Young Modulus of Copper Essay Example for Free

untried Modulus of Copper EssayTheoryThe following quantities is important for the experiments concernsStress is defined as ? =Force / cross-section(a) area ( F/A ) zephyr is defined as ? = Extension / natural duration ( e/l )The ratio of Stress to Strain, is the Young modulus (E= ?/?)Since a stiffer material requires larger stress to produce the corresponding strain , a stiffer material would have a greater Young modulus ( a greater position in a graph of ? against ? ) .For a non brittle material, usually there are two puts of overrefinement before sorting. Stage 1 live deformationIn this stage, the conducting electrify would return to its natural length when the stress is removed. Hookes law is usually obeyed in this stage, therefore the graph is almost a straight line.When the wire is further stretched, it reaches the stretchable limit and stun intostage 2.Stage 2 Plastic deformationIn this stage, the stress is not directly proportional to the strain and and a sm all amount of stress support produce a large strain. If the wire passes the yield point, its get out have permanent extension and will not return to its current length. Finally, when the wire is kept to stretched, it will break at the breaking point. turnExperiment 1Study the stress-strain behaviour of a copper wire1.A micrometer screw tidal bore was used to measure the diameter of the copper wire at some(prenominal) points. taut value was taken and the cross-sectional area of the wire was calculated.2.A pulley was mounted on one side of the table. A 2 m segment of the wire was cut out and was clamped firmly by using a G-clamp which was at a space about 1.5 m form the pulley.3.The wire was put over the pulley. Some newspapers were limit one the ground below the pulley.4.A label marker is sticked on the wire at a blank about 0.5 m from the pulley. A bill rule was placed below the wire and was fixed on the table by sticky tape.5.A 100g hanger was tied to wire.6.The length b etween the G-clamp and the sticker, which represents the natural length, was measured.7.100g load was added to the hanger one by one , and the extension was recorded each time.8.Load was kept increasing until the wire broke.Experiment 2 Elastic deformation and Young modulus1.A new wire of the same length and thickness was used and steps 1 to 7 in experiment 1 were repeated.2.Load was added to the hanger carefully. All the load were removed each time to come off whether the wire would return to the original length. Results were recorded.3.Step 2 was repeated until the elastic limit was just exceeded.Precautions1.The hanger should be more than than 0.5 m above the newspapers. This allows the wire to get enough space for extensions before it breaks. Also it should not be kept too high from the ground, this may cause the tiles of the floor to break.2.The sticker should not be placed too close to the pulley. If not the wire may touch the pulley when the wire is extended. A distance of 0.4 m is preferred.3.The load should be added to the hanger slowly and carefully. This is to avoid exerting impulse to the wire and making the masses to oscillate. differently the wire may get extra extension and make the records not appropriate.4.Records should be taken still after the sticker stops moving. This is because the wire takes time to extend itself, especially at the later stage when the wire passed the elastic limit and was near breaking.ResultsDiameter of the copper wireD1D2D3D4MeanValue(in 0.005mm)0.3700.3650.6700.3700.3688Natural length of the wire=1.15mExperiment 1Load(kg)0.10.20.30.40.50.60.70.8Extension(10-3 m)00.50.5111.51.52.0Load(kg)0.911.11.21.31.41.51.6Extension(10-3 m)2.52.53.03.03.54.05.512Load(kg)1.71.81.92.02.12.22.3 humbledExtension(10-3 m)193446607798125/ level best load for elastic deformation=1.3 kgLoad for breaking the wire=2.3 kgExperiment 2 Load(kg)0.10.20.30.40.50.60.70.8Extension(10-3)00.50.811.21.51.52Load(kg)0.911.11.2ElasticlimitexceededExte nsion(10-3)2.52.533.5///Calculations GraphsMaximum possible error of metre rule = 0.1 cm=0.01mMaximum possible error ofmicrometer screw gauge =0.005mm=510-6 mcross-section(a) area of the wire = 1.06810-7 m2 parcel error = 26.77810-3 =1.3557%?Cross-sectional area = (1.071 0.01)x10-7 m2Experiment 1Stress Strain relationshipStress(M Pa)9.34518.6928.0337.3846.7356.0765.4274.76Strain(10-3)00.43480.43480.86960.86961.3041.3041.7392Stress(M Pa)84.1193.45102.8112.1121.5130.8140.1149.5Strain(10-3)2.1742.1742.6092.6093.0433.4784.78310.44Stress(M Pa)158.9168.2177.6186.9196.3205.6215.0BrokenStress(10-3)16.5229.5740.0052.6166.9682.61108.7/Stress at elastic limit=124 M PaPercentage error=Percentage error of the area of the wire=1.3557%?Stress at elastic limit=(124 2)M PaBreaking stress=(215 Pa 3)M PaExperiment 2Stress Strain relationship up to elastic limitStress(M Pa)9.34518.6928.0337.3846.7356.0765.4274.76Strain(10-3)00.46730.74770.93461.1211.4021.4021.869Stress(M Pa)84.1193.45102.8112.1El asticlimitexceededStrain(10-3)2.3362.3362.8043.271///Mean of the stress=60.7 M PaMean of the strain=1.5610-3Slope of the best-fit line=38.9 G PaMaximum slope=42.2 G PaMinimum slope=30.0 G PaMean error=(38.9-36.1)=2.8 G Pa?Young modulus of the copper wire=(38.9 2.8)G PaErrors and Difficulties1.There were systematic errors in this experiment. The masses were not leaden to check what its actual weight is. The wire may not be made of pure copper. The publicise temperature may vary due to air-conditioners. Besides, gravitational acceleration is taken as 10ms-2 instead of 9.8ms-22.There was a random error in deliberateing the sticker. Since the sticker had a few distance from the ruler, errors due to parallax would arise if we view form a little bit right or left. So it is difficult to obtain the critical value. To improve this, a nail can be added onto the sticker. The nail was more stable and gave readings very sharply.3.At the lineage of the experiment, the wire is very uneven. Th e first few extensions we taken may be only due to the straighten of the wire into a straight shape.(just like stretching a spring into a straight wire)sermon1.Near the breaking point, the shape of the wire is very narrow.2.During elastic deformation, the hanger falls and loses gravitational potential energy. This energy agitate to elastic potential energy. If the wire is unloaded, the energy will be restored to GPE and the wire will return to is original length.3.During plastic deformation, the loss of gravitational potential energy becomes the work done to increase the length of the wire (increase the separations of the particles in the wire). This energy would not be restored even the wire is unloaded.4.Double of the amount of the load is required to break the wires.ConclusionTo obtain the Young modulus of the copper wire by this experiment is convenient. A few apparatus and steps are needed, and it only involves easy calculations. But by comparing to the actual value(124G Pa) , the result we get (38.9 G Pa) has a great difference from it.This may due to the experiment is done in several assumptions and estimations. We assumed g=10ms-2 and the wire is made of pure copper. We neglected environmental factors and assumed the wire was stretched as in every parts.In short, although the experiment is not accurate enough, it provides a good chance for students to execute what they have learned. It is quite shocked that a very thin and long wire can hold firm more than 2 kg load.