first year em ppt.pdf
-
Upload
dhananjay-kumar -
Category
Documents
-
view
228 -
download
6
Transcript of first year em ppt.pdf
-
W2
T
-
Question 1Question-1
W1
W2Yaxis
W1
XaxisX axis
-
SolutionSolutionFree body diagrams of W1 and W2 arFreebodydiagramsofW1andW2ar
T T
W1Freebodydiagramforblock1
re as following:reasfollowing:
W2b d d f bl kFreebodydiagramforblock2
-
Equilibrium equationsEquilibrium equationss for block 1s for block 1
-
Equilibrium equationsEquilibrium equationss for block 2s for block 2
-
Question 2Question 2
-
Solutions:Solutions:-eebodydiagramsofW1andW2areasfollowing:
Freebodydiagramforblock1y g
Freebodydiagramforblock2
-
Equilibrium equationsEquilibrium equationss for block 1s for block 1
-
Equilibrium equationsEquilibrium equationss for block 2s for block 2
-
Question 3Question 3
T bl k f i ht W1 100TwoblocksareofweightW1=100andsupportsonitstopanotherblweightW2isattachedbyaninclineg yFindthemagnitudeofthehorizontblocktocauseslippingtoimpend.contact surface is 0 3contactsurfaceis0.3
3
4
3
00N t h i t l f00NrestsonahorizontalsurfaceockofweightW2=250N.TheedstringABtotheverticalwall.gtalforcePappliedtothelowerThecoefficientoffrictionforall
P
-
SolutionSolutionFreebodydiagramsofW1andW2ar
T
Freebodydiagramforblock2
reasfollowing:
P
Freebodydiagramforblock1
-
Equilibrium equationsEquilibrium equationss for block 2s for block 2
T
-
Equilibrium equationsEquilibrium equationss for block 1s for block 1
P
Free body diagram for block 1Freebodydiagramforblock1
-
Question 10Question-10
Wh t i th l f P i th tWhatisthevalueofPinthesystemimpend?Assumetheepulleyissmbetweentheothercontactsurface
h t th ti tmshowntocausethemotiontomoothandcoefficientoffrictionesis0.2
P
500N
P
-
IntroductionIntroduction Basic terms:Basicterms:
Motion :Abodyissaidtobeinmotionifitischangingitspo
DistanceandDisplacement :Distanceisthetotallengthofpathcoveredbythecalar quantitycalarquantity.Displacementisthelineardistancebetweenthepthasmagnitudeanddirectionthusitisvectorqua
peedandVelocity:peedisdefinedastherateofchangeofdistanceV l it i d fi d th t f h f di lVelocityisdefinedastherateofchangeofdisplace
to Dynamicsto Dynamics
ositionwithrespecttoareferencepoint.
bodytoreachfrompointAtopointB.Itisa
ointAandpointB.antity.
withtime.Speedisscalarquantity.t ith ti V l it i t titementwithtime.Velocityisvectorquantity.
-
Types of motionTypes of motionTranslation: Amotionissaidtobetranslationifa
ll l i i i l i i iaralleltoitsoriginalpositionatanytime.
Rectilinearmotion: Duringtranslationifthepathalled rectilinear motionalledrectilinearmotion
Curvilinearmotion: Duringtranslationifthepathalledcurvilinearmotion.
Rotation: Amotionissaidtobeinrotationalmotioncentriccircles.
Motioncanbeacombinationoftranslationandroorexamplemotionofawheelofacarisbothrota
astraightdrawnonthemovingbodyremains
tracedbyanypointinthebodyisstraight,itis
htracedbyanypointinthebodyiscurve,itis
ionifalltheparticleoftherigidbodymovein
otation.ationalandtranslational
-
Motion of body with uniforMotion of body with uniforrm(constant) accelerationrm(constant) acceleration
-
Question bank (10 mQuestion bank (10 mark)ark)
-
D Alemberts principlD Alembert s principlee
-
Work Energy methodWork Energy methoddd
-
Work Energy EquatioWork- Energy Equatioon for translationon for translation