🏗️ Chapter 9: Mechanical Properties of Solids (Class 11) 🔩
Hi Future Engineers & Scientists! Hum daily life mein alag-alag solid objects dekhte hain – kuch hard (like steel 🔩), kuch easily deformable (like rubber ゴム). Solid objects external forces lagne par kaise behave karte hain? Why do some regain their shape while others don’t? Let’s explore the mechanical properties of solids!
Hi Future Engineers & Scientists! Hum daily life mein alag-alag solid objects dekhte hain – kuch kathor (jaise steel), kuch aasani se deform hone wale (jaise rubber). Solid objects par bahari bal lagne par ve kaise behave karte hain? Kyun kuch apna shape wapas pa lete hain jabki kuch nahi? Chalo solids ki mechanical properties ko explore karein!📌 Elasticity and Plasticity (Pratyasthata Aur Sughatyata)
- When an external force is applied to a solid, its shape or size (or both) may change. This change is called Deformation. Jab kisi solid par bahari bal lagaya jaata hai, toh uska aakar ya size (ya dono) badal sakta hai. Is badlav ko Deformation kehte hain.
- The external force causing deformation is called the Deforming Force.
- When the deforming force is removed, bodies try to regain their original shape and size due to an internal restoring force. Jab deforming force hata diya jaata hai, toh vastu apne andar ke restoring force ke karan apni original shape aur size wapas paane ki koshish karti hai.
Elasticity: The property of a body by virtue of which it tends to regain its original size and shape after the removal of the deforming force.
Pratyasthata (Elasticity): Vastu ka vah gun jiske karan vah deforming force hatane ke baad apni original size aur shape wapas paane ki koshish karti hai.A body that completely regains its original configuration is called Perfectly Elastic.
Plasticity: The property of a body by virtue of which it does NOT regain its original size and shape even after the removal of the deforming force.
Sughatyata (Plasticity): Vastu ka vah gun jiske karan vah deforming force hatane ke baad bhi apni original size aur shape wapas NAHI paa paati hai.A body that does not regain its original configuration at all is called Perfectly Plastic.
No body is perfectly elastic or perfectly plastic; real bodies lie somewhere in between.
💪📏 Stress and Strain (Pratibal Aur Vikriti)
Stress (σ)
When a deforming force is applied, an internal restoring force develops within the body per unit area of cross-section to oppose the change.
Jab deforming force lagaya jaata hai, toh badlav ka virodh karne ke liye vastu ke andar cross-section ke prati unit area par ek internal restoring force develop hota hai.Definition: The internal restoring force set up per unit area of cross-section of the deformed body.
Formula: Stress (σ) = Restoring Force (F)Area of cross-section (A)
(In equilibrium, restoring force = applied deforming force)
- SI Unit: Newton per square metre (N/m² or Nm⁻²) or Pascal (Pa).
- Dimensional Formula: [Force]/[Area] = [MLT⁻²]/[L²] = [ML⁻¹T⁻²].
Types of Stress:
- Longitudinal Stress: Force applied perpendicular to the cross-section, causing change in length.
- Tensile Stress: If length increases (stretching ↔️).
- Compressive Stress: If length decreases (compressing ➡️⬅️).
- Volumetric (or Bulk) Stress: Force applied uniformly & perpendicularly over the entire surface, causing change in volume (like pressure 💧).
- Shear (or Tangential) Stress: Force applied parallel (tangentially) to a surface, causing change in shape (relative displacement between faces 🩸➡️).
Strain (ε)
When a deforming force acts on a body, the body undergoes a change in its dimensions.
Jab deforming force vastu par kaam karta hai, toh vastu ke dimensions mein badlav aata hai.Definition: The ratio of the change in configuration (dimension like length, volume, shape) to the original configuration.
Paribhasha: Configuration mein badlav (jaise lambai, aayatan, aakar) aur original configuration ka anupat.- It’s a ratio, so it is **dimensionless** and has **no units**.
Types of Strain:
- Longitudinal Strain: Change in length (
ΔL
) per unit original length (L
).Strain = ΔLL
. - Volumetric Strain: Change in volume (
ΔV
) per unit original volume (V
).Strain = ΔVV
. (Often negative if volume decreases). - Shear Strain: The angle (θ, in radians) through which a face originally perpendicular to the fixed face gets turned/displaced when tangential force is applied. For small angles,
tan θ ≈ θ = ΔxL
(where Δx is relative displacement, L is distance between faces).
Stress-Strain Relationship & Elastic Limit
- When stress is applied, strain is produced. The relationship depends on the material.
- Elastic Limit: The maximum stress within which the body completely regains its original shape and size after the removal of the deforming force. Beyond this limit, the body acquires a permanent set (deformation) or even fractures. ⚠️ Pratyastha Seema: Woh maximum stress jiske andar deforming force hatane par vastu poori tarah apna original shape/size wapas pa leti hai. Is limit ke paar, vastu mein permanent deformation aa jaata hai ya woh toot jaati hai.
🔗 Hooke’s Law
Hooke’s Law: Within the elastic limit, stress developed is directly proportional to the strain produced.
Pratyastha seema ke andar, utpann pratibal (stress) utpann vikriti (strain) ke seedhe anupatik (directly proportional) hota hai.Stress ∝ Strain
or
Stress = E × Strain
- Here, E is the constant of proportionality, called the Modulus of Elasticity of the material. Yahan, E anupatikta sthirank (constant of proportionality) hai, jise padarth ka Pratyasthata Gunank (Modulus of Elasticity) kehte hain.
- Modulus of Elasticity depends only on the nature of the material and temperature. It is independent of stress and strain.
- Its SI unit is the same as stress (N/m² or Pa) because strain is dimensionless.
- Dimensional Formula: [ML⁻¹T⁻²].
- Larger the value of E, the more elastic the material (means it requires more stress for the same strain, it’s stiffer). Steel is more elastic than rubber. E ki value jitni zyada hogi, material utna zyada elastic (kathhor) hoga. Steel rubber se zyada elastic hai.
Stress-Strain Curve (Qualitative Idea)
(Imagine plotting Stress on y-axis vs Strain on x-axis for a typical metal wire)
- Proportional Limit (O-A): Straight line region where Stress ∝ Strain (Hooke’s Law obeyed).
- Elastic Limit (Point B): Point up to which material regains original shape when stress removed.
- Yield Point (Point C): Stress at which material starts to deform permanently (plastic deformation begins).
- Breaking Point / Fracture Point (Point E): Stress at which the material breaks.
- Ductile Materials (like copper, steel) show a large plastic region before fracture.
- Brittle Materials (like glass, cast iron) fracture soon after the elastic limit.
🏋️ Moduli of Elasticity (Pratyasthata Gunank)
Corresponding to the three types of stress and strain, there are three main moduli of elasticity:
Teen prakaar ke stress aur strain ke corresponding, teen mukhya pratyasthata gunank hote hain:1. Young’s Modulus (Y) (Young Gunank)
Ratio of longitudinal stress to longitudinal strain within the elastic limit.
Formula:
Y = Longitudinal StressLongitudinal Strain = (F/A) (ΔL/L) = F × LA × ΔL
Unit: N/m² or Pa. Dimension: [ML⁻¹T⁻²]. Measures resistance to change in length.
Pratyastha seema ke andar longitudinal stress aur longitudinal strain ka anupat. Lambai mein badlav ke prati pratirodh maapta hai.2. Bulk Modulus (B) (Aayatan Gunank)
Ratio of volumetric stress (Pressure, P) to volumetric strain (
-ΔV/V
) within the elastic limit. Negative sign indicates volume decreases when pressure increases.Formula:
B = Volumetric StressVolumetric Strain = P (-ΔV/V) = - P × VΔV
Unit: N/m² or Pa. Dimension: [ML⁻¹T⁻²]. Measures resistance to change in volume.
Compressibility (k): Reciprocal of Bulk Modulus (
Pratyastha seema ke andar volumetric stress (Pressure, P) aur volumetric strain (-ΔV/V) ka anupat. Aayatan mein badlav ke prati pratirodh maapta hai.k = 1/B
). Measures how easily a substance can be compressed.3. Shear Modulus (or Modulus of Rigidity) (G or η) (Aparupan Gunank)
Ratio of shear stress to shear strain (θ) within the elastic limit.
Formula:
G = Shear StressShear Strain = (Ftangential / A) θ = (Ftangential / A) (Δx / L)
Unit: N/m² or Pa. Dimension: [ML⁻¹T⁻²]. Measures resistance to change in shape (rigidity). Applicable only to solids.
Pratyastha seema ke andar shear stress aur shear strain (θ) ka anupat. Aakar mein badlav ke prati pratirodh (kathorta) maapta hai. Kewal solids ke liye lagu.*(Qualitative idea: Think how hard it is to twist or deform the shape of a solid block sideways)*.
Poisson’s Ratio (σ or ν) (Payasan Anupat) – Qualitative Idea
When a wire is stretched longitudinally, its length increases (longitudinal strain) but its diameter decreases (lateral strain).
Poisson’s Ratio (σ): Within the elastic limit, the ratio of lateral strain to the longitudinal strain.
Formula: σ = Lateral StrainLongitudinal Strain = (-ΔD / D) (ΔL / L)
It’s a ratio of two strains, so it’s a dimensionless number. Typical values range from 0 to 0.5.
Jab ek taar ko lambaai mein kheenchte hain, toh uski lambai badhti hai lekin uska vyas (diameter) kam hota hai. Payasan Anupat, pratyastha seema ke andar, paarshvik vikriti (lateral strain) aur anudaidharya vikriti (longitudinal strain) ka anupat hai. Yeh dimensionless hai.Elastic Energy (Pratyastha Urja)
Elastic Potential Energy: When a body is deformed (stretched or compressed) within its elastic limit, work is done against the internal restoring forces. This work done is stored in the body as elastic potential energy.
Jab kisi vastu ko uski pratyastha seema ke andar deform kiya jaata hai, toh internal restoring forces ke viruddh kaam kiya jaata hai. Yeh kiya gaya kaam vastu mein pratyastha sthitij urja (elastic potential energy) ke roop mein store ho jaata hai.Elastic Potential Energy per unit volume (Energy Density) stored in a stretched wire:
Energy Density = 12 × Stress × Strain
= 12 × Y × (Strain)²
= 12 × (Stress)²Y
Total Elastic Energy = Energy Density × Volume
⚙️ Solved Practice Problems: Solid Properties
Problem 1: A steel wire of length 4 m and cross-section area 2×10⁻⁶ m² is stretched by 2 mm when a force of 400 N is applied. Calculate the stress and strain.
Given: L = 4 m, A = 2×10⁻⁶ m², F = 400 N, ΔL = 2 mm = 2 × 10⁻³ m.
Stress (σ):
σ = ForceArea = 400 N2 × 10⁻⁶ m²
= 200 × 10⁶ N/m² = 2 × 10⁸ N/m²
(or Pa).
Strain (ε):
ε = Change in Length (ΔL)Original Length (L) = 2 × 10⁻³ m4 m
= 0.5 × 10⁻³ = 5 × 10⁻⁴
(Dimensionless).
Answer: Stress = 2 × 10⁸ N/m², Strain = 5 × 10⁻⁴
Problem 2: Using the results from Problem 1, calculate Young’s modulus (Y) for the steel wire.
We know, Stress = 2 × 10⁸ N/m² and Strain = 5 × 10⁻⁴.
Young’s Modulus Y = Stress / Strain.
Y = 2 × 10⁸ N/m²5 × 10⁻⁴
= (25) × 10⁸⁻⁽⁻⁴⁾ N/m²
= 0.4 × 10¹² N/m² = 4 × 10¹¹ N/m²
.
Answer: Y = 4 × 10¹¹ N/m² (or Pa)
Problem 3: A spherical object contracts in volume by 0.01% when subjected to a uniform pressure of 100 atm. Calculate the bulk modulus (B) of the material. (1 atm ≈ 1.01×10⁵ Pa).
Pressure P = 100 atm = 100 × 1.01 × 10⁵ Pa = 1.01 × 10⁷ Pa.
Volume contracts by 0.01%, so fractional change in volume:
ΔVV = -0.01 % = - 0.01100 = -10⁻⁴
(Negative sign for contraction).
Bulk Modulus B = Pressure (P)(-ΔV / V)
B = 1.01 × 10⁷ Pa(- (-10⁻⁴)) = 1.01 × 10⁷10⁻⁴ Pa
= 1.01 × 10⁷⁺⁴ Pa = 1.01 × 10¹¹ Pa
.
Answer: B ≈ 1.01 × 10¹¹ Pa
Problem 4: A 2 cm cube has its upper face displaced by 0.1 mm by a tangential force of 8000 N. Calculate the shear stress and shear strain.
Given: Cube side L = 2 cm = 0.02 m.
Area of the face A = L² = (0.02 m)² = 0.0004 m² = 4 × 10⁻⁴ m².
Tangential Force F = 8000 N.
Displacement of upper face Δx = 0.1 mm = 0.1 × 10⁻³ m = 10⁻⁴ m.
Shear Stress:
Stress = Tangential ForceArea = 8000 N4 × 10⁻⁴ m²
= 2000 × 10⁴ N/m² = 2 × 10⁷ N/m²
.
Shear Strain:
The height between the fixed bottom face and the displaced upper face is L = 0.02 m.
Strain (θ) ≈ tan θ = ΔxL = 10⁻⁴ m0.02 m
= 10⁻⁴2 × 10⁻² = 0.5 × 10⁻² = 5 × 10⁻³
(Dimensionless).
Answer: Shear Stress = 2 × 10⁷ Pa, Shear Strain = 5 × 10⁻³
Problem 5: Calculate the elastic potential energy stored per unit volume in a wire with Young’s modulus Y = 2 × 10¹¹ N/m² when stretched by a strain of 10⁻³.
Given: Y = 2 × 10¹¹ N/m², Strain (ε) = 10⁻³.
Elastic Energy Density (Energy per unit volume) formula:
Energy Density = 12 × Y × (Strain)²
= 12 × (2 × 10¹¹ N/m²) × (10⁻³)²
= 12 × (2 × 10¹¹) × (10⁻⁶) J/m³
= 1 × 10¹¹⁻⁶ J/m³ = 10⁵ J/m³
.
Answer: 10⁵ J/m³
❓ Sawal Jawab (Questions & Answers)
🤏 Very Short Answer Questions
1. Define Elasticity.
Property of a body to regain its original shape/size after removal of deforming force.
2. Define Plasticity.
Property of a body by which it does NOT regain its original shape/size after removal of deforming force.
3. Define Stress.
Internal restoring force per unit area of cross-section.
4. What is the SI unit of Stress?
N/m² or Pascal (Pa).
5. Define Strain.
Ratio of change in configuration to the original configuration.
6. What is the unit of Strain?
It has no unit (dimensionless ratio).
7. State Hooke’s Law.
Within the elastic limit, stress is directly proportional to strain.
8. What is the constant E in Hooke’s law (Stress = E × Strain) called?
Modulus of Elasticity.
9. What does a larger value of Young’s modulus (Y) indicate?
The material is more elastic or stiffer (requires more stress for same longitudinal strain).
10. Define Longitudinal Strain.
Change in length / Original length.
11. Define Volumetric Strain.
Change in volume / Original volume.
12. What type of stress causes change in volume?
Volumetric Stress (Pressure).
13. What is the dimensional formula for Modulus of Elasticity?
[ML⁻¹T⁻²] (Same as Stress).
14. Define Poisson’s ratio.
Ratio of lateral strain to longitudinal strain within the elastic limit.
15. What is Elastic Potential Energy?
Energy stored in a body due to its deformation (work done during deformation).
16. Give an example of a nearly perfectly elastic material.
Quartz fibre.
17. Give an example of a plastic material.
Putty, Mud.
18. What is the reciprocal of Bulk Modulus called?
Compressibility.
📝 Short Answer Questions
1. Differentiate between Elastic and Plastic bodies.
- Elastic bodies regain original shape/size after removing deforming force (e.g., steel spring).
- Plastic bodies do NOT regain original shape/size after removing deforming force (e.g., putty).
2. Define the three types of stress (Longitudinal, Volumetric, Shear).
- Longitudinal: Force perpendicular to area, changes length (Tensile/Compressive).
- Volumetric: Uniform force perpendicular to entire surface, changes volume (like Pressure).
- Shear: Force parallel/tangential to surface, changes shape.
3. Define the three types of strain (Longitudinal, Volumetric, Shear).
- Longitudinal: Change in length / Original length (ΔL/L).
- Volumetric: Change in volume / Original volume (ΔV/V).
- Shear: Angle of deformation (θ) or Δx/L.
4. What is Elastic Limit? What happens beyond it?
- Elastic Limit: Max stress upto which body returns to original configuration completely after force removal.
- Beyond Elastic Limit: Body gets permanently deformed (plasticity) or fractures (breaks).
5. Define Young’s Modulus (Y). What does it measure?
- Y = Longitudinal Stress / Longitudinal Strain = (F/A)/(ΔL/L).
- It measures the material’s resistance to change in length (stiffness against stretching/compression).
- SI Unit: N/m² or Pa.
6. Define Bulk Modulus (B). What does its reciprocal measure?
- B = Volumetric Stress / Volumetric Strain = P / (-ΔV/V).
- It measures the material’s resistance to change in volume under pressure.
- Its reciprocal (1/B) is called Compressibility (k), measuring how easily volume changes.
7. Define Shear Modulus (G). Which state of matter does it apply to primarily?
- G = Shear Stress / Shear Strain = (Ftangential/A) / θ.
- It measures the material’s resistance to change in shape (rigidity).
- It applies primarily to Solids, as fluids cannot sustain shear stress.
8. Why is steel considered more elastic than rubber?
- Elasticity means resistance to deformation.
- For the same applied stress (force/area), rubber stretches much more (larger strain) than steel (smaller strain).
- Since Modulus E = Stress/Strain, a smaller strain for the same stress means steel has a much higher Young’s modulus (Y) than rubber.
- Therefore, steel resists deformation more strongly and is considered more elastic.
9. What is Poisson’s Ratio? Is it dimensionless?
- Ratio of Lateral Strain (change in diameter/original diameter) to Longitudinal Strain (change in length/original length).
- Symbol: σ (sigma) or ν (nu).
σ = Lateral Strain / Longitudinal Strain
.- Yes, it is dimensionless because it’s a ratio of two strains (which are themselves dimensionless).
10. Write the expression for Elastic Potential Energy stored per unit volume.
- Energy Density = ½ × Stress × Strain.
- OR Energy Density = ½ × Y × (Strain)².
- OR Energy Density = ½ × (Stress)² / Y.
- Unit: Joules per cubic metre (J/m³).
11. Draw a qualitative Stress-Strain curve for a ductile material like copper.
(Description of the graph)
- Initial straight line (O to A): Proportional region (Hooke’s Law).
- Curve up to B: Elastic region (returns to original shape). Point B = Elastic Limit / Yield Point.
- Curve continues, large plastic deformation region (C to D): Strain increases significantly for small stress increase.
- Point D: Ultimate Tensile Strength (max stress).
- Curve drops slightly then Point E: Fracture Point (breaks).
- Region between B and E represents plastic behavior.
12. Which is generally greater for metals: Young’s Modulus (Y) or Bulk Modulus (B)?
- For most common metals, the Bulk Modulus (B) is generally slightly smaller than or comparable to Young’s Modulus (Y).
- For example, Steel: Y ≈ 200 GPa, B ≈ 160 GPa. Copper: Y ≈ 110 GPa, B ≈ 140 GPa. Aluminum: Y ≈ 70 GPa, B ≈ 70 GPa.
- Shear Modulus (G) is usually the smallest of the three (roughly Y/3).
13. What is the difference between Tensile stress and Compressive stress?
- Both are types of Longitudinal Stress (Force applied perpendicular to area).
- Tensile Stress: Occurs when forces pull on the object, tending to increase its length (Stretching).
- Compressive Stress: Occurs when forces push on the object, tending to decrease its length (Compressing).
14. What are elastomers?
- Materials which can be stretched to cause large strains and still regain their original form.
- They do NOT obey Hooke’s Law (stress is not proportional to strain over large range).
- Example: Rubber used in aorta of heart, rubber bands.
15. The breaking stress for a metal is 7.8 × 10⁹ N/m². Find the maximum length of a wire of this metal which can hang vertically without breaking under its own weight (Density of metal = 7800 kg/m³; g ≈ 10 m/s²).
- Let max length = L, area = A, density = ρ.
- Weight of wire W = Mass × g = (Volume × Density) × g = (A × L × ρ) × g.
- This weight acts at the top support, causing max stress there.
- Max Stress = Weight / Area = (A L ρ g) / A = L ρ g.
- Given Max Stress = 7.8 × 10⁹ N/m².
- L ρ g = 7.8 × 10⁹
- L × 7800 × 10 = 7.8 × 10⁹
- L × 7.8 × 10⁴ = 7.8 × 10⁹
- L = (7.8 × 10⁹) / (7.8 × 10⁴) = 10⁹⁻⁴ = 10⁵ m.
- Answer: 10⁵ m (or 100 km).
📜 Long Answer Questions
1. State and explain Hooke’s Law. Discuss the Stress-Strain curve for a metallic wire.
Hooke’s Law: Within the elastic limit, stress is directly proportional to strain (Stress = E × Strain), where E is Modulus of Elasticity.
Stress-Strain Curve (for a ductile metal):
- O to A (Proportional Limit): Straight line. Stress ∝ Strain. Hooke’s law obeyed perfectly.
- A to B (Elastic Limit/Yield Point): Slightly curved. Stress is not strictly proportional, but the material still returns to original shape when unloaded. Point B is the yield point/elastic limit.
- B to D (Plastic Region): If loaded beyond B, material enters plastic region. Strain increases rapidly for small stress increase. Permanent deformation occurs even after unloading.
- D (Ultimate Tensile Strength): Max stress the material can withstand. Beyond this, ‘necking’ starts (wire becomes thinner at one point).
- D to E (Fracture): Stress decreases slightly but strain increases rapidly until fracture occurs at Point E.
Brittle materials fracture shortly after the elastic limit.
2. Define Young’s Modulus, Bulk Modulus, and Shear Modulus. Write their formulas and SI units.
1. Young’s Modulus (Y):
- Definition: Ratio of longitudinal stress to longitudinal strain (within elastic limit).
- Formula: Y = (F/A) / (ΔL/L) = FL / AΔL.
- Measures: Resistance to change in length (Stiffness).
- SI Unit: N/m² or Pa.
2. Bulk Modulus (B):
- Definition: Ratio of volumetric stress (Pressure P) to volumetric strain (within elastic limit).
- Formula: B = P / (-ΔV/V) = -PV / ΔV.
- Measures: Resistance to change in volume (Incompressibility).
- SI Unit: N/m² or Pa.
3. Shear Modulus (G or η):
- Definition: Ratio of shear stress to shear strain (within elastic limit).
- Formula: G = (Ftangential/A) / θ = (FtangentialL) / (AΔx).
- Measures: Resistance to change in shape (Rigidity).
- SI Unit: N/m² or Pa.
3. Explain the concept of Elastic Potential Energy. Derive the expression for energy stored per unit volume in a stretched wire.
Elastic Potential Energy: Work done in deforming an elastic body (against internal restoring forces) gets stored as potential energy within it. When the force is removed, this energy helps restore the body’s shape.
Derivation for Stretched Wire:
- Consider a wire of length L, area A, Young’s Modulus Y, stretched by ΔL by force F.
- Stress = F/A, Strain = ΔL/L. Assume Hooke’s law holds: F/A = Y(ΔL/L) => F = (YA/L)ΔL.
- Force is not constant; it increases from 0 to F as extension increases from 0 to ΔL.
- Work done (dW) for small extension (dl) = Force(l) × dl. Where Force(l) = (YA/L)l.
- dW = (YA/L) l dl.
- Total Work Done (W) for extension ΔL = ∫dW = ∫0ΔL (YA/L) l dl.
- W = (YA/L) [l²/2]0ΔL = (YA/L) (ΔL²/2).
- This Work Done is stored as Elastic Potential Energy (U). U = ½ (YA/L) ΔL².
Energy per unit Volume (Energy Density):
- Volume = A × L.
- Energy Density (u) = U / Volume = [½ (YA/L) ΔL²] / (AL)
- u = ½ × (Y) × (ΔL/L)² = ½ × Y × (Strain)².
- Since Y = Stress/Strain, we can write: u = ½ × (Stress/Strain) × Strain² = ½ × Stress × Strain.
- Also, Strain = Stress/Y, so: u = ½ × Stress × (Stress/Y) = ½ × (Stress)² / Y.
4. Define Poisson’s ratio. What does it signify? Can it be negative?
Poisson’s Ratio (σ or ν): Within the elastic limit, it is the ratio of lateral strain (strain perpendicular to the applied force) to the longitudinal strain (strain parallel to the applied force).
- Formula: σ = – (Lateral Strain) / (Longitudinal Strain) = – (ΔD/D) / (ΔL/L).
- The negative sign is often included because longitudinal extension (ΔL>0) usually causes lateral contraction (ΔD<0), making σ positive.
- Significance: It measures the tendency of a material to contract/expand in directions perpendicular to the direction of stretching/compression. It links changes in dimensions along different axes.
- It is a dimensionless quantity.
- Values: Theoretically, σ can range from -1 to +0.5. For most isotropic materials, experimental values lie between 0 and 0.5 (e.g., steel ≈ 0.3, rubber ≈ 0.5).
- Negative Poisson’s Ratio?: Yes, some materials called **auxetic materials** contract laterally when compressed longitudinally (or expand laterally when stretched), exhibiting a negative Poisson’s ratio. These are special engineered or natural structures.
5. A steel wire of length 1m and radius 1mm is stretched by a force of 100π N. If Young’s modulus Y=2×10¹¹ N/m², find the stress, strain, and elongation.
- Given: L = 1m, Radius r = 1mm = 1×10⁻³m, Force F = 100π N, Y = 2×10¹¹ N/m².
- Area (A): A = πr² = π(10⁻³)² = π × 10⁻⁶ m².
- Stress (σ): σ = F/A = (100π N) / (π × 10⁻⁶ m²) = 100 / 10⁻⁶ = 100 × 10⁶ = 1 × 10⁸ N/m² (or Pa).
- Strain (ε): From Hooke’s Law, Strain = Stress / Y.
ε = (1 × 10⁸ N/m²) / (2 × 10¹¹ N/m²) = 0.5 × 10⁻³ = 5 × 10⁻⁴. - Elongation (ΔL): Strain = ΔL / L => ΔL = Strain × L.
ΔL = (5 × 10⁻⁴) × (1 m) = 5 × 10⁻⁴ m = 0.5 × 10⁻³ m = 0.5 mm.
Answer: Stress=10⁸ Pa, Strain=5×10⁻⁴, Elongation=0.5 mm.
6. What do you understand by elastic fatigue?
Elastic Fatigue: It is the phenomenon where an elastic material loses its strength, or its elastic properties temporarily deteriorate, due to repeated alternating deforming forces applied to it.
- When a material is subjected to continuous, rapid cycles of stress and strain, its internal structure gets disturbed.
- It may not return exactly to its original state immediately after the force is removed, or it might require less stress to reach its elastic limit, or its breaking point might lower.
- This ‘tiredness’ of the elastic material is called elastic fatigue.
- Example: This is why old bridges are sometimes declared unsafe after prolonged use, as the materials undergo fatigue due to repeated stress cycles from traffic and temperature changes. Bridges need regular inspection for signs of fatigue.
- The elastic properties can often be regained after a period of rest, but repeated fatigue can lead to eventual failure.
7. Explain ductile and brittle materials based on the stress-strain curve.
The shape of the stress-strain curve beyond the elastic limit differentiates ductile and brittle materials:
- Ductile Materials:
- These materials exhibit a significant **plastic region** after the yield point (elastic limit).
- They undergo considerable deformation (elongation/strain) before fracturing.
- Stress-strain curve shows a large difference between the yield point and the fracture point.
- Examples: Copper, Aluminum, Mild Steel. They can be drawn into wires (ductility).
- Brittle Materials:
- These materials show very little or **no plastic deformation**.
- They fracture (break) suddenly soon after the elastic limit is crossed, with very little elongation.
- The yield point, ultimate strength, and fracture point are very close on the stress-strain curve.
- Examples: Glass, Cast Iron, Ceramics, Concrete. They tend to shatter when overloaded.
8. Two wires of same length and material but radii r₁ and r₂ are stretched by the same force. Find the ratio of stresses and strains produced in them.
Let Force = F, Length = L, Material has Young’s Modulus Y.
- Wire 1: Radius r₁, Area A₁ = πr₁².
- Wire 2: Radius r₂, Area A₂ = πr₂².
Ratio of Stresses:
- Stress σ = Force / Area.
- σ₁ = F / A₁ = F / (πr₁²)
- σ₂ = F / A₂ = F / (πr₂²)
- Ratio:
σ₁σ₂ = (F / A₁)(F / A₂) = A₂A₁ = πr₂²πr₁² = r₂²r₁²
.
Ratio of Strains:
- Young’s Modulus Y = Stress / Strain => Strain ε = Stress / Y.
- Since material is same, Y is same for both (Y₁=Y₂=Y).
- ε₁ = σ₁ / Y
- ε₂ = σ₂ / Y
- Ratio:
ε₁ε₂ = (σ₁ / Y)(σ₂ / Y) = σ₁σ₂
. - From stress ratio,
ε₁ε₂ = r₂²r₁²
.
Answer: Ratio of Stresses (σ₁/σ₂) = r₂²/r₁²; Ratio of Strains (ε₁/ε₂) = r₂²/r₁².
9. What is the elastic potential energy stored in a wire of length L, area A, stretched by an amount x, if its Young’s Modulus is Y?
- Force required to produce extension x: F = (YA/L)x (from Y = (F/A)/(x/L)).
- This force varies from 0 to F as extension goes from 0 to x. Average force = (0+F)/2 = F/2.
- Work Done (Stored Energy U) = Average Force × Extension.
- U = (F/2) × x.
- Substitute F = (YA/L)x:
- U = (1/2) × [(YA/L)x] × x
- U = ½ (YA/L) x²
(Alternatively, using Energy Density = ½ × Y × (Strain)²: Strain = x/L. Volume = AL. U = (½ × Y × (x/L)²) × (AL) = ½ Y (x²/L²) AL = ½ (YA/L) x²).
Answer: U = ½ (YA/L) x²
10. Differentiate between Pressure and Stress.
- Stress: Internal restoring force per unit area developed *within* a deformed body. Can be tensile, compressive, or shear. A tensor quantity (though often treated as scalar/vector in simple cases). Depends on internal forces. (Vastu ke andar develop hua internal force per unit area).
- Pressure: External force acting perpendicularly per unit area *on* a surface (usually of a fluid). Always compressive. A scalar quantity. Depends on external forces. (Kisi satah par perpendicularly lag raha bahari force per unit area).
- While both have same dimension [ML⁻¹T⁻²] and SI unit (Pa or N/m²), they represent different physical concepts related to internal restoring forces vs external applied forces. Volumetric stress is numerically equal to pressure.