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Shocking, the slow changes inHKM’s thin coat by HKM2 ...
www.damtp.cam.ac.uk/user/hinch/talks/hkm3.pdf23 May 2006: Solution. h1 = cos θ A(T ) cos(θ τ ) B(T ) sin(θ τ ). n>1. [An cos n(θ τ ) Bn sin n(θ τ )] eαn2(n21)τ. ... Secularity condition – resonant sin(θ τ ) and cos(θ τ ). d. dT. (. A. B. ). =. (. a b. b a. )(. -
N13LBb.dvi
www.damtp.cam.ac.uk/user/rrh/notes/N13LBb.pdf22 May 2006: 1. 0. dy cos(py) = ddp. (sin(p). p. ). =1. p2sin(p) 1. ... X(x) = A sin(αx) B cos(αx) ,. T(t) = D exp(κα2t). • -
This isa super vis or’ sco py ofth enote ...
www.damtp.cam.ac.uk/user/sjc1/teaching/AandG/notes.pdf11 Nov 2006: Then. z1z2 = r1r2 (cos θ1. cos θ2 sin θ1. sin θ2i (sin θ1. ... 1.30). Proof. From (1.25). cos nθ i sin nθ = ei (nθ). -
This isa super vis or’ sco py ofth enote ...
www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/notes.pdf28 Oct 2006: 2πnxL. ), (0.14a). where. an =2L. x0Lx0. f(x) cos(. 2πnxL. )dx, (0.14b). ... n=1. an cos(nπxL. ), (0.16a). where. an =2L. L0. ge(x) cos(nπxL. -
This isa super vis or’ sco py ofth enote ...
www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/Michaelmas/notes.pdf28 Oct 2006: 2πnxL. ), (0.14a). where. an =2L. x0Lx0. f(x) cos(. 2πnxL. )dx, (0.14b). ... n=1. an cos(nπxL. ), (0.16a). where. an =2L. L0. ge(x) cos(nπxL.
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