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Contents - Student subdomain for University of Bath

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180 CHAPTER 7. CALCULUS<br />

so θ1θ2<br />

θ 3<br />

= θ 1θ 2 θ 3 + 2xθ 1 θ 2 θ 3 − (2x + 1)θ 1 θ 2 θ 3<br />

θ 2 3<br />

= 0,<br />

is, unexpectedly, a constant c, and we should be considering<br />

Q(c)(x, θ 1 , θ 2 ), with θ 3 = cθ 1 θ 2 . This is perhaps not so surprising if we<br />

give the θ i their conventional meanings as exp(x) etc., and write L =<br />

Q(x, exp(x), exp(x 2 ), exp(x 2 + x)), where we can clearly write exp(x 2 +<br />

x) = exp(x 2 ) exp(x). Of course, θ 1 might equally well be 100 exp(x), etc.,<br />

so all we can deduce (in the language <strong>of</strong> differential algebra) is that the<br />

ratio is a constant c, not necessarily that c = 1.<br />

Equally, we could consider L = Q(x, θ 1 , θ 2 , θ 3 ) where θ 1 ′ = 1<br />

x−1 , θ′ 2 = 1<br />

and θ 3 ′ =<br />

2x<br />

x 2 −1 . Then<br />

x−1<br />

(θ 1 + θ 2 − θ 3 ) ′ = θ 1 ′ + θ 2 ′ − θ 3<br />

′<br />

=<br />

1<br />

x − 1 + 1<br />

x − 1 − 2x<br />

x 2 − 1<br />

= 0,<br />

and again we have a hidden constant c = θ 1 + θ 2 − θ 3 , and we should be<br />

considering Q(c)(x, θ 1 , θ 2 ), with θ 3 = θ 1 + θ 2 − c. Again, this is not so<br />

surprising if we give the θ i their conventional meanings as log(x − 1) etc.,<br />

where we can clearly write log(x 2 − 1) = log(x − 1) + logx+1). Of course,<br />

θ 1 might equally well be 100 + log(x − 1), etc., so all we can deduce (in<br />

the language <strong>of</strong> differential algebra) is that θ 1 + θ 2 − θ 3 is a constant c,<br />

not necessarily that c = 0.<br />

3. Hidden algebraics. It is possible to start from a field C, make k exponential<br />

and logarithmic extensions (Definition 82) <strong>of</strong> C(x) to create L, but have<br />

the transcendence degree <strong>of</strong> L over C(x) be less than k, i.e. <strong>for</strong> there<br />

to be unexpected algebraic elements <strong>of</strong> L, where we had thought they<br />

were transcendental. The obvious example is that √ x = exp( 1 2<br />

log x), but<br />

there are more subtle ones, such as the following variant <strong>of</strong> the exponential<br />

example from the previous item. Consider L = Q(x, θ 1 , θ 2 , θ 3 ) where<br />

θ 1 ′ = θ 1 , θ 2 ′ = 2xθ 2 and θ 3 ′ = (2x + 1 2 )θ 3. Then<br />

(<br />

θ1 θ2<br />

2 ) ′<br />

= θ ( )<br />

3 θ1 θ2<br />

2 ′<br />

− 2θ1 θ2θ 2 3<br />

′<br />

θ 2 3<br />

θ 3 3<br />

= θ 3θ ′ 1θ 2 2 + θ 3 θ 1 θ ′ 2θ 2 − 2θ 1 θ 2 θ ′ 3<br />

θ 3 3<br />

= θ 1θ 2 2θ 3 + 4xθ 1 θ 2 2θ 3 − 2(2x + 1 2 )θ 1θ 2 2θ 3<br />

θ 3 3<br />

= 0,<br />

so again we have an unexpected constant c. The correct rewriting now is<br />

Q(c)(x, θ 1 , θ 2 , θ 3 ), with θ 3 = √ cθ 1 θ 2 2 .

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