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    https://www-wales.ch.cam.ac.uk/OPTIM.doc/node4.html
    29 Jun 2024: and N-N 1.0D0 -1.0D0 0.33333333333333D0 0.33333333333333D0 1.0D0 0.0D0 comment: coefficients A, B, C, D of 1 cosφ, 1 - cosφ, 1 cos 3φ and 1 ... cos(φ π/4) comment: for Helical, Extended and Turn residues in order, four per line 0.0D0 1.2D0 1.2D0
  3. 3 The Motion of Rigid Bodies�

    www.damtp.cam.ac.uk/user/tong/dynamics/dynhtml/S3.html
    27 Mar 2022: We write. 𝐞. a. ′′. =. R. 1. (. θ. ). a. b. 𝐞. b. ′. with. R. 1. (. θ. ). =. (. 1. 0. 0. 0. cos. θ. sin. θ. 0. -. ... V. eff. (. θ. ). =. I. 1. (. b. -. a. cos. θ. ). 2. 2. sin. 2. θ. M. g.
  4. doublependulum1.txt

    www3.eng.cam.ac.uk/~hemh1/doublependulum1.pdf
    12 Feb 2008: b=t1AL-t2;. V=-M1GB1cos(t1) - M2G(B2cos(t2) AAcos(ALt1));. T=0.5((I1M1B12)t1d.2 I2t2d.2 M2(B2t2d.sin(b)).2 M2(AAt1d. B2t2d.cos(b)).2);. ... i[0 -B1 -2B1 -B1 0 -AAcos(AL)];. line2=[AAsin(AL)[0 B2sin(t2-t1)]]. i[-AAcos(AL)[0 -B2cos(t2-t1)]];.
  5. Scattering from a pair of infinitely narrow slits

    https://www.doitpoms.ac.uk/tlplib/diffraction/example2.php
    The scattering density of two infinitely narrow slits separated by spacing b can be described using delta functions:. ... rm{i}}{{{bf{x}}sin 2theta } over lambda }} right){rm{d}}x} cr & {rm{ = 2}}{{rm{A}}_0}cos left( {{{pi b sin 2theta } over lambda }}
  6. 2009 Paper I A1. −1 ± √3. 2. 𝑥 ...

    https://www.robinson.cam.ac.uk/iar1/teaching/nst1a_maths_tripos_answers_2005-9.pdf
    2 Jan 2024: 3. (a) 3/𝑥; (b) cos 2𝑥 2𝑥 sin 2𝑥. 4. (a). ... 15. (b). 𝜋490; (c) 𝐴0 = 1; 𝐴𝑛 = 2(1)𝑛 cos 𝑛𝜋𝑥/(𝑛2𝜋2 1).
  7. 12 Jun 2024: x(, ) = ( cos , sin , ) (4.18). with a   b and 0  < 2. ... equation tells us that. µ0I =. Z. C. B dx =. Z 2. 0. d b() =) B(x) =µ0I. 2( sin , cos , 0).
  8. Analysis of Deformation Processes (all content)

    https://www.doitpoms.ac.uk/tlplib/metal-forming-3/printall.php
    left| {Os} right| = ) (frac{{2cos theta }}{{sin theta }}). (left| {qr} right| = ) (frac{1}{{tan theta }}) = (frac{{cos theta }}{{sin theta }}). Lengths in drawing of indent: (QR = SO =) (frac{b}{2}). (OR = ... kb ) (left{ {frac{1}{{sin theta cos theta }}
  9. Raman Spectroscopy (all content)

    https://www.doitpoms.ac.uk/tlplib/raman/printall.php
    Using the trigonometric identity:. [sin A times sin B = frac{{cos (A - B) - cos (A B)}}{2}]. ... vib}}}})t) - frac{{{alpha _0}{E_0}}}{2}cos (2pi ({upsilon _{rm{p}}} {nu _{{rm{vib}}}})t)].
  10. • Notched bar in tension

    https://www.doitpoms.ac.uk/tlplib/metal-forming-3/limit_example1.php
    Notched bar in tension. • Notched bar in tension. The plane strain condition is satisfied when breath, b » h, the depth of the bar. ... Let displacement along shear plane AB = δx. Then internal work done = ( {k.left| {AB} right|bdelta x} = ksqrt 2
  11. • Notched bar in plane bending

    https://www.doitpoms.ac.uk/tlplib/metal-forming-3/limit_example2.php
    kern 1pt} 2}}}left{ {{{sin }2}frac{alpha }{2} - 2frac{alpha }{2}cos frac{alpha }{2}sin frac{alpha }{2}} right}). = ... cos {raise0.5exhbox{$scriptstyle alpha $} kern-0.1em/kern-0.15em lower0.25exhbox{$scriptstyle 2$}}}} = {raise0.7exhbox{$1$}!

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