Johnny Tremain essays

Johnny Tremain essays In the face of adversity, our character can change extremely. Ester Forbes writes about this example in her book, Johnny Tremain, which takes place in Boston, Massachusetts, in 1773, during the revolutionary war. As we read the book, we see Johnny facing many obstacles and problems causing him to start a different and new life. However, Johnny encounters bad luck, but he learns to understand his problems better and accepts them. Johnny Tremain starts out as a arrogant boy who one day wants to be a silversmith. Unfortunately one day, he was in a silversmiths shop and injures his hand from burning hot silver, which causes him to deeply damage his hand. He no longer could be a silversmith. Of course, Johnny was deeply ashamed of his hand and always hid it from the world. Gradually, he then has the courage to show his hand. Johnny felt no more shame over his burned hand -pg. 254- Later, Johnny comes across the printing press of the Boston Observer while looking for another job. While there, Johnny gets the chance to meet Rab and immediately makes friend with him. Johnny than notice that he enjoyed telling Rab stories about his hand, but with nonce of the belligerent arrogance which he had been answering the questions kind people had put to him. - page 146- This is the first time since the accident he felt able to stand aside from his problems to see himself. - pg. 255- Rab turns his life around and shows him another world that he could and must face. Without Rab, Johnny might not have believed in himself and achieved much. A big influence on Johnnys life were his friends. As previously mentioned, Rab contributed much to Johnnys life. Rab has shown Johnny that he could achieve anything he waned too. Rab taught Johnny how to ride Goblin, gets ...

History of the Thermometer and Lord Kelvin

History of the Thermometer and Lord Kelvin Lord Kelvin invented the Kelvin Scale in 1848 used on thermometers. The Kelvin Scale measures the ultimate extremes of hot and cold. Kelvin developed the idea of absolute temperature, what is called the Second Law of Thermodynamics, and developed the dynamical theory of heat. In the 19th century, scientists were researching what was the lowest temperature possible. The Kelvin scale uses the same units as the Celcius scale, but it starts at ABSOLUTE ZERO, the temperature at which everything including air freezes solid. Absolute zero is O K, which is - 273 °C degrees Celsius. Lord Kelvin - Biography Sir William Thomson, Baron Kelvin of Largs, Lord Kelvin of Scotland (1824 - 1907) studied at Cambridge University, was a champion rower, and later became a Professor of Natural Philosophy at the University of Glasgow. Among his other achievements was the 1852 discovery of the Joule-Thomson Effect of gasses and his work on the first transatlantic telegraph cable (for which he was knighted), and his inventing of the mirror galvanometer used in cable signaling, the siphon recorder, the mechanical tide predictor, an improved ships compass. Extracts from: Philosophical Magazine October 1848 Cambridge University Press, 1882 ...The characteristic property of the scale which I now propose is, that all degrees have the same value; that is, that a unit of heat descending from a body A at the temperature T ° of this scale, to a body B at the temperature (T-1) °, would give out the same mechanical effect, whatever be the number T. This may justly be termed an absolute scale since its characteristic is quite independent of the physical properties of any specific substance. To compare this scale with that of the air-thermometer, the values (according to the principle of estimation stated above) of degrees of the air-thermometer must be known. Now an expression, obtained by Carnot from the consideration of his ideal steam-engine, enables us to calculate these values when the latent heat of a given volume and the pressure of saturated vapor at any temperature are experimentally determined. The determination of these elements is the principal object of Regnaults great work, already referred to, but, at present, his researches are not complete. In the first part, which alone has been as yet published, the latent heats of a given weight, and the pressures of saturated vapour at all temperatures between 0 ° and 230 ° (Cent. of the air-thermometer), have been ascertained; but it would be necessary in addition to know the densities of saturated vapour at different temperatures, to enable us to determine the latent heat of a given volume at any temperature. M. Regnault announces his intention of instituting researches for this object; but till the results are made known, we have no way of completing the data necessary for the present problem, except by estimating the density of saturated vapour at any temperature (the corresponding pressure being known by Regnaults researches already published) according to the approximate laws of compressibility and expansion (the laws of Mariotte and Gay-Lussac, or Boyle and Dalton). Within the limits of natural temperature in ordinary climates, the density of saturated vapour is actually found by Regnault (Études Hydromà ©triques in the Annales de Chimie) to verify very closely these laws; and we have reasons to believe from experiments which have been made by Gay-Lussac and others, that as high as the temperature 100 ° there can be no considerable deviation; but our estimate of the density of saturated vapour, founded on these laws, may be very erroneous at such high temperatures at 230 °. Hence a completely satisfactory calculation of the proposed scale cannot be made till after the additional experimental data shall have been obtained; but with the data which we actually possess, we may make an approximate comparison of the new scale with that of the air-thermometer, which at least between 0 ° and 100 ° will be tolerably satisfactory. The labour of performing the necessary calculations for effecting a comparison of the proposed scale with that of the air-thermometer, between the limits of 0 ° and 230 ° of the latter, has been kindly undertaken by Mr. William Steele, lately of Glasgow College, now of St. Peters College, Cambridge. His results in tabulated forms were laid before the Society, with a diagram, in which the comparison between the two scales is represented graphically. In the first table, the amounts of mechanical effect due to the descent of a unit of heat through the successive degrees of the air-thermometer are exhibited. The unit of heat adopted is the quantity necessary to elevate the temperature of a kilogramme of water from 0 ° to 1 ° of the air-thermometer; and the unit of mechanical effect is a metre-kilogramme; that is, a kilogramme raised a metre high. In the second table, the temperatures according to the proposed scale, which correspond to the different degrees of the air-thermometer from 0 ° to 230 °, are exhibited. The arbitrary points which coincide on the two scales are 0 ° and 100 °. If we add together the first hundred numbers given in the first table, we find 135.7 for the amount of work due to a unit of heat descending from a body A at 100 ° to B at 0 °. Now 79 such units of heat would, according to Dr. Black (his result being very slightly corrected by Regnault), melt a kilogramme of ice. Hence if the heat necessary to melt a pound of ice be now taken as unity, and if a metre-pound be taken as the unit of mechanical effect, the amount of work to be obtained by the descent of a unit of heat from 100 ° to 0 ° is 79x135.7, or 10,700 nearly. This is the same as 35,100 foot-pounds, which is a little more than the work of a one-horse-power engine (33,000 foot pounds) in a minute; and consequently, if we had a steam-engine working with perfect economy at one-horse-power, the boiler being at the temperature 100 °, and the condenser kept at 0 ° by a constant supply of ice, rather less than a pound of ice would be melted in a minute.