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  2. Oscillating Systems Natural SciencesPhysics Part 1A J. S. Biggins ...

    www.tcm.phy.cam.ac.uk/~jsb56/resources/oschandout.pdf
    24 Oct 2022: 7. 1. 0. 12. 0. 24. 02. 24. 0 1 2 3 4 5 6 7 8. ... 24. The vectorsum of thex1 andx2 phasors gives a third one representingx3, also spinning atω0.
  3. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMCurrentResearchTalk2022.pdf
    14 Mar 2022: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.
  4. LagrangianDynamics Engineering Part IBPaper 1 Lectures 9-16 J. S. ...

    www.tcm.phy.cam.ac.uk/~jsb56/resources/1B_Mechanics_handout.pdf
    24 Oct 2022: 23. 6.5 Second integral of the equation of motion. 24. 6.5.1 Second integral for the simple pendulum (non-examinable).
  5. DCE_2200031 1..23

    www.tcm.phy.cam.ac.uk/~gjc29/papers/MarkandayConduitConduitPurstlChristofidouChechikBaxterHeasonStone22.pdf
    11 Oct 2022: x (x1,…, xI) is a vector, here of size I 24, comprising the individual design variables andproperties.
  6. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/GrapheneCentreTalk2022.pdf
    13 May 2022: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.
  7. Intellegens_Apr22

    www.tcm.phy.cam.ac.uk/~tmw38/Whitehead22.pdf
    21 Nov 2022: beyond catalytic converters, including the design of metal alloys (15, 23), batteries (24), and pharmaceutical drugs (21). ... J. Conduit, Mater. Des., 2017, 131, 358. 24. M.-F. Ng, J.

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