Published online by Cambridge University Press: 01 January 2022
In this paper I examine Salmon's response to two counterexamples to his conserved quantity (CQ) theory of causation. The first counterexample that I examine involves a time-wise gerrymandered world line of a series of patches of wall that is absorbing energy as a result of being illuminated in an astrodome. Salmon says that since the gerrymandered world line does not fulfill his “no-interaction requirement,” his CQ theory does not suffer from the counterexample. But I will argue that his response fails both at a theoretical level and at a practical level. In so doing I point out a problem for CQ theorists’ definition of a causal interaction. The second counterexample is concerned with a time-wise gerrymandered world line of a series of patches that are in shadow, in Hitchcock's well-known example. Salmon's response is based on a principle that Salmon thinks is derivable from the concept of a conserved quantity. However, I argue that the principle has a counterexample.
The ideas in this paper have come to me in discussion with Inkyo Chung. I am much indebted to him. I am also grateful to Bosuk Yoon, John McGuire, Inrae Cho, Sangwook Yi, Sungsu Kim, and two anonymous referees for their helpful advice. I owe a substantial debt to one referee, in particular, for his extensive and valuable comments.