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Investigating Specific Heat As A Function Of Temp

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THE LATENT HEAT CALORIMETER

The specific heats of various solid samples were measured

Investigate specific heat as a function of temp 1. INTRODUCTION uses for latent heat, meteroreology, and specific heat, cooking pans

The specific heat capacity is defined as the amount of energy required to raise a substance by a temperature… tippler?. It is a fundamental property of materials and thus its determination has been given great importance throughout history.

Prior to thermodynamic research, the concept of heat transfer in materials was thought of as being a result of the containment of an invisible fluid called caloric. However

Before modern thermodynamics, it was thought that the transfer of heat was due to an invisible fluid …show more content…

He later established the general theory of specific heats by observing the amount of heat required to raise the temperature of different substances by the same temperature interval.

In 1819, the French physicists Pierre-Louis Dulong and Alexis-Thérèse Petit observed that the heat capacity per atom for metals were extremely similar within the temperature range of 300-500K. They determined heat capacities by surrounding the bulb of a mercury thermometer with a hot powdered sample and subsequently monitoring the cooling rate [2]. Since their experimental results for the heat capacities of different metals were close to that of an average, 3R, where R is the universal gas constant, it was concluded and accepted that the value of the heat capacity of an element is constant.

In 1892, Sir James Dewar performed experiments in the pursuit of determining the specific heat capacity of palladium. He measured the rise in the volume of vapour produced when placing the solid in boiling liquid. In doing so he invented the Dewar flask by placing a brass container within another container and depriving the gap between them of air, creating near-vacuum conditions.

In 1907 Albert Einstein made the first attempt to apply quantum theory to the molar heat capacity of solids [1] He made two assumptions: each atom in the lattice of a material is an independent quantum harmonic oscillator and that all vibrational modes

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