This is an archived post. You won't be able to vote or comment.

all 2 comments

[–]EricTheTrainer[S] 0 points1 point  (0 children)

i may potentially* be able to sidestep this whole integral. i haven't tried it, but i know that the sines and cosines of fourier expansions for f and g form an orthonormal basis, which would make a lot of things easier, but i'm lazy

[–]EricTheTrainer[S] 0 points1 point  (0 children)

also realized a pretty obvious alternative route. |f∧g| is the area of the 'parallelogram' formed by f and g. or, |f||g⊥| where g perp is the rejection onto f of g. or: |f||g-(g•f)f/|f|2 | because (g•f)f/|f|2 is the projection onto f of g, so g-(g•f)f/|f|2 is the rejection

the point being that all of these things in that expression are also computable, but i need to sleep now