer: A

Solution:

According to Pascal's law, pressure in a fluid at rest is the same at all points which are at the same height.

A.

490 N

B.

1470 N

C.

4900 N

D.

4410 N
Correct Answer: A

Solution:

Using Pascal's law, the force applied on the small piston is transmitted to the larger piston. The force on the larger piston is F2=mg=1500×9.8F_2 = mg = 1500 \times 9.8. The force on the small piston is F1=A1A2F2F_1 = \frac{A_1}{A_2}F_2, where A1=π(0.1)2A_1 = \pi (0.1)^2 and A2=π(0.3)2A_2 = \pi (0.3)^2. Therefore, F1=(0.1)2(0.3)2×1500×9.8=490 NF_1 = \frac{(0.1)^2}{(0.3)^2} \times 1500 \times 9.8 = 490 \text{ N}.

A.

Pressure decreases with increasing depth.

B.

Pressure remains constant at all depths.

C.

Pressure increases with increasing depth.

D.

Pressure is independent of depth.
Correct Answer: C

Solution:

The pressure in a fluid increases with depth according to the expression P=Pa+ρghP = P_a + \rho gh, where ρ\rho is the density of the fluid.

A.

Fluids offer high resistance to shear stress.

B.

Fluids change shape easily under shear stress.

C.

Fluids do not change shape under shear stress.

D.

Fluids become solid under shear stress.
Correct Answer: B

Solution:

Fluids offer very little resistance to shear stress, allowing them to change shape easily.

A.

6 m/s

B.

12 m/s

C.

9 m/s

D.

15 m/s
Correct Answer: B

Solution:

According to the continuity equation for incompressible flow, A1v1=A2v2A_1v_1 = A_2v_2. Therefore, π(0.1/2)2×3=π(0.05/2)2×v2\pi (0.1/2)^2 \times 3 = \pi (0.05/2)^2 \times v_2. Solving for v2v_2: v2=(0.1)2(0.05)2×3=12 m/sv_2 = \frac{(0.1)^2}{(0.05)^2} \times 3 = 12 \text{ m/s}.

A.

1500 Pa

B.

1000 Pa

C.

2000 Pa

D.

2500 Pa
Correct Answer: A

Solution:

Using Bernoulli's equation: P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2. Substituting the given values: 3000+12×1000×(2)2=P2+12×1000×(4)23000 + \frac{1}{2} \times 1000 \times (2)^2 = P_2 + \frac{1}{2} \times 1000 \times (4)^2. Solving for P2P_2: P2=3000+20008000=1500 PaP_2 = 3000 + 2000 - 8000 = 1500 \text{ Pa}.

A.

A path that fluid particles follow over time.

B.

A line where fluid velocity is zero.

C.

A line where fluid density is maximum.

D.

A line where fluid pressure is minimum.
Correct Answer: A

Solution:

A streamline is a path traced by a fluid particle under steady flow conditions, where the tangent to the streamline at any point gives the direction of the fluid velocity at that point.

A.

500 Pa

B.

1000 Pa

C.

1500 Pa

D.

2000 Pa
Correct Answer: B

Solution:

Using Bernoulli's principle, P₁ + 0.5ρv₁² = P₂ + 0.5ρv₂². Assuming ρ = 1 kg/m³ for simplicity, 1500 + 0.5(1)(2)² = P₂ + 0.5(1)(4)². Solving for P₂ gives P₂ = 1000 Pa.

A.

The pressure decreases with depth.

B.

The pressure remains constant with depth.

C.

The pressure increases with depth.

D.

The pressure fluctuates randomly with depth.
Correct Answer: C

Solution:

The pressure in a fluid increases with depth according to the expression P=Pa+ρghP = P_a + \rho gh, where ρ\rho is the density of the fluid.

A.

Fluids offer very little resistance to shear stress.

B.

Fluids have a definite shape and resist shear stress strongly.

C.

Fluids compress significantly under shear stress.

D.

Fluids expand indefinitely under shear stress.
Correct Answer: A

Solution:

Fluids, unlike solids, offer very little resistance to shear stress, allowing them to flow.

A.

Fluids have a definite shape and resist shear stress.

B.

Fluids have no definite shape and offer little resistance to shear stress.

C.

Fluids are highly compressible and have a fixed volume.

D.

Fluids cannot flow and have a fixed shape.
Correct Answer: B

Solution:

Fluids, unlike solids, do not have a definite shape and offer very little resistance to shear stress, allowing them to flow.

A.

300 N

B.

900 N

C.

1200 N

D.

1500 N
Correct Answer: B

Solution:

According to Pascal's law, the pressure applied to the small piston is transmitted undiminished to the larger piston. The force on the larger piston is given by F2=F1×A2A1F_2 = F_1 \times \frac{A_2}{A_1}, where A1=π(0.05)2A_1 = \pi (0.05)^2 and A2=π(0.15)2A_2 = \pi (0.15)^2. Thus, F2=100×0.1520.052=900 NF_2 = 100 \times \frac{0.15^2}{0.05^2} = 900 \text{ N}.

A.

18,000 N

B.

6,000 N

C.

54,000 N

D.

12,000 N
Correct Answer: C

Solution:

According to Pascal's law, the pressure applied on the small piston is transmitted undiminished to the larger piston. The force exerted on the larger piston can be calculated using the formula: F2=P×A2F_2 = P \times A_2 where A2=π(0.3)2A_2 = \pi (0.3)^2 and P=2.0×103P = 2.0 \times 10^3 N/m². Therefore, F2=2.0×103×π×(0.3)2=54,000F_2 = 2.0 \times 10^3 \times \pi \times (0.3)^2 = 54,000 N.

A.

Pressure is higher at the bottom of the fluid.

B.

Pressure is the same at all points at the same height.

C.

Pressure decreases with depth.

D.

Pressure is only exerted on solid surfaces.
Correct Answer: B

Solution:

Pascal's law states that pressure in a fluid at rest is the same at all points which are at the same height.

A.

1.5 m/s

B.

3 m/s

C.

6 m/s

D.

9 m/s
Correct Answer: C

Solution:

According to the equation of continuity for incompressible fluids, A1v1=A2v2A_1v_1 = A_2v_2. Given A1=0.02 m2A_1 = 0.02 \text{ m}^2, v1=3 m/sv_1 = 3 \text{ m/s}, and A2=0.01 m2A_2 = 0.01 \text{ m}^2, we find v2=A1v1A2=0.02×30.01=6 m/sv_2 = \frac{A_1v_1}{A_2} = \frac{0.02 \times 3}{0.01} = 6 \text{ m/s}.

A.

It increases.

B.

It decreases.

C.

It remains constant.

D.

It fluctuates randomly.
Correct Answer: B

Solution:

As temperature rises, the atoms of the liquid become more mobile, and the coefficient of viscosity decreases.

A.

Bar

B.

Pascal

C.

Torr

D.

Atmosphere
Correct Answer: B

Solution:

The unit of pressure in the International System of Units (SI) is the pascal (Pa), which is equivalent to N m⁻².

A.

4 m/s

B.

8 m/s

C.

16 m/s

D.

32 m/s
Correct Answer: B

Solution:

Using the principle of conservation of mass for incompressible fluids, the flow rate must be constant: A1v1=A2v2A_1 v_1 = A_2 v_2. Given A1=π(0.1/2)2A_1 = \pi (0.1/2)^2 and A2=π(0.05/2)2A_2 = \pi (0.05/2)^2, we find v2=v1A1A2=2×(0.1/2)2(0.05/2)2=8 m/sv_2 = v_1 \frac{A_1}{A_2} = 2 \times \frac{(0.1/2)^2}{(0.05/2)^2} = 8 \text{ m/s}.

A.

1225 N

B.

2450 N

C.

490 N

D.

980 N
Correct Answer: C

Solution:

Using Pascal's law, the pressure applied on the small piston is equal to the pressure on the large piston. Therefore, F1/A1=F2/A2F_1/A_1 = F_2/A_2, where F2=2000×9.8F_2 = 2000 \times 9.8 N. Solving for F1F_1, we get F1=F2×(A1/A2)=2000×9.8×(π×0.052)/(π×0.22)=490 NF_1 = F_2 \times (A_1/A_2) = 2000 \times 9.8 \times (\pi \times 0.05^2)/(\pi \times 0.2^2) = 490 \text{ N}.

A.

The velocity of the fluid at the hole is independent of the height of the fluid column.

B.

The pressure at the hole is equal to atmospheric pressure.

C.

The velocity of the fluid at the hole increases with the height of the fluid column.

D.

The pressure at the hole is greater than atmospheric pressure.
Correct Answer: B

Solution:

According to Bernoulli's principle, the pressure at the hole is equal to atmospheric pressure because the fluid is exposed to the atmosphere as it exits the container. The velocity of the fluid at the hole is related to the height of the fluid column, but the pressure is atmospheric.

A.

Fluids can flow and have no definite shape.

B.

Fluids are always compressible.

C.

Fluids have a fixed shape and volume.

D.

Fluids cannot exert pressure.
Correct Answer: A

Solution:

Fluids, which include liquids and gases, can flow and do not have a definite shape of their own.

A.

The velocity of fluid particles varies randomly at a given point.

B.

The velocity of fluid particles remains constant over time at a given point.

C.

The velocity of fluid particles is always zero at a given point.

D.

The velocity of fluid particles increases exponentially at a given point.
Correct Answer: B

Solution:

In a streamline flow, the velocity of each passing fluid particle remains constant in time at any given point.

A.

8000 Pa

B.

4000 Pa

C.

2000 Pa

D.

500 Pa
Correct Answer: A

Solution:

Using the continuity equation and Bernoulli's principle, the velocity at the second section is doubled due to the halved diameter. Thus, v2=6v_2 = 6 m/s. Applying Bernoulli's equation: P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2. Solving for P2P_2: P2=2000+12×1000×(3262)=8000P_2 = 2000 + \frac{1}{2} \times 1000 \times (3^2 - 6^2) = 8000 Pa.

A.

500 Pa

B.

1000 Pa

C.

1500 Pa

D.

2000 Pa
Correct Answer: A

Solution:

Using Bernoulli's principle, P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2. Solving for P2P_2, we get P2=2000+12ρ(3262)P_2 = 2000 + \frac{1}{2} \rho (3^2 - 6^2). Assuming ρ=1000 kg/m3\rho = 1000 \text{ kg/m}^3, P2=2000+0.5×1000×(936)=500 PaP_2 = 2000 + 0.5 \times 1000 \times (9 - 36) = 500 \text{ Pa}.

A.

1500 N

B.

4500 N

C.

5000 N

D.

3000 N
Correct Answer: B

Solution:

According to Pascal's law, the pressure applied to a confined fluid is transmitted undiminished throughout the fluid. Therefore, F₁/A₁ = F₂/A₂. The area of the small piston is A₁ = π(0.1)² and the area of the large piston is A₂ = π(0.3)². Solving for F₂ gives F₂ = F₁(A₂/A₁) = 500 N (π(0.3)²/π(0.1)²) = 4500 N.

A.

0.012 N

B.

0.025 N

C.

0.015 N

D.

0.018 N
Correct Answer: C

Solution:

Stokes' law for viscous drag force is given by: F=6πηavF = 6 \pi \eta a v. Substituting the given values: F=6×π×0.1×0.02×0.5=0.015 NF = 6 \times \pi \times 0.1 \times 0.02 \times 0.5 = 0.015 \text{ N}.

A.

10 m/s

B.

8 m/s

C.

12 m/s

D.

6 m/s
Correct Answer: A

Solution:

According to the principle of continuity for incompressible flow, the product of cross-sectional area and velocity at any two points in the flow must be constant. Therefore, A₁v₁ = A₂v₂. Substituting the given values: (0.05 m²)(4 m/s) = (0.02 m²)(v₂). Solving for v₂ gives v₂ = 10 m/s.

A.

It remains constant at all points in space.

B.

It varies randomly at different points.

C.

It remains constant at a given point over time.

D.

It is always zero.
Correct Answer: C

Solution:

In a streamline flow, the velocity of each passing fluid particle remains constant in time at any given point.

A.

-0.58 cm

B.

0.58 cm

C.

-1.16 cm

D.

1.16 cm
Correct Answer: A

Solution:

The height of capillary rise or fall is given by the formula: h=2Scosθρgrh = \frac{2S \cos \theta}{\rho g r}. Substituting the given values: h=2×0.485×cos(140°)13,600×9.8×0.00025h = \frac{2 \times 0.485 \times \cos(140°)}{13,600 \times 9.8 \times 0.00025}. Calculating the cosine of 140° gives a negative value, indicating a fall: h=0.0058h = -0.0058 m or -0.58 cm.

A.

1 m/s

B.

2 m/s

C.

4 m/s

D.

8 m/s
Correct Answer: D

Solution:

According to the equation of continuity for incompressible flow, A1v1=A2v2A_1v_1 = A_2v_2. Given that the diameters are 0.04 m and 0.02 m, the areas are proportional to the square of the diameters. Therefore, v2=v1×(d1d2)2=2×(0.040.02)2=8 m/sv_2 = v_1 \times \left(\frac{d_1}{d_2}\right)^2 = 2 \times \left(\frac{0.04}{0.02}\right)^2 = 8 \text{ m/s}.

A.

2.94 cm

B.

3.92 cm

C.

4.80 cm

D.

5.88 cm
Correct Answer: A

Solution:

The height of capillary rise is given by h=2Scosθρgrh = \frac{2S \cos \theta}{\rho g r}. Substituting the given values, h=2×0.072×cos01000×9.8×0.0005=2.94 cmh = \frac{2 \times 0.072 \times \cos 0}{1000 \times 9.8 \times 0.0005} = 2.94 \text{ cm}.

A.

5000 N

B.

1000 N

C.

500 N

D.

2000 N
Correct Answer: A

Solution:

According to Pascal's law, the pressure is the same on both pistons: F1A1=F2A2\frac{F_1}{A_1} = \frac{F_2}{A_2}. Given F1=200 NF_1 = 200 \ N, A1=0.02 m2A_1 = 0.02 \ m^2, and A2=0.5 m2A_2 = 0.5 \ m^2, we solve for F2F_2: F2=F1×A2A1=200×0.50.02=5000 NF_2 = \frac{F_1 \times A_2}{A_1} = \frac{200 \times 0.5}{0.02} = 5000 \ N.

A.

A force per unit volume acting within the fluid.

B.

A force per unit length acting in the plane of the interface between the liquid and the bounding surface.

C.

A force per unit area acting perpendicular to the surface.

D.

A force that acts only in gases.
Correct Answer: B

Solution:

Surface tension is a force per unit length (or surface energy per unit area) acting in the plane of the interface between the liquid and the bounding surface.

A.

1:3

B.

1:9

C.

3:1

D.

9:1
Correct Answer: D

Solution:

The force exerted by the large piston is proportional to the square of the radius ratio, so the ratio is (15/5)2=9:1(15/5)^2 = 9:1.

A.

Liquids are generally incompressible.

B.

Gases are less compressible than liquids.

C.

Solids are more compressible than gases.

D.

All fluids have the same compressibility.
Correct Answer: A

Solution:

Liquids are considered to be incompressible because their volume does not change significantly with pressure.

A.

The pressure inside the bubble increases.

B.

The pressure inside the bubble decreases.

C.

The pressure inside the bubble remains constant.

D.

The pressure inside the bubble becomes zero.
Correct Answer: B

Solution:

As a bubble rises, the pressure due to the liquid column above it decreases, leading to a decrease in pressure inside the bubble.

A.

750 Pa

B.

1500 Pa

C.

3000 Pa

D.

500 Pa
Correct Answer: A

Solution:

Using Bernoulli's principle, P1+12ρv12=P2+12ρv22P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2. Assuming ρ=1000 kg/m3\rho = 1000 \text{ kg/m}^3, P2=P1+12ρ(v12v22)=1500+12×1000×(2242)=750 PaP_2 = P_1 + \frac{1}{2} \rho (v_1^2 - v_2^2) = 1500 + \frac{1}{2} \times 1000 \times (2^2 - 4^2) = 750 \text{ Pa}.

A.

1 N m²

B.

1 N m⁻²

C.

1 N

D.

1 N m
Correct Answer: B

Solution:

The unit of pressure, pascal (Pa), is defined as 1 N m⁻².

A.

Pascal's Law

B.

Archimedes' Principle

C.

Bernoulli's Principle

D.

Newton's Third Law
Correct Answer: C

Solution:

Bernoulli's principle states that as we move along a streamline, the sum of the pressure, kinetic energy per unit volume, and potential energy per unit volume remains constant. This principle is used to explain the lift force on an airplane wing.

A.

1.5 m/s

B.

3 m/s

C.

6 m/s

D.

9 m/s
Correct Answer: C

Solution:

According to the equation of continuity for incompressible fluids, A1v1=A2v2A_1 v_1 = A_2 v_2. Given A1=0.02 m2A_1 = 0.02 \text{ m}^2, v1=3 m/sv_1 = 3 \text{ m/s}, A2=0.01 m2A_2 = 0.01 \text{ m}^2, solve for v2v_2: v2=A1v1A2=0.02×30.01=6 m/sv_2 = \frac{A_1 v_1}{A_2} = \frac{0.02 \times 3}{0.01} = 6 \text{ m/s}.

True or False

Correct Answer: False

Solution:

In a steady flow, the velocity of a fluid particle at any given point remains constant over time.

Correct Answer: True

Solution:

Surface tension is caused by the higher potential energy of molecules at the surface, which is not balanced by neighboring molecules as it is in the interior.

Correct Answer: False

Solution:

Bernoulli's principle does not hold perfectly in the presence of viscous drag. The principle is an approximation that assumes no viscosity, which is not true for real fluids.

Correct Answer: True

Solution:

As the temperature rises, the atoms of the liquid become more mobile, and the coefficient of viscosity decreases.

Correct Answer: False

Solution:

Surface tension is a scalar quantity, defined as force per unit length or energy per unit area acting at the interface between a liquid and another phase.

Correct Answer: False

Solution:

In a steady flow, streamlines cannot intersect because it would imply that a fluid particle has two different velocities at the same point.

Correct Answer: False

Solution:

The excess pressure inside a bubble of gas in a liquid is given by 2S/r. The formula 4S/r applies to a bubble of liquid in a gas.

Correct Answer: True

Solution:

This expression shows how pressure increases with depth in a fluid due to the weight of the fluid above.

Correct Answer: True

Solution:

As the temperature rises, the atoms of the liquid become more mobile, reducing the coefficient of viscosity.

Correct Answer: False

Solution:

Surface tension arises due to the excess potential energy of molecules at the interface between a fluid and another substance, not just between two fluids.

Correct Answer: True

Solution:

According to Pascal's law, the pressure in a fluid at rest is the same at all points which are at the same height.

Correct Answer: False

Solution:

Fluids, which include liquids and gases, do not have a definite shape. Liquids have a fixed volume, while gases fill the entire volume of their container.

Correct Answer: True

Solution:

Surface tension is indeed a force per unit length (or surface energy per unit area) acting at the interface between the liquid and the bounding surface.

Correct Answer: False

Solution:

According to Pascal's law, the pressure in a fluid at rest is the same at all points that are at the same height.

Correct Answer: False

Solution:

Bernoulli's principle does not hold in the presence of viscous drag on the fluid. The work done by this dissipative viscous force must be taken into account.

Correct Answer: True

Solution:

With an increase in temperature, the atoms in a liquid become more mobile, leading to a decrease in the coefficient of viscosity.

Correct Answer: False

Solution:

As temperature rises, the viscosity of a liquid typically decreases because the molecules become more mobile.

Correct Answer: False

Solution:

Bernoulli's principle applies to ideal fluid motion without viscous drag. In the presence of viscosity, the dissipative forces must be considered, which affects the pressure and energy conservation described by Bernoulli's equation.

Correct Answer: False

Solution:

Fluids do not have a definite shape of their own. They take the shape of their container.

Correct Answer: True

Solution:

This expression represents how pressure in a fluid increases with depth due to the weight of the fluid above.

Correct Answer: True

Solution:

A streamline is defined as a curve whose tangent at any point is in the direction of the fluid velocity at that point in a steady flow.

Correct Answer: True

Solution:

The coefficient of viscosity is defined as the ratio of shear stress to the time rate of shearing strain.

Correct Answer: False

Solution:

Unlike solids, liquids do not have a definite shape. They take the shape of their container.

Correct Answer: True

Solution:

This is a consequence of the continuity equation, which states that the product of cross-sectional area and velocity is constant for incompressible fluid flow.

Correct Answer: True

Solution:

Fluids, unlike solids, change shape easily under shear stress because their resistance to shear stress is about a million times smaller than that of solids.

Correct Answer: True

Solution:

The capillary rise is indeed due to surface tension and is inversely proportional to the radius of the tube, meaning it is larger for smaller radii.

Correct Answer: True

Solution:

As temperature rises, the atoms in a liquid become more mobile, reducing the coefficient of viscosity.

Correct Answer: True

Solution:

The pascal (Pa) is the SI unit of pressure and is equivalent to one newton per square meter (N m⁻²).

Correct Answer: False

Solution:

In a steady flow, streamlines do not intersect because each point in the fluid has a unique velocity.

Correct Answer: True

Solution:

In steady flow, the velocity of fluid particles at any given point does not change with time, although it may vary from point to point in space.

Correct Answer: True

Solution:

The pressure in a fluid varies with depth according to the expression P=Pa+ρghP = P_a + \rho gh, where ρ\rho is the density of the fluid.

Correct Answer: False

Solution:

Surface tension arises due to the excess potential energy of molecules at the interface between two substances, at least one of which is a fluid. It is not a property of a single fluid alone.

Correct Answer: False

Solution:

In a steady flow, the velocity of a fluid particle remains constant at a given point over time, but it can vary from one point in space to another.

Correct Answer: False

Solution:

In a steady flow, streamlines do not intersect. If they did, it would imply that a fluid particle at the intersection would have two different velocities, which is impossible.

Correct Answer: True

Solution:

According to Pascal's law, the pressure in a fluid at rest is the same at all points which are at the same height.

Correct Answer: True

Solution:

Surface tension arises because molecules at the surface have higher potential energy than those in the interior, due to the imbalance of intermolecular forces.

Correct Answer: False

Solution:

Fluids, unlike solids, do not have a definite shape of their own. They take the shape of their container.

Correct Answer: False

Solution:

In streamline flow, the velocity of fluid particles at a given point remains constant over time, but the velocity can vary at different points in space. Streamlines indicate the path of fluid particles, and while the flow is steady, it doesn't mean the velocity is uniform across different spatial locations.

Correct Answer: True

Solution:

In a steady flow, the velocity of a fluid particle may change as it moves from one point to another, but at any given point, the velocity remains constant over time.

Correct Answer: True

Solution:

The pressure difference is given by the formula ΔP=2Sr\Delta P = \frac{2S}{r}, where SS is the surface tension and rr is the radius of the tube.

Correct Answer: True

Solution:

The unit of pressure, pascal (Pa), is indeed equivalent to N m⁻².

Correct Answer: True

Solution:

The pressure inside a bubble is higher than the atmospheric pressure due to the surface tension of the liquid, which creates an excess pressure inside the bubble.

Correct Answer: True

Solution:

Fluids can flow and do not have a fixed shape, unlike solids. This property allows them to conform to the shape of their container.

Correct Answer: True

Solution:

Viscosity is a measure of a fluid's resistance to deformation at a given rate, such as when it is sheared or stretched.

Correct Answer: True

Solution:

The continuity equation for incompressible fluids states that the product of the cross-sectional area and velocity is constant along a streamline, ensuring the same volume flow rate at any point in the pipe.

Correct Answer: False

Solution:

The unit of pressure is the pascal (Pa), which is equivalent to N/m², whereas the unit of force is the newton (N).

Correct Answer: True

Solution:

Bernoulli's principle is an application of the conservation of energy to fluid motion, stating that P+12ρv2+ρgh=constantP + \frac{1}{2} \rho v^2 + \rho gh = \text{constant} along a streamline.

Correct Answer: True

Solution:

Fluids, unlike solids, can easily change shape when subjected to shear stress. The shearing stress of fluids is about a million times smaller than that of solids, indicating their low resistance to shear stress.

Correct Answer: True

Solution:

Bernoulli's principle is about the conservation of energy in a fluid flow, stating that the sum of pressure, kinetic energy per unit volume, and potential energy per unit volume remains constant along a streamline.

Correct Answer: False

Solution:

Surface tension arises due to the excess potential energy of molecules at the interface between two substances, at least one of which is a fluid.

Correct Answer: True

Solution:

The pressure difference across a liquid surface in a capillary tube is indeed due to surface tension, which causes the capillary rise or depression depending on the contact angle.

Correct Answer: True

Solution:

Water is often considered incompressible because its volume does not change significantly under pressure.

Correct Answer: False

Solution:

The pressure inside a capillary tube at the liquid surface is lower than the atmospheric pressure due to the capillary rise caused by surface tension.

Correct Answer: True

Solution:

Fluids, unlike solids, offer very little resistance to shear stress, which allows them to flow. This is a fundamental property that distinguishes fluids from solids.