Mechanical Properties of Fluids
Class 11 Physics · Physics Part II · Chapter 2
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View allCBSE Class 11 · Physics
Ch 8–14 formulas and table values, by page- Marks booster + cheatsheet: key concepts in 2 lines each, common traps
- 20-mark block: Ch 8–12
- 10-mark block: Oscillations and Waves
- Common traps, corrected
- 7 chapters: every solved-example result
- Sound, standing waves and beats covered
CBSE Class 11 · Physics
Every formula of Ch 1–7, with page numbers- Marks booster + cheatsheet: key concepts in 2 lines each, common traps
- 23-mark block: Ch 1–4
- 17-mark block: Ch 5–7
- Common traps, corrected
- 7 chapters: every solved-example result
- Every unit and dimension, listed
Summary
Liquids and gases are fluids because they flow and offer very little resistance to shear stress. Pressure is the normal force per unit area; in a fluid at rest it acts equally in all directions (a scalar) and increases with depth as \(P=P_0+\rho gh\). Pascal's law states that a pressure applied to an enclosed fluid is transmitted undiminished to every point, the basis of the hydraulic lift and brakes. Atmospheric pressure is measured by a barometer. For an ideal fluid in steady streamline flow the equation of continuity, \(Av=\) constant, expresses conservation of mass, and Bernoulli's principle, \(P+\tfrac12\rho v^{2}+\rho gh=\) constant, expresses conservation of energy, explaining the lift on an aerofoil and the working of a venturimeter. Real fluids have viscosity, an internal friction described by the coefficient \(\eta\); Stokes' law gives the viscous drag on a sphere and leads to terminal velocity. Flow is laminar below a critical Reynolds number and turbulent above it. Surface tension arises from intermolecular attraction at a liquid surface, giving rise to excess pressure inside drops and bubbles, capillary rise, and angle of contact, with surface energy equal to surface tension times area.






