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Circular Motion and Centripetal Force, Lecture notes of Physics

A series of equations and calculations related to circular motion and centripetal force. It includes information on angular displacement, angular speed, and centripetal acceleration, as well as the forces involved in circular motion such as centripetal force and gravitational force. The document also discusses the relationship between centripetal force and gravity, and provides examples of how to calculate these forces.

Typology: Lecture notes

2022/2023

Available from 07/28/2023

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Download Circular Motion and Centripetal Force and more Lecture notes Physics in PDF only on Docsity! \ G. i C ircu\or mot-ion Ex__ -1 irne to, cbrY)pleJe af)e \ocrp = ~06 (o.+ con~to.nit s?eecA) u) a~~lar di5?la.ceme_r1t a.lier 10s? - _b_o~_ i bJ on8ular Sf~eol? CJ penod 2. {\.eiue_r)c y z ol) \ineQr -S.feecl a) _An0ubr Jisp\Qce(Yleot )_a ,e:an0ie movee,l ~ince. '6tnrt- _i ot «f-lT =') 0 = lT/1 ro.cl = bJ,. An~ulo.r s?e.€cl Jl-0 = L:16 -= ±Jt = 11 roJ $' ( ho,~ mon) rc,__J,ua~ \ b 'F '-IO=> ~0 ver s.e.cond J Cro ,, CJ 'Denod-.1T = L\ o or w = .B.lL -=1 T = ~11 -= ~1T -=- L,os. r , w lf/10 -=-.___ __, h-e.ctuenc\1,\t = ] _j_ ; 0.0:1-51-h -,- - - T i,o~ d) \·1 neo., 5Ve_ed_ "4 -= 2- -= Qirr -=- ~1f )( GO -= 311 ms'~ ~;kn~-, .J t T 462.0 .,,, I <:' w __ --, I.\ TY\ ~I !001-e v= ;, v =WI' mdliu~ \1f\ea.r O.f\~u\ci..r sre-eo.- s-p'eQcl Centri~toJ o.ccele.ronan T=4os fJ ----- ~ . rri=1500k~ I cen+ripe.1-rd .for-ce.. - o...-= ~Y2,,_-v, :• -t e.) o\.irechon ot the acceleration? P J accelera \ion 1 l -furce. ca.,u<:>i ni -the acce\a-Q hon~ h) c:aose oi +he_ b-ce --'7,(: _ alwo.~~ +owar6'~ v,.-v1 , , +he centre) h) +ric:hon be'lweer, 'tyes oncA \.he. roo..ol 1 cenrr·,~e+--o.l tree = the.. ~rce_ _-\ho:\- o.ct:5 to ¼.e.~'\> tY\e ob~ec,t mov1<1~ 1n o. c1rc:le. een \r i p.e la I all e \era tiDI'\ = a cc~\ eroJi m J. u e. m the_ - ce1Yr'ri?e\.o. ( ~,ce G,?_ Newton':') lo.w oi dro.vit-o.non M F Dniv~r~Q, oro.vitohcrio. \ CDf'\ S.r-o."l ( = t(;+ x 1611 NM'"kf) ( Gro..vitu hof"\al -he\ol H 1/,: ,/ 7t(\ m • (compare. a\wo..ys a+\ru.chve sma.\\ kst lY)o,.S.S / ~roidutional f'ie\J: "ne°'ilth ,\';J- \ units, \Jkf = the. \orce. per on·,+ mo..~-:, ex-perte.nc..e&. b1 c..._ s0'\a.l\ -po·1nt VY\0-..S~ yi\o..c.ecl. o+ +hu+- po"int (Oos,e+o Earth'~ ~ur~a.ce. +hi':) \s co.l\~cl \ \/ a.cc el er~ hon olu.e_ m iro..0t 4l" ancl ~,ve0 unih ms-1.) 1) Po\nt Y¥\o5S 2)Sphedcal mass H • r The_ helci -s\le°'ijth1 i-;, exoc-1--ly \-he. SQ.me · a.~ lo()1 ClS -\he poi1\-I: x ·1:':i ootsicle. the sphere\_ (=e. J;~~ce',~ ) E )( . Gro.v",to.-nona \ he\cl ~:/rre.n0-\h on 'Eos+h Sa~e1lld-e So.\el\i\e.-::: Q(') obje_c+ (CArhha)JjrnoonJ orh,hnd Q.(()L.)Ocl oroun..o Cl pla.!"et or -stur - - - ' . / 1c+o +he ,cenhe.& the. Earth) r ®r\1 \ f I force rJ 0,avi+y = cenlripetal brre = 1=(. - - - - -- - -1 :c; Hm = rnv'-, I rl. y ' I I ( Uo\e,I
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