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Influenced: Lucy Hall Winifred Judson

Biography

Dorothy Marshall was born on 12 December 1868 in London. She was on of the three daughters of Julian Marshall, connoisseur and collector, and Florence Ashton Thomas, musician and author.

Education

Marshall was educated at King Edward VI High School for Girls, Birmingham (KEVI) and went to Bedford College in 1886. Two years later, Marshall went on to study chemistry, physics and electrical technology at University College and graduated with a B.Sc. (third class honors, chemistry) in 1891. As a postgraduate student at University College until 1894, Marshall studied heats of vaporization of liquids. One of her three lengthy publications was co-authored with William Ramsay and the other one with Ernest Howard Griffiths, both appeared in 1896 and 1897. I In 1896, Marshall was appointed as Demonstrator at Girton College, Cambridge and promoted to Resident Lecturer in Chemistry a year later. Marshall left Girton in 1906 to become a Senior Science Lecturer position at Avery Hill College. Appointed as Acting Principal in 1907, she resigned due to "illness" in order to refuse the position. In 1908, she became the Senior Science Mistress of Huddersfield Municipal High School . In 1913 she moved south to Clapham High School to take a position as Chemistry Mistress. Like many other women in chemistry, Marshall started war work in 1916. She worked with the National Physical Laboratory as scientific research assistant until the end of her career.

Awards

As an excellent student, Marshall won several awards. She took three silver medals in analytical, organic, and general chemistry in 1888-1889. The following year, she won a prize in philosophy and logic. In 1889, she held a Tuffnell Scholarship.

Works

In her papers on the heats of vaporization of liquids, Marshall introduced a method of comparing directly the heats of evaporation of different liquids at their boiling points. The method used would conduct results that were not affected by errors in thermometer, changes in the specific heat of water, the capacity for heat of the calorimeter, and the loss or gain of heat by radiation. For setting up the apparatus, she wrote, "The liquid to be evaporated was contained in a small silver flask, connected with which was a spiral coil of silver tubing 18 feet in length. Both flask and spiral were within the calorimeter, and the water-vapour, after passing through the spiral, emerged from the apparatus at the temperature of the calorimeter. Surrounding the flask, and between it and the spiral, a coil of platinum-silver wire was arranged and flask, spiral, and coil were entirely immersed in a certain singularly limpid oil consisting of hydrocarbons only. "The calorimeter (which was filled to the roof with the oil, and the equality of temperature maintained by rapid stirring) was suspended by glass tubes within a steel chamber, whose walls were maintained at a constant temperature. So long, therefore, as the calorimeter and the surrounding walls were at equal temperatures, there was no loss or gain by radiation. If during an experiment the temperature of the surrounding walls changed, the method of experiment involved a corresponding change in the temperature of the calorimeter, and, therefore, some loss or gain of heat would be experienced. The apparatus was so designed that any such change in temperature was extremely small (in no case amounting to rhy°), yet, in order to estimate the loss or gain, it was necessary to know approximately the capacity for heat of the calorimeter and contents. Small differences between the temperature of the calorimeter and the surrounding walls would, during an experiment, be of no consequence provided that the oscillations were of such a nature that the mean temperature of the calorimeter was that of the surrounding space, and it will be found that this condition was fulfilled."

By using equation $L=[M/(m.e)].[(V.10^{8})/J]$

where

L= heat in calories

M = mass of liquid vaporized

m = mass of copper deposited

e= electrochemical equivalent of copper

V = declustering potential in volts

J = mechanical equivalent of heat

Marshall calculated that the value of $L$ for benzene is 94.4 cal