Constantan and Copper Essay Example for Free

Constantan and Copper Es narrateThis crystalline whence depart non be able to hold the amount of underscore which go taboo be exerted by the bur thuslys slowly being added on however we stick out predict that the fuzz element leading face ofttimes stress and on that pointfore allow for experience necking as the atoms as projectn in the diagram pull up stakes slide the atoms and therefore they post slide past each other more(prenominal) easily, consequently resulting in the separate of the tangible. Copper is generally by itself very weak that is why it motifs to be hardened and streng past for many industrial applications. It is therefore mixed with other alloys and melted. When carrying come to the fore this experiment I support that as the number of weights is increased for copper, this will slowly exert pressure and the molecules will slowly pull obscure as the bond will break between the molecules. The material will reach its elastic limit, where it has reached its record where by after if any more weights are added consequently it will deform and non dedicate to its original state. Here is a diagram below which illustrates this (Image additionalcted from natural philosophy textbook)The equations that I will acquire in this investigation to find step up the quarry, which is to find out youngs modulus of both materials through drawing of the represents from the results I will need to use the avocation equation as this is what will aid me achieve this part of the aim From my charts, I will find out the gradient and therefore be able to work out youngs modulus by the principlee above. I believe that youngs modulus for constantan will be high because I consider from the express provided that it will be able to take more contrast then the copper (crystalline).I deem this simply because constantan being an admixture can take more of a load then a pure metal. Here is a typical example of a stress train chart (obtained from my physics textbook) Fair test Test the conducting fit out to get an amount I will do this three quantify. All of my foretells will be to three significant figures. I will carry this out on the same day in the same conditions, using all of the same apparatus. I will stay fresh the metre stick stuck down to the table and not move it, so that it wont chance upon my results, when marking off the extension. ApparatusI will be using the following Pulley m ruler and a marker Mass weights and actual storage unit Wooden blocks to hold the fit out in place A G clamp. Safety I will ensure that I keep this a safe experiment by Keeping the cardboard over the electrify, as when the cable snaps the wire would not suddenly lift up and cause any danger. I will also pass sure there are not people crowding the experiment when it is being carried out, as the weights can cause danger if they fall. Results I gather in entered the results I reserve been given into Microsoft excel.From this the extension I have been given, is given in mm, hardly in physics we have to convert mm to metres. From the materials given I would find out the area of the wire as the area can depend on the wires, as they can have different thicknesses. Diameter 0. 37mm The cross sectional area pi r2=1. 07510-7m2 To find the out the cross sectional area I simply had worked out the radius, which was 0. 000185, I achieved this figure by dividing the diameter (0. 37) by 2000. By calculating this I was left with this figure. I will need to find out stress over argument which will give me youngs modulus.Since the length of the wire is 2. 1metres this will be used to find out the strain. Here are my results for copper Here is my table of results covering results from the copper wire. I have worked out the stress and strain which therefore simply allowed me to work out the youngs modulus of copper, and this I have shown on the computer. I have also shown the table showing the formulae I had g ossip in the cells in Microsoft Excel. I have shown this below, in the last four columns where I had input the formula into the cells to aid me to work out youngs modulus of copper.I have shown the results I had obtained for copper above, now I will produce a table showing the results I achieved for constantan the alloy which I believe would have a higher youngs modulus then copper. I had used the same length of wire which is 2. 1metres as I made sure this was a fair test when conducting the experiment. I have worked out the cross sectional area as the same in the procedure before. Here are my results for constantan Diameter 0. 3510-3 body politic p r29. 621010-8 m2 Here are my results stated above showing the results from the constantan wire.The results show the youngs modulus for constantan at the given force. Below is the formulae table showing the formulae which were input into the cells from stress and strain. When simplifying these results it will be evident I belie that the constantan wire will have the higher youngs module, and this will be clear in the graphs I produce. I have now simplified my results so that I can easily plot my graph from these results. I have made them show the stress to the antecedent of 10 to the 7, and strain which is ten to the power of minus three. Here are my two tables Results for constantan (for graph)Stress Nm multiplication 10 Strain Youngs Modulus times by 10 (times 10 ) Stress Nm times ten Strain (e/L) Youngs Modulus times by ten times by ten Analysis In this experiment my aim objective was to find youngs modulus from copper and constantan wire. I have shown this by winning the first step which was to produce the results table, and from this I have plotted the graphs showing the force against the amount extension. spy my graphs you can see that I have plotted two separate graphs showing force against the average extension for both materials.Furthermore, you can also see that I have created the graphs showing stres s-strain for copper and constantan. This graph typically shows youngs modulus. The wires had reacted to the weights in the way that I had expected as I predicted that constantan wire will have the higher youngs modulus and is more tough typically because it is an alloy which contains 40% nickel note which makes this element extra strong, whereas the copper is a pure metal and will not be able to take the strain of the load and this is proven as the copper wire could and take 24N as it broke, whereas constantan wire could take almost double the amount 42N.This illustrates that constantan wire needs more force to tender the wire whereas copper is a material which is frail and would extend by a suitable weight which puts strain onto the material. We can perceive that copper is more easy to stretch by the info I have produced in the table as at 20N it had an average extension of 0. 013 metres, however constantan wire if what my surmisal is, then I believe that at 20N, constantan sho uld have a smaller average extension then copper has. Looking at the table, the average extension for constantan at 20N is 0. 006 metres.This proves my theory correct as these two results show the variance between the two materials instantly. We can now say that constantan is more tensile, as an alloy it has an enables the dislocation of the atoms which help grip the structure together and therefore give it the property of being tough, this is explained in my diagram I have force on paginate 3. I believe that the atoms in the pure metal copper, had displaced and therefore become unstable when the load was placing strain upon the wire. This would ultimately, make the atoms move out of position and break up, resulting in the wire shattering.This is why when the copper wire had reached its maximum load which was 24N, the atoms had suffered a long-lasting deformation in the arrangement as they would have been changed in their formation, but unable to move back. This is the same prin ciple with the wire, as it was being stretched and the atoms moved out of place, but the load was greater then the elastic limit could handle and this is why there is a permanent deformation where the wire does not return back to it original shape and changes length, resulting in the increase in extension.In the constantan wire, this would be identical however the atoms would be harder to move out of place, as this material can handle far more load then the copper wire could. So at the same weight (24N) this wire would still return to its original shape because it is in its elastic state. even so once it exceeds it elastic limit, then the wire loses its formation of atoms and does not return to its original shape. Here is a graph showing elastic and plastic locations in this graph, this is a way of working out youngs modulus, or by working out the gradient of a graph.I have also anchor a diagram from my physics textbook, which shows the general yield stress for materials including copper and constantan. By observing the diagram this will give further evidence for my analysis upon the results I have achieved What each of my graphs show My first graph shows force against the average extension for the copper wire, this graph shows that the average extension had increased with the force, however only to a certain point, as this remained elastic from 0N to 24N. After this remained plastic, where the wire could not handle any more load and had shattered.My second graph shows force against average extension for constantan wire. This wire indicated through the graph actually can handle much load, and it has a very large elastic region, as this alloy is very tough, therefore can handle large amounts of weights. This wire could handle 42N however after it then remains plastic, and broke. The third and final graph illustrates further insight into the youngs modulus of copper and constantan wire, as I have plotted the two materials on the same graph.It is indicated that constantan has a higher youngs modulus compared to copper material. This is because copper can easily be shattered as it stretched very much compared to constantan. The gradient is smaller compared the constantans, which manner copper has the smaller youngs modulus because it is a metal and nothing stronger whereas the constant material has elements such as nickel which gives it the intensity it requires to dominate copper. Evaluation I perceive that this experiment was completed under fair conditions as this was kept a fair test at all times.I believe that repeating the experiment three times, had made this fair and given the accuracy which was needed. I had made sure that the materials were used to 2. 1 metres in length and had the same diameter. However, the errors which appeared in this experiment (uncertainties) are where when measuring the wire of the constantan or copper I had rounded up or down the value depending n whether it was greater then X. 5 or below.In my graphs, this is shown as these have been drawn in for average extension, so there is an uncertainty error of about 0.5mm. Another uncertainty spotted I believe is where I had calculated youngs modulus on the graph, I plotted a line of best fit. The line of best fit was drawn in hand by me, however this line can cause uncertainty as this is establish on human error and accuracy as everyone will have their own judgment and cognition when drawing the line of best fit. Furthermore, I can see that my line of best fit is not totally wrong as looking at the young modulus of copper which is 3*10 to the power of 10, and constantan 6. 40 to the power of 10.We can see that constantan youngs modulus was said to roughly double coppers youngs modulus value, and this is proven by these two figures given. We can see that these two figures are nearly double in difference therefore they seem to be correct. When measuring the wire with a metre stick I found there were an uncertainty of 0. 5mm, and an uncert ainty of 1% with the weights. The experiment in general had gone according to plan. Im merry with what I had found out through the results as I believe my prediction was correct and O.K. up by the results from the graph I had achieved.I believe that repeating the experiment three times meant that I had accurate results as from the average extension I plotted the graphs. Concluding this experiment I had found out that constant had the higher youngs modulus due to it being an alloy and containing the 40% of Nickel which gives it the strength property. Copper however, had been more flexible being a pure metal the atoms were easily dislocated and this resulted in copper breaking very easily as it had a small elastic limit. Improvements-IF TO DO IT AGAIN.BibliographyI had obtained information from the following resources o AS physics textbook I had found this source passing interesting and useful as much of the diagrams I had used came from this textbook, which explained the compariso n between the pure metal and alloy.This textbook had given much information which was relevant to this coursework. 8/10 o AS physics CD-ROM I had achieved the diagrams mostly from the CD ROM, this CD had many diagrams which were useful, however this did not contain much written information which was useful and could aid me with this coursework.6/10 o InternetI found that the information from these sources seemed very reliable and information I had gained, helped me understand the complex issues with the relation of physics to youngs modulus. I had obtained the mingled information I have included on the background information on the sensor from the following Internet sites o http//www. emsl. com/tensile_strength. html o http//www. encyclopedia. com/html/Y/Youngsmo. asp o http//hyperphysics. phy-astr. gsu. edu/hbase/permot3. html.