Classifier Instance:

Anchor text: Lavoisier
Target Entity: Antoine_Lavoisier
Preceding Context: For a time-dependent process of heating of the calorimetric material, defined by a continuous joint progression P(t_1,t_2)\ of V(t)\ and T(t)\ , starting at time t_1\ and ending at time t_2\ , there can be calculated an accumulated quantity of heat delivered, \Delta Q(P(t_1,t_2))\, . This calculation is done by mathematical integration along the progression with respect to time. This is because increments of heat are 'additive'; but this does not mean that heat is a conservative quantity. The idea that heat was a conservative quantity was invented by
Succeeding Context: , and is called the 'caloric theory'; by the middle of the nineteenth century it was recognized as mistaken. Written with the symbol \Delta\ , the quantity \Delta Q(P(t_1,t_2))\, is not at all restricted to be an increment with very small values; this is in contrast with \delta Q\ .
Paragraph Title: Cumulation of heating
Source Page: Calorimetry

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