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Lesson 1 – Density, Liquid Pressure and Pascal Principle

Physics

Lesson 1 – Density, Liquid Pressure and Pascal Principle

Overview

Overview

🎯 Learning outcomes

  • Define density and specific gravity (relative density) with standard SI dimensions and temperature dependence.
  • Formulate the conservation of mass and volume in non-contracting liquid mixtures.
  • Derive the fundamental hydrostatic equation for pressure at depth P = Pa + ρgh.
  • Analyze U-tube manometers, connecting vessels, and mercury Torricellian barometers.
  • Measure arterial blood pressure (systolic vs. diastolic) and evaluate clinical anomalies.
  • State Pascal’s Principle and deduce hydraulic press mechanical advantage, displacement ratios, and work efficiency.

🌳 Concept tree

  1. Lesson 1 – Density
  2. Liquid Pressure and Pascal Principle

├── Key terms

├── Laws and key relationships

  • ├── Intensive Physics of Density and Non-Contracting Fluid Mixtures
  • ├── Liquid Pressure at Depth and Manometric Measuring Instruments

├── Pascal's Principle and Hydraulic Systems

├── Worked examples

├── Exam tips

└── Real-world applications

Lesson 1 – Density, Liquid Pressure and Pascal Principle · 1 / 13
Key terms

Key terms

Comparison aspectMain ideaKeywords
Density (ρ)The mass per unit volume of a homogeneous substance at a given temperature and pressure: ρ = m / V (in kg/m3 or g/cm3). It is an intensive physical property independent of sample sizemassunitvolumehomogeneous
Relative Density (Specific Gravity)The dimensionless ratio of the density of a substance to the density of pure distilled water at 4°C: Relative Density = ρsubstance / ρwater = msubstance / mwater (for equal volumes).dimensionlessratiosubstancepure
Hydrostatic Liquid PressureThe perpendicular normal force exerted by a static liquid column on a unit horizontal surface area containing a specified point at depth h: P = ρghperpendicularnormalforceexerted
Gauge Pressure (Pgauge)The difference between absolute fluid pressure and ambient atmospheric pressure: Pgauge = Pabsolute – Patm = ρgh.differencebetweenabsolutefluid
Pascal’s Principle
  • When external pressure is applied to an enclosed
  • incompressible static fluid
  • that pressure is transmitted undiminished throughout every portion of the fluid and perpendicularly to the walls of its containing vessel
externalpressureappliedenclosed
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 2 / 13
Laws and key relationships

Laws and key relationships

Comparison aspectMain ideaKeywords
Hydrostatic Depth Pressure Law[ Formula: P = Pa + ρgh ] Absolute pressure inside an open liquid container increases linearly with depth h, fluid density ρ, and gravitational acceleration g.FormulaAbsoluteinsideopen
Equilibrium of Immiscible Liquids in a U-Tube
  • [ Formula: ρ1 · h1 = ρ2 · h2 ] At static equilibrium
  • pressure at points on the same horizontal level inside the same continuous homogeneous fluid must be equal
Formulastaticpressurepoints
Hydraulic Press Mechanical Advantage (η)[ Formula: η = F / f = A / a = R2 / r2 = y1 / y2 = v1 / v2 ] Force amplification ratio equals the piston area ratio and the inverse ratio of piston displacements. Work input equals work output in an ideal 100% efficient pressFormulaForceamplificationratio
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 3 / 13
Intensive Physics of Density and Non-Contracting Fluid Mixtures

Intensive Physics of Density and Non-Contracting Fluid Mixtures

  • Density (symbol ρ, Greek letter rho) is a fundamental intensive physical property of all states of matter, defined as the mass contained within a unit volume: ρ = m / V.
  • In the International System of Units (SI), density is expressed in kilograms per cubic meter (kg/m3), where 1 g/cm3 = 1,000 kg/m3.
  • Density depends strictly on two microscopic variables: (1) The atomic or molecular mass of the constituent elements, and (2) The intermolecular spacing between molecules, which is directly governed by ambient temperature and pressure.
  • Relative Density (Specific Gravity) is a dimensionless quantity comparing the density of any substance to that of pure water at its maximum density temperature of 4°C (1,000 kg/m3): Relative Density = ρsubstance / 1,000.
  • Because it is a ratio of identical physical dimensions, it has no units.
  • Multiplying relative density by 1,000 instantly yields the absolute density in kg/m3.
Fluid Mixtures→When two miscible liquids of volumes V1 and V2 and densities ρ1 and ρ2 are blended without chemical reaction or intermolecular contraction, total mass is conserved: mmix = m1 + m2, which yields: ρmix × Vmix = (ρ1 × V1) + (ρ2 × V2). If volume contraction occurs due to intermolecular dissolution (e.g., ethanol and water), Vmix < V1 + V2, causing the mixture density to exceed the theoretical arithmetic weighted mean.
Comparison aspectMain ideaKeywords
Clinical & Industrial Diagnostics
  • (a) Medical diagnosis of anemia: Healthy adult blood density ranges strictly between 1
  • 040 and 1
  • 060 kg/m3
MedicaldiagnosisanemiaHealthy
•
  • A drop below 1
  • 040 kg/m3 signifies anemia (deficiency of hemoglobin and erythrocytes)
dropbelowsignifiesanemia
(b) Urine density diagnostics
  • Normal urine density is approximately 1
  • 020 kg/m3
  • elevation above normal indicates hyper-concentration of excreted metabolic salts
Normalapproximatelyelevationabove
(c) Lead-acid automobile batteriesA hydrometer measures the density of electrolyte sulfuric acidhydrometermeasuresdensityelectrolyte
•
  • In a fully charged battery
  • sulfuric acid density is 1.28–1.30 g/cm3
  • discharge consumes acid into water and lead sulfate
  • dropping density below 1.20 g/cm3
fullychargedbatterysulfuric
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 4 / 13
Liquid Pressure at Depth and Manometric Measuring Instruments

Liquid Pressure at Depth and Manometric Measuring Instruments

  • Pressure at a point inside a static liquid is physically defined as the normal compressive weight of the liquid column resting above that point per unit cross-sectional area: P = F / A = (m × g) / A = (ρ × V × g) / A = (ρ × A × h × g) / A = ρgh.
  • When the liquid vessel is exposed to ambient atmospheric air, total absolute pressure is: P = Patm + ρgh.
  • The gauge pressure is simply: Pgauge = P – Patm = ρgh.
Comparison aspectMain ideaKeywords
Characteristics of Hydrostatic Pressure(1) Liquid pressure at a given depth acts uniformly in all spatial directions (omnidirectional)Liquidgivendepthacts
•
  • (2) In connected vessels of varying geometric shapes
  • the liquid levels in all branches stabilize at the exact same horizontal height regardless of vessel geometry or cross-sectional area
  • because pressure depends solely on vertical depth h
  • not base surface area or liquid volume
connectedvesselsvaryinggeometric
The U-Tube Manometer
  • A U-shaped glass tube partially filled with liquid. When two immiscible liquids (e.g
  • water and oil) are poured into opposite arms
  • at equilibrium
  • the pressure at the separating interface level must balance: P1 = P2 → Patm + ρ1·g·h1 = Patm + ρ2·g·h2 → ρ1·h1 = ρ2·h2. The column heights above the common interface are inversely proportional to their respective densities
shapedglasspartiallyfilled
Comparison aspectMain ideaKeywords
Torricellian Mercury Barometer
  • Evangelista Torricelli balanced atmospheric air weight against a dense mercury column. At sea level and 0°C
  • atmospheric pressure balances exactly 76 cm of mercury (0.76 mHg). The vacuum above the mercury column is known as Torricellian Vacuum
  • containing only trace mercury vapor. Standard atmospheric pressure: Patm = ρHg × g × h = 13
  • 600 kg/m3 × 9.8 m/s2 × 0.76 m = 1.013 × 105 N/m2 (Pascals) = 1.013 bar = 760 Torr (mmHg)
Evangelistabalancedatmosphericweight
Sphygmomanometer Blood Pressure Dynamics
  • Arterial pressure cycles between Systolic Pressure (~120 mmHg
  • maximum pressure during left ventricular systole when aortic valves open) and Diastolic Pressure (~80 mmHg
  • minimum resting pressure during ventricular diastole)
ArterialcyclesbetweenSystolic
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 5 / 13
Pascal’s Principle and Hydraulic Systems

Pascal’s Principle and Hydraulic Systems

  • Pascal’s Principle applies strictly to incompressible fluids (liquids), stating that: Any pressure applied to an enclosed static fluid is transmitted without diminution to every portion of the fluid and to container walls.
  • Gases are highly compressible due to enormous intermolecular voids; hence, applied work compresses the gas volume rather than transmitting pressure instantaneously.
  • The Hydraulic Press Architecture Consists of two communicating cylinders fitted with leak-proof movable pistons of unequal areas: a small piston of cross-sectional area a (radius r) and a large piston of area A (radius R). When a small input force f is exerted downwards on the small piston, it creates pressure: P = f / a. This pressure transmits across the fluid to act upwards beneath the large piston: P = F / A. Equating pressures yields: F / A = f / a, or: F = f × (A / a).
Comparison aspectMain ideaKeywords
Mechanical Advantage (η)
  • Because A > a
  • the output force F is multiplied by the area ratio: η = F / f = A / a = R2 / r2 = D2 / d2 = y1 / y2 = v1 / v2
  • where y1 is the downward displacement of the small piston
  • y2 is the upward displacement of the large piston
  • v1 is the small piston velocity
  • and v2 is the large piston velocity
Becauseoutputforcemultiplied
Conservation of Energy & Efficiency
  • Force is multiplied
  • but work is NEVER created. In an ideal press without friction: Work Output = Work Input (F × y2 = f × y1). In real-world hydraulic machinery
  • hydraulic fluid viscosity
  • fluid turbulence
  • and seal friction dissipate energy: Efficiency = (Work Output / Work Input) × 100% = [(F × y2) / (f × y1)] × 100% < 100%
ForcemultipliedworkNEVER
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 6 / 13
Worked examples

Worked examples

✍️ Worked examples→Barometric Mountain Height Calculation
Comparison aspectMain ideaKeywords
Problem StatementA Torricellian mercury barometer reads 76 cmHg at the base of a mountain and 70.8 cmHg at its summitTorricellianmercurybarometerreads
•
  • If the average density of atmospheric air over this altitude is 1.25 kg/m3 and the density of mercury is 13
  • 600 kg/m3
  • calculate the absolute height of the mountain
averagedensityatmosphericover
Detailed Solution & Derivation
  • Step 1: The drop in barometric pressure between ground and summit equals the weight of the air column spanning the mountain height: ΔPHg = ΔPair. Step 2: ρHg × g × (hground – hsummit) = ρair × g × Hmountain. Step 3: Cancel g from both sides: ρHg × ΔhHg = ρair × Hmountain. Step 4: Convert Δh to meters: Δh = 76 cm – 70.8 cm = 5.2 cm = 0.052 m. Step 5: Substitute numerical values: 13
  • 600 kg/m3 × 0.052 m = 1.25 kg/m3 × Hmountain. 707.2 = 1.25 × Hmountain → Hmountain = 707.2 / 1.25 = 565.76 meters
Stepdropbarometricpressure

✍️ Worked examples

Comparison aspectMain ideaKeywords
Worked Example 2Hydraulic Press Force and Displacement DynamicsHydraulicPressForceDisplacement
Problem Statement
  • A hydraulic press has a small piston of radius 2 cm and a large piston of radius 20 cm. If an input force of 50 N is applied to the small piston: (1) Find the mechanical advantage of the press
  • (2) Determine the maximum load mass the large piston can lift (g = 10 m/s2)
  • (3) If the small piston moves downwards by 10 cm
  • how far does the large piston rise?
hydraulicpresssmallpiston
Detailed Solution & Derivation
  • Step 1: Mechanical Advantage η = A / a = R2 / r2 = (20 cm)2 / (2 cm)2 = 400 / 4 = 100. Step 2: Output force F = η × f = 100 × 50 N = 5
  • 000 N. Maximum lifted mass M = F / g = 5
  • 000 N / 10 m/s2 = 500 kg. Step 3: Displacement ratio: η = y1 / y2 → 100 = 10 cm / y2 → y2 = 10 cm / 100 = 0.1 cm (1 mm)
StepMechanicalAdvantageOutput
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 7 / 13
Exam tips

Exam tips

Comparison aspectMain ideaKeywords
Exam Trap
  • In a Torricellian barometer
  • tilting the tube changes the slanted length of the mercury thread
  • but the VERTICAL perpendicular height h remains strictly 76 cmHg at standard sea level atmospheric pressure
Torricellianbarometertiltingtube
Crucial Rule
  • When air bubbles enter a hydraulic press cylinder
  • the system efficiency crashes drastically because applied mechanical work is wasted on compressing the air bubbles rather than transmitting pressure to the large piston
bubblesenterhydraulicpress
•
  • Pressure at the bottom of a container depends exclusively on vertical liquid height h
  • NOT on total liquid volume or the shape of the container walls
Pressurebottomcontainerdepends
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 8 / 13
Real-world applications

Real-world applications

Comparison aspectMain ideaKeywords
Automotive Hydraulic Disc Brakes
  • Stepping on the brake pedal exerts pressure on hydraulic master cylinders
  • transmitting equal fluid pressure instantly to all four caliper pistons to clamp rotating brake discs
Steppingpedalexertspressure
Deep-Sea Submersible Engineering
  • Submarine hulls must be engineered with reinforced spherical titanium alloys to withstand extreme hydrostatic crushing pressures (P = ρgh exceeds 1
  • 000 atmospheres in deep ocean trenches)
Submarinehullsmustengineered
Aircraft AltimetersAneroid barometers calibrated to altitude indicate flight elevation based on the known exponential decay of atmospheric pressure with heightAneroidbarometerscalibratedaltitude
•
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Lesson 1 – Density, Liquid Pressure and Pascal Principle · 9 / 13
Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula

Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula

💡 Core Diagrams & Reference Data→All data, reference comparison tables, and anatomical figures have been accurately digitized from official curriculum textbooks.

🔬 Figure 1 – Liquid Pressure at a Point and Depth Dependence

  1. Scientific details and precise observational breakdown:
  2. Work and
  3. Energy
  4. Chapter
  5. Lesson One:
  6. Work
  7. Lesson Two:
  8. Energy

🔬 Figure 2 – U-Tube Manometer and Barometer Setup

  • Scientific details and precise observational breakdown:

a horizontal surface. A force of magnitude 40 N

acted upon it, moving it from rest through

  1. a displacement of 4.5 m from point a to point b. If
  2. the friction force is 15 N, calculate the work done on
  3. the body by the resultant force acting on it.

Questions that measure hic

  • Choose the correct answer:
  • (1) In the opposite figure, a crane is lifting a load iW £ NN

of mass 0.5 ton with a constant velocity from

  • the ground to a height of 10 m. Given that the oT) xen?
Parameter / Element Extracted Specification & Details
Item 1 re es
Item 2 @13m ®15m ©3m @5m
Item 3 t Second | Essay Questions
Item 4 (1) Explain:
Item 5 (1) Kinetic energy is a scalar quantity.
Item 6 (2) Kinetic energy of a static body equals zero.
Item 7 (2) An object of mass 2 kg that is moving with a constant speed has a kinetic energy of 25J
Item 8 calculate:
Item 9 (1) The magnitude of its velocity.
Item 10 (2) The work done on the object by the net force.
Item 11 (3) Compare between the elastic potential energy and the gravitational potential energy (in
Item 12 terms of: definition).
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 10 / 13
Part 11

Part 11

  • 📖
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 11 / 13
📌 Comprehensive Scientific Terminology Dictionary:

📌 Comprehensive Scientific Terminology Dictionary:

  • Density (ρ):
  • The mass per unit volume of a homogeneous substance at a given temperature and pressure: ρ = m / V (in kg/m3 or g/cm3).
  • It is an intensive physical property independent of sample size.
  • Relative Density (Specific Gravity):
  • The dimensionless ratio of the density of a substance to the density of pure distilled water at 4°C: Relative Density = ρ_substance / ρ_water = msubstance / mwater (for equal volumes).
  • Hydrostatic Liquid Pressure:
  • The perpendicular normal force exerted by a static liquid column on a unit horizontal surface area containing a specified point at depth h: P = ρgh.
  • Gauge Pressure (Pgauge):
  • The difference between absolute fluid pressure and ambient atmospheric pressure: Pgauge = Pabsolute – Patm = ρgh.
  • Pascal's Principle:
  • When external pressure is applied to an enclosed, incompressible static fluid, that pressure is transmitted undiminished throughout every portion of the fluid and perpendicularly to the walls of its containing vessel.
  • ⚖️ Governing Scientific Laws, Theorems & Mathematical Models:
  • Hydrostatic Depth Pressure Law:
  • [ Formula P = Pa + ρgh ] Absolute pressure inside an open liquid container increases linearly with depth h, fluid density ρ, and gravitational acceleration g.
  • Equilibrium of Immiscible Liquids in a U:
  • Tube [ Formula: ρ1 · h1 = ρ2 · h2 ] At static equilibrium, pressure at points on the same horizontal level inside the same continuous homogeneous fluid must be equal.
  • Hydraulic Press Mechanical Advantage (η):
  • [ Formula η = F / f = A / a = R2 / r2 = y1 / y2 = v1 / v2 ] Force amplification ratio equals the piston area ratio and the inverse ratio of piston displacements. Work input equals work output in an ideal 100% efficient press.
  • 📌 Exhaustive In:
  • Depth Pedagogical Breakdown:
  • ◄ 1. Intensive Physics of Density and Non:

Contracting Fluid Mixtures

  • Density (symbol ρ, Greek letter rho) is a fundamental intensive physical property of all states of matter, defined as the mass contained within a unit volume:
  • ρ = m / V.
  • In the International System of Units (SI), density is expressed in kilograms per cubic meter (kg/m3), where 1 g/cm3 = 1,000 kg/m3.
  • Density depends strictly on two microscopic variables: (1) The atomic or molecular mass of the constituent elements, and (2) The intermolecular spacing between molecules, which is directly governed by ambient temperature and pressure.
  • Relative Density (Specific Gravity) is a dimensionless quantity comparing the density of any substance to that of pure water at its maximum density temperature of 4°C (1,000 kg/m3):
  • Relative Density = ρ_substance / 1,000.
  • Because it is a ratio of identical physical dimensions, it has no units.
  • Multiplying relative density by 1,000 instantly yields the absolute density in kg/m3.
  • Fluid Mixtures:
  • When two miscible liquids of volumes V1 and V2 and densities ρ1 and ρ2 are blended without chemical reaction or intermolecular contraction, total mass is conserved: mmix = m1 + m2, which yields: ρ_mix × Vmix = (ρ1 × V1) + (ρ2 × V2).
  • If volume contraction occurs due to intermolecular dissolution (e.g., ethanol and water), Vmix < V1 + V2, causing the mixture density to exceed the theoretical arithmetic weighted mean.
  • Clinical & Industrial Diagnostics:
  • (a) Medical diagnosis of anemia Healthy adult blood density ranges strictly between 1,040 and 1,060 kg/m3. A drop below 1,040 kg/m3 signifies anemia (deficiency of hemoglobin and erythrocytes). (b) Urine density diagnostics: Normal urine density is approximately 1,020 kg/m3; elevation above normal indicates hyper-concentration of excreted metabolic salts. (c) Lead-acid automobile batteries: A hydrometer measures the density of electrolyte sulfuric acid. In a fully charged battery, sulfuric acid density is 1.28–1.30 g/cm3; discharge consumes acid into water and lead sulfate, dropping density below 1.20 g/cm3.
  • Figure (Figure 1:
  • Liquid Pressure at a Point and Depth Dependence.png): Hydrostatic pressure dependence on fluid column depth h and liquid density rho.
  • ◄ 2. Liquid Pressure at Depth and Manometric Measuring Instruments
  • Pressure at a point inside a static liquid is physically defined as the normal compressive weight of the liquid column resting above that point per unit cross:
  • sectional area P = F / A = (m × g) / A = (ρ × V × g) / A = (ρ × A × h × g) / A = ρgh. When the liquid vessel is exposed to ambient atmospheric air, total absolute pressure is: P = Patm + ρgh. The gauge pressure is simply: Pgauge = P – Patm = ρgh.
  • Characteristics of Hydrostatic Pressure:
  • (1) Liquid pressure at a given depth acts uniformly in all spatial directions (omnidirectional). (2) In connected vessels of varying geometric shapes, the liquid levels in all branches stabilize at the exact same horizontal height regardless of vessel geometry or cross-sectional area, because pressure depends solely on vertical depth h, not base surface area or liquid volume.
  • The U:
  • Tube Manometer A U-shaped glass tube partially filled with liquid. When two immiscible liquids (e.g., water and oil) are poured into opposite arms, at equilibrium, the pressure at the separating interface level must balance: P1 = P2 → Patm + ρ1·g·h1 = Patm + ρ2·g·h2 → ρ1·h1 = ρ2·h2. The column heights above the common interface are inversely proportional to their respective densities.
  • Torricellian Mercury Barometer:
  • Evangelista Torricelli balanced atmospheric air weight against a dense mercury column.
  • At sea level and 0°C, atmospheric pressure balances exactly 76 cm of mercury (0.76 mHg).
  • The vacuum above the mercury column is known as Torricellian Vacuum, containing only trace mercury vapor.
  • Standard atmospheric pressure: Patm = ρ_Hg × g × h = 13,600 kg/m3 × 9.8 m/s2 × 0.76 m = 1.013 × 105 N/m2 (Pascals) = 1.013 bar = 760 Torr (mmHg).
  • Sphygmomanometer Blood Pressure Dynamics:
  • Arterial pressure cycles between Systolic Pressure (~120 mmHg, maximum pressure during left ventricular systole when aortic valves open) and Diastolic Pressure (~80 mmHg, minimum resting pressure during ventricular diastole).
  • Figure (Figure 2:
  • U-Tube Manometer and Barometer Setup.png): U-tube manometer with immiscible liquids at equilibrium and Torricellian mercury barometer column.

◄ 3. Pascal's Principle and Hydraulic Systems

  • Pascal's Principle applies strictly to incompressible fluids (liquids), stating that:
  • Any pressure applied to an enclosed static fluid is transmitted without diminution to every portion of the fluid and to container walls.
  • Gases are highly compressible due to enormous intermolecular voids; hence, applied work compresses the gas volume rather than transmitting pressure instantaneously.
  • The Hydraulic Press Architecture:
  • Consists of two communicating cylinders fitted with leak-proof movable pistons of unequal areas: a small piston of cross-sectional area a (radius r) and a large piston of area A (radius R).
  • When a small input force f is exerted downwards on the small piston, it creates pressure: P = f / a.
  • This pressure transmits across the fluid to act upwards beneath the large piston: P = F / A.
  • Equating pressures yields: F / A = f / a, or: F = f × (A / a).
  • Mechanical Advantage (η):
  • Because A > a, the output force F is multiplied by the area ratio: η = F / f = A / a = R2 / r2 = D2 / d2 = y1 / y2 = v1 / v2, where y1 is the downward displacement of the small piston, y2 is the upward displacement of the large piston, v1 is the small piston velocity, and v2 is the large piston velocity.
  • Conservation of Energy & Efficiency:
  • Force is multiplied, but work is NEVER created.
  • In an ideal press without friction: Work Output = Work Input (F × y2 = f × y1).
  • In real-world hydraulic machinery, hydraulic fluid viscosity, fluid turbulence, and seal friction dissipate energy: Efficiency = (Work Output / Work Input) × 100% = [(F × y2) / (f × y1)] × 100% < 100%.
  • Figure (Table 1:
  • Pascal Principle and Hydraulic Press Mechanics.png): Mechanical advantage formulas, force amplification factors, and work conservation in hydraulic systems.
  • 🧮 Exemplary Step:
  • by-Step Worked Problems & Applied Exercises:
  • Worked Example 1:

Barometric Mountain Height Calculation

  • Problem Statement:
  • A Torricellian mercury barometer reads 76 cmHg at the base of a mountain and 70.8 cmHg at its summit.
  • If the average density of atmospheric air over this altitude is 1.25 kg/m3 and the density of mercury is 13,600 kg/m3, calculate the absolute height of the mountain.
  • Detailed Solution & Derivation:
  • Step 1 The drop in barometric pressure between ground and summit equals the weight of the air column spanning the mountain height: ΔP_Hg = ΔPair. Step 2: ρ_Hg × g × (hground – hsummit) = ρ_air × g × Hmountain. Step 3: Cancel g from both sides: ρ_Hg × Δh_Hg = ρ_air × Hmountain. Step 4: Convert Δh to meters: Δh = 76 cm – 70.8 cm = 5.2 cm = 0.052 m. Step 5: Substitute numerical values: 13,600 kg/m3 × 0.052 m = 1.25 kg/m3 × Hmountain. 707.2 = 1.25 × Hmountain → Hmountain = 707.2 / 1.25 = 565.76 meters.
  • Worked Example 2:

Hydraulic Press Force and Displacement Dynamics

  • Problem Statement:
  • A hydraulic press has a small piston of radius 2 cm and a large piston of radius 20 cm.
  • If an input force of 50 N is applied to the small piston: (1) Find the mechanical advantage of the press; (2) Determine the maximum load mass the large piston can lift (g = 10 m/s2); (3) If the small piston moves downwards by 10 cm, how far does the large piston rise?
  • Detailed Solution & Derivation:
  • Step 1 Mechanical Advantage η = A / a = R2 / r2 = (20 cm)2 / (2 cm)2 = 400 / 4 = 100. Step 2: Output force F = η × f = 100 × 50 N = 5,000 N. Maximum lifted mass M = F / g = 5,000 N / 10 m/s2 = 500 kg. Step 3: Displacement ratio: η = y1 / y2 → 100 = 10 cm / y2 → y2 = 10 cm / 100 = 0.1 cm (1 mm).
  • 💡 Master Teacher Insights & Critical Exam Cautions:
  • Exam Trap:
  • In a Torricellian barometer, tilting the tube changes the slanted length of the mercury thread, but the VERTICAL perpendicular height h remains strictly 76 cmHg at standard sea level atmospheric pressure.
  • Crucial Rule:
  • When air bubbles enter a hydraulic press cylinder, the system efficiency crashes drastically because applied mechanical work is wasted on compressing the air bubbles rather than transmitting pressure to the large piston.
  • ★ Pressure at the bottom of a container depends exclusively on vertical liquid height h, NOT on total liquid volume or the shape of the container walls.
  • 🌍 Practical Real:
  • World, Industrial & Societal Connections:
  • ✔ Automotive Hydraulic Disc Brakes:
  • Stepping on the brake pedal exerts pressure on hydraulic master cylinders, transmitting equal fluid pressure instantly to all four caliper pistons to clamp rotating brake discs.
  • ✔ Deep:
  • Sea Submersible Engineering Submarine hulls must be engineered with reinforced spherical titanium alloys to withstand extreme hydrostatic crushing pressures (P = ρgh exceeds 1,000 atmospheres in deep ocean trenches).
  • ✔ Aircraft Altimeters:
  • Aneroid barometers calibrated to altitude indicate flight elevation based on the known exponential decay of atmospheric pressure with height.
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 12 / 13
🔍 In-Depth Explanations, Deductions & Multi-Book Insights:

🔍 In-Depth Explanations, Deductions & Multi-Book Insights:

  • ★ Comprehensive Study & Detailed Pedagogical Guide ★
  • Comprehensive Explanation Density, Liquid Pressure at Depth and Pascal's Principle
  • Physics (Secondary Stage – 2nd Secondary) | Grade 11 (2nd Secondary) | 2026 / 2027 Official Curriculum | Chapter 1: Fluid Mechanics & Pressure
  • 🎯 Targeted Learning Outcomes & Pedagogical Objectives:
  • • Define density and specific gravity (relative density) with standard SI dimensions and temperature dependence.
  • • Formulate the conservation of mass and volume in non-contracting liquid mixtures.
  • • Derive the fundamental hydrostatic equation for pressure at depth: P = Pa + ρgh.
  • • Analyze U-tube manometers, connecting vessels, and mercury Torricellian barometers.
  • • Measure arterial blood pressure (systolic vs. diastolic) and evaluate clinical anomalies.
  • • State Pascal's Principle and deduce hydraulic press mechanical advantage, displacement ratios, and work efficiency.
Lesson 1 – Density, Liquid Pressure and Pascal Principle · 13 / 13