Tensile Test 1. Purpose and Procedure of Tensile Testing Tensile testing is a destructive mechanical testing method where a sample is subjected to a controlled, increasing axial tensile load until it fractures. The load applied to the specimen and the resulting elongation are recorded simultaneously. Purpose of the Test: ο· Mechanical Property Determination: To determine fundamental mechanical parameters such as Young's modulus, yield strength, ultimate tensile strength (UTS), ductility, and fracture behaviour. ο· Quality Assurance and Material Validation: To verify that manufactured batches or received stock meet commercial standards and strength specifications. ο· Engineering Design Data: To provide quantitative stress-strain data required to calculate safe allowable loads, cross-sectional dimensions, and safety factors for structural components. ο· Material Comparison: To compare how different alloys, heat treatments (e.g., annealing vs. quenching), or cold-working processes alter mechanical behaviour. General Procedure Overview: The test specimen is mounted into the upper and lower grips of a Universal Testing Machine (UTM). An axial pulling force is applied at a specified, quasistatic loading rate. An extensometer attached to the gauge length records elongation, while a load cell measures the instantaneous force. The data acquisition system translates the load-displacement output into stress-strain data. 2. Engineering and True Stress-Strain Curves Raw load-elongation data is converted to stress and strain to eliminate geometric size dependencies. Engineering Stress (π) and Engineering Strain (π) Engineering stress and strain are calculated based strictly on the original, undeformed dimensions of the specimen: π= π= π π΄0 ΔπΏ πΏ − πΏ0 = πΏ0 πΏ0 [MPa] [dimensionless] ο· π = instantaneous applied force (N) ο· π΄0 = original cross-sectional area (mm2 ) ο· πΏ0 = original gauge length (mm) ο· πΏ = instantaneous gauge length (mm) Engineering stress-strain curves are standard in structural design because original component dimensions are fixed and known beforehand. True Stress (ππ ) and True Strain (ππ ) True stress and true strain use the instantaneous cross-sectional area (π΄π ) and gauge length (πΏπ ) during deformation: ππ‘ = ππ‘ = ln ( π π΄π [MPa] πΏπ ) = ln(1 + π ) πΏ0 Assuming constant material volume during uniform plastic deformation (π΄0 πΏ0 = π΄π πΏπ ), true stress relates to engineering values prior to necking by: ππ‘ = π(1 + π ) Key Differences & Necking Behavior ο· Elastic & Uniform Plastic Region: Deformations are small; engineering and true curves lie close to each other. ο· Post-Necking (Past UTS): Localized cross-sectional area reduction ("necking") occurs. In the engineering curve, stress appears to drop because the applied load decreases while dividing by the fixed original area π΄0. In the true stress curve, stress continues to rise until fracture because the true load-bearing area π΄π decreases sharply and the material continues to strain harden. 3. Test Specimen Details and Experimental Procedure 3.1 Objective & Apparatus Used ο· Objective: To conduct a tensile test on a given test specimen and determine its tensile strength using a Universal Testing Machine (UTM). ο· Equipment Used: o Universal Testing Machine (UTM) with TW Elite control and data acquisition software o Digital / Vernier Calliper o Turned metallic tensile test specimen 3.2 Test Specimen Geometry and Dimensions (Initial & Final) The tensile test was conducted on an Aluminium specimen with the following dimensions: ο· Material: Aluminium ο· Initial Gauge Length (πΏ1): 45.12 mm ο· Initial Gauge Diameter (π1): 10 mm ο· Initial Cross-Sectional Area (π΄1): π ⋅ π12 π ⋅ (10)2 π΄1 = = = 78.54 mm2 4 4 ο· Grip Separation: 53.12 mm ο· Final Gauge Length after Breaking (πΏ2 ): 53.16 mm ο· Final Diameter at Breaking Place (π2): 6 mm ο· Final Cross-Sectional Area at Fracture (π΄2): π ⋅ π22 π ⋅ (6)2 π΄2 = = = 28.27 mm2 4 4 3.3 Test Parameters & Settings ο· Test Rate (Loading / Displacement Speed): 0.1 mm/sec (6.0 mm/min) ο· Data Acquisition Rate: 2 Hz 3.4 Step-by-Step Experimental Procedure 1. Measurement of Initial Dimensions: The original gauge length (πΏ1 = 45.12 mm) and diameter (π1 = 10 mm) of the turned Aluminium specimen were measured using a Vernier Calliper. 2. Specimen Mounting: The specimen was properly aligned and clamped into the upper and lower grips of the Universal Testing Machine (UTM) with a set grip separation of 53.12 mm. 3. Software Setup & Test Initiation: Input values and test parameters (Test rate: 0.1 mm/s, Data acquisition rate: 2 Hz) were entered into the TW Elite software, and the load application was initiated. 4. Execution: The tensile load was continuously applied at the constant displacement rate while load and elongation were recorded until complete fracture of the specimen occurred. 5. Post-Fracture Measurements: The two broken halves of the fractured specimen were joined together, and the final length (πΏ2 = 53.16 mm) and the final diameter at the necked fracture zone (π2 = 6 mm) were measured and recorded. 3.5 Observations and Key Experimental Findings ο· Material Tested: Aluminium ο· Change in Length (ΔπΏ): ΔπΏ = πΏ2 − πΏ1 = 53.16 mm − 45.12 mm = 8.04 mm ο· Diameter Reduction (Δπ): Δπ = π1 − π2 = 10 mm − 6 mm = 4 mm ο· Angle of Necking / Shear Fracture Plane: ≈ 45β (typical ductile shear fracture along planes of maximum shear stress) ο· Peak Load (πpeak ): 18.995 kN (18,995 N) ο· Peak Stress (Ultimate Tensile Strength): πpeak = ο· 18.995 kN 2 2 = 0.2419 kN/mm = 241.9 MPa 78.54 mm Strain at Break (πbreak ): 0.138 mm/mm (13.8%) 4. Material Properties Measurable Using Tensile Testing ο· Modulus of Elasticity (Young's Modulus, πΈ): The ratio of tensile stress to tensile strain within the linear elastic limit (πΈ = π/π). It quantifies the inherent atomic bond stiffness and resistance to elastic deformation. ο· Yield Strength (ππ¦ ) / 0.2% Offset Proof Stress: The stress at which permanent, non-recoverable plastic deformation begins. For materials like aluminium that do not have a sharp yield drop, a line drawn parallel to the initial elastic slope at a 0.2% strain offset (π = 0.002) determines the proof stress. ο· Ultimate Tensile Strength (UTS / Peak Stress, ππ’ ): The maximum engineering stress sustained by the material before the onset of localized necking. ο· Fracture Strength (ππ ): The engineering stress at which the material separates into two pieces. ο· Ductility (% Elongation and % Reduction in Area): Quantifies the extent of plastic deformation a material can endure prior to failure: % Elongation = ( πΏ2 − πΏ1 ) × 100% πΏ1 % Reduction in Area = ( π΄1 − π΄2 ) × 100% π΄1 ο· Modulus of Resilience (ππ ): The maximum elastic energy per unit volume absorbed without permanent deformation (area under the elastic portion). ο· Modulus of Toughness (ππ‘ ): The total strain energy absorbed per unit volume before complete rupture (total area under the entire stress-strain curve). 5. Advantages of Tensile Testing ο· Direct and Uniaxial Stress Distribution: Provides a clean, onedimensional stress state, making theoretical modeling and mechanical property calculation direct and reliable. ο· Multiple Properties in a Single Experiment: Yield strength, ultimate tensile strength, Young's modulus, ductility, and fracture behavior are obtained simultaneously from one test. ο· Global Standardization: Adherence to established test standards (such as ASTM E8/E8M and ISO 6892-1) ensures reproducibility across different labs and test equipment. ο· Primary Basis for Structural Design: Yield strength and UTS directly define working stress limits, allowable loads, and safety factors for engineering components. ο· Effective Quality Control: Serves as a standard inspection tool to verify whether raw materials, alloys, or heat-treated components meet commercial engineering specifications. 6. Experimental Data (from Lab Work) and Property Measurements 61 Recorded Lab Data & Specimen Geometry (Aluminium Specimen) Parameter Symbol / Relation Value from Lab Sheet Material — Aluminium Initial Gauge Length πΏ1 45.12 mm Initial Diameter π1 10 mm π ⋅ π12 π΄1 = 4 78.54 mm2 Initial Cross-Sectional Area Grip Separation — 53.12 mm Test Rate / Speed — 0.1 mm/s (6.0 mm/min) Parameter Symbol / Relation Data Acquisition Rate — Peak Load Value from Lab Sheet 2 Hz πpeak 18.995 kN (18,995 N) Peak Stress πpeak 0.2419 kN/mm2 (241.9 MPa) Strain at Break πbreak 0.138 mm/mm (13.8%) Final Length After Breaking πΏ2 53.16 mm Final Diameter at Fracture π2 6 mm Final Cross-Sectional Area π ⋅ π22 π΄2 = 4 28.27 mm2 Change in Length ΔπΏ = πΏ2 − πΏ1 8.04 mm Reduction in Diameter Δπ = π1 − π2 4 mm Necking / Fracture Angle — 45β (Shear failure plane) 6.2 Calculations of Mechanical Properties from Lab Observations 1. Modulus of Elasticity (Young's Modulus, πΈ): For standard structural aluminium alloys, the linear elastic slope in the proportional region yields: πΈ= Δπ ≈ 69 – 71 GPa Δπ 2. Yield Strength (0.2% Proof Stress, π0.2%): Because aluminium does not show a sharp yield drop, the proof stress is determined by drawing a line with slope πΈ offset by 0.002 (0.2%) strain: π0.2% ≈ 190 – 215 MPa (0.190 – 0.215 kN/mm2 ) 3. Ultimate Tensile Strength (Peak Stress, UTS): UTS = πpeak = πpeak 18.995 kN = = 0.2419 kN/mm2 = 241.9 MPa 2 π΄1 78.54 mm 4. Ductility (% Elongation and % Reduction in Area): ο· Percentage Elongation (%EL): %πΈπΏ = ( πΏ2 − πΏ1 53.16 − 45.12 8.04 ) × 100% = ( ) × 100% = ( ) × 100% πΏ1 45.12 45.12 = 17.82% (Note: The recorded extensometer/software strain at break along the monitored span is 0.138 or 13.8%, while manual end-to-end measurement gives 17.82%.) ο· Percentage Reduction in Area (%RA): %π π΄ = ( π΄1 − π΄2 78.54 − 28.27 50.27 ) × 100% = ( ) × 100% = ( ) × 100% π΄1 78.54 78.54 = 64.00% 5. True Fracture Stress (ππ,true): ππ,true = πfracture π΄2 7. External Resources & References 1. ASTM International. (2021). ASTM E8/E8M-21: Standard Test Methods for Tension Testing of Metallic Materials. West Conshohocken, PA; ASTM International. 2. International Organization for Standardization. (2019). ISO 6892-1:2019: Metallic materials — Tensile testing — Part 1: Method of test at room temperature. Geneva, Switzerland: ISO. 3. Callister, W. D., & Rethwisch, D. G. (2018). Materials Science and Engineering: An Introduction (10th ed.). Hoboken, NJ: John Wiley & Sons. 4. Dieter, G. E. (1986). Mechanical Metallurgy (3rd ed.). New York, NY: McGraw-Hill Book Company. 5. Dowling, N. E. (2013). Mechanical Behaviour of Materials: Engineering Methods for Deformation, Fracture, and Fatigue (4th ed.). Boston, MA: Pearson. Q&A SECTION Question 1 Ultimate Tensile strength or Yield strength which is preferred as a design parameter for a proper selection of materials for structural application and why? Answer: Yield Strength (ππ¦ ) is preferred as the primary design parameter for structural applications. ο· Prevention of Permanent Distortion: Structural components (e.g., beams, bridges, aircraft frames, pressure vessels) must maintain their original dimensions, tight tolerances, and alignments during service. If operating stresses exceed the yield strength, non-recoverable plastic deformation occurs, causing misalignment, structural sagging, binding of moving parts, and functional failure. ο· Basis for Allowable Working Stress: In linear elastic structural design, the working allowable stress (πallowable ) is calculated directly from the yield strength using a Factor of Safety (FOS): πallowable = ππ¦ FOS This guarantees that all operating stress states remain strictly in the reversible elastic regime where Hooke's Law holds. ο· UTS Represents Post-Deformation Capacity: Ultimate Tensile Strength (UTS) is achieved only after extensive plastic elongation and severe necking have already occurred. Relying on UTS would allow major geometric collapse before the nominal material capacity is reached. (UTS is only used as a secondary check to ensure a safety margin against total structural rupture under unexpected overloads). Question 2 What is strain hardening? Explain with a drawing. Answer: Strain hardening (also referred to as work hardening or cold working) is the process where a ductile material becomes stronger, harder, and more resistant to further deformation as it undergoes plastic (permanent) deformation below its recrystallization temperature. 1. Microscopic Mechanism ο· At the crystalline level, plastic deformation takes place via the movement and generation of line defects called dislocations. ο· As plastic deformation increases, the dislocation density in the crystal lattice multiplies drastically (from roughly 107 cm−2 in an annealed material to 1011 --1012 cm−2 in a deformed state). ο· These moving dislocations intersect, entangle, and pin each other, creating internal stress fields that act as barriers against further dislocation movement. ο· Consequently, a progressively higher applied shear stress is required to overcome these barriers and produce additional plastic flow, leading to an increase in macroscopic yield strength and tensile strength. 2. Explanation of the Drawing (Macroscopic Loading & Unloading Behaviour). Initial Elastic & Plastic Loading: The virgin metal is loaded from the origin. It deforms elastically along the initial linear slope (Young's modulus πΈ) until it reaches its original yield strength ππ¦0. Loading past ππ¦0 induces plastic deformation and strain hardening along the curve up to Point A (ππ¦1). Elastic Unloading: When the load is released from Point A, the material unloads elastically along a straight dashed line parallel to the original elastic slope (πΈ). During unloading: ππ¦1 ο· The elastic portion of strain is recovered: ππ = ο· A permanent plastic strain ππ remains in the specimen. πΈ Subsequent Reloading: When the specimen is reloaded, deformation proceeds elastically back along the unloading line directly up to Point A. Result: Plastic deformation does not resume until the stress exceeds the elevated stress level at Point A. Thus, the material now has a new, higher yield strength (ππ¦1 > ππ¦0), expanding its elastic range at the expense of remaining ductility. Question 3 Name any two standards used for the tensile testing of metal and composites (at least one for each). Answer: ο· Standard for Metals: o ASTM E8 / E8M: Standard Test Methods for Tension Testing of Metallic Materials (or ISO 6892-1: Metallic materials — Tensile testing — Part 1: Method of test at room temperature) ο· Standard for Composites: o ASTM D3039 / D3039M: Standard Test Method for Tensile Properties of Polymer Matrix Composite Materials (or ISO 527-4 / ISO 527-5: Plastics — Determination of tensile properties of isotropic and orthotropic fibre-reinforced plastic composites) Question 4 What is the loading rate/displacement speed in a quasi-static tensile test as per a standard (refer a standard and name the standard)? Answer: ο· Reference Standard: ASTM E8 / E8M (Standard Test Methods for Tension Testing of Metallic Materials). ο· Specified Loading Rates & Displacement Speeds: o Elastic & Yield Determination Regime (Strain-Rate Control / Method A): The strain rate is maintained within 0.00025 to 0.0025 mm/mm/min (or a stress rate between 1.15 and 11.5 MPa/s). o ο· Post-Yield & Plastic Regime to Fracture (Crosshead Speed Control): Once yielding is complete, the testing speed is increased to a uniform crosshead displacement rate between 0.05 and 0.5 mm/mm of gauge length per minute (which corresponds to 1.0 to 2.5 mm/min for standard 50 mm gauge length specimens). Purpose: These low speeds ensure that quasi-static equilibrium is maintained without dynamic inertial effects, strain-rate sensitivity, or adiabatic deformation heating. Question 5 Draw stress-strain curves for (i) a metal, (ii) a ceramic, (iii) a polymer. Highlight key features. Label with the material name. Answer: Key Features Highlighted by Material: ο· (i) Metal (e.g., Structural Mild Steel / Ductile Aluminium): o Linear Elastic Region: Steep initial slope (πΈ ≈ 70–210 GPa) following Hooke's Law. ο· ο· o Yield Point: Distinct yield strength (ππ¦ ) marking the onset of dislocation motion. o Strain Hardening & UTS: Continuous increase in strength up to peak load (UTS). o Necking & Ductile Fracture: Localized cross-sectional area reduction and cup-and-cone shear fracture at high failure strain (ππ ≈ 15–25%). (ii) Ceramic (e.g., Alumina Al2 O3 / Silicon Carbide): o Very High Elastic Modulus: Extremely steep linear slope (πΈ ≈ 300–400 GPa). o Brittle Fracture: Direct failure in the linear elastic regime with zero plastic deformation (ππ < 0.2%) due to the inability of dislocations to move past covalent/ionic bonds and rapid propagation of micro-cracks. (iii) Polymer (e.g., Thermoplastic HDPE / PMMA): o Low Modulus & Viscoelasticity: Low initial slope (πΈ ≈ 1–3 GPa). o Yielding & Neck Formation: Reaches an initial yield peak at low stress (≈ 30–40 MPa). o Cold Drawing (Plateau): Long flat plateau where folded polymer chains uncoil and reorient along the loading axis. o Strain Alignment & High Elongation: Orientation hardening occurs near failure, leading to fracture at very large strains (ππ > 40–50%).
0
You can add this document to your study collection(s)
Sign in Available only to authorized usersYou can add this document to your saved list
Sign in Available only to authorized users(For complaints, use another form )