The integrated form of Kirchhoffs Law. A,H(T2) = A, H(T;) + A, Cp(T2 - T) where A,H(T;) and A,H(T2) are the reaction enthalpies at temperatures T;and Tz respectively and A,Cp is the heat capacity of the reaction works based on the assumption that: A. For extremely large temperature changes, the heat capacity of the reaction can be assumed independent of temperature. B. For extremely large temperature changes, the heat capacity of the reaction increases linearly as a function of temperature C. For extremely small temperature changes, the heat capacity of the reaction can be assumed independent of temperature D. For extremely small temperature changes, the heat capacity of the reaction increases linearly as a function of temperature O E. Both (B) and (C)

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The integrated form of Kirchhoff's Law: A, H(T2) = A,H(T;) + A,Cp(T2 - T)
where
A,H(T;) and 4,H(T2) are the reaction enthalpies at temperatures T; and T2 respectively and
A,Cp is the heat capacity of the reaction
works based on the assumption that:
A. For extremely large temperature changes, the heat capacity of the reaction can be
assumed independent of temperature.
B. For extremely large temperature changes, the heat capacity of the reaction increases
linearly as a function of temperature
C. For extremely small temperature changes, the heat capacity of the reaction can be
assumed independent of temperature
D. For extremely small temperature changes, the heat capacity of the reaction increases
linearly as a function of temperature
O E. Both (B) and (C)
Transcribed Image Text:The integrated form of Kirchhoff's Law: A, H(T2) = A,H(T;) + A,Cp(T2 - T) where A,H(T;) and 4,H(T2) are the reaction enthalpies at temperatures T; and T2 respectively and A,Cp is the heat capacity of the reaction works based on the assumption that: A. For extremely large temperature changes, the heat capacity of the reaction can be assumed independent of temperature. B. For extremely large temperature changes, the heat capacity of the reaction increases linearly as a function of temperature C. For extremely small temperature changes, the heat capacity of the reaction can be assumed independent of temperature D. For extremely small temperature changes, the heat capacity of the reaction increases linearly as a function of temperature O E. Both (B) and (C)
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