lecture 7 ch5 f18 forces
TRANSCRIPT
![Page 1: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/1.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Lecture 7Chapter 5
Dynamics: Forces and Newton’s Laws of Motion
Physics I
Team work of force demonstration
Course website:https://sites.uml.edu/andriy-danylov/teaching/physics-i/
![Page 2: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/2.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Today we are going to discuss:
Chapter 5:
Some leftovers from rotational motion Force, Mass: Section 5.1
Weight—the Force of Gravity; and the Normal Force/Tension:Section 5.2-5.4
Newton’s First Law of Motion: Section 5.6 Newton’s Second Law of Motion: Section 5.5 Free-Body Diagram: Section 5.7
![Page 3: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/3.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
tanv
Rotational Kinematic Quantities (Review)
Angular descriptionof rotation
Linear descriptionof rotation
Connecting equations
Let’s look at accelerations
![Page 4: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/4.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Accelerations
tanv
r
aR
tana
totala
Tangential acceleration atan is always tangent to the circle.
Rantotal aaa t
22t Rantotal aaa
Finally, any object that is undergoing circular motionexperiences two accelerations: centripetal and tangential.Total
acceleration:
;tanv
atan results from a change in the magnitude of vtan
aR (centripetal acceleration)results from a change in the direction of vtan
Centripetal acceleration aRalways points toward the
center of the circle.
aR
aR
In uniform circular motion (=const), although the speed is constant, there is a centripetal acceleration because the direction of the velocity vector is always changing.
(two servants of a king)
![Page 5: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/5.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
A particle moves with uniform circular motion if its angular velocity (and vtan) is constant.
Let’s relate the period and
The period T is related to the speed vtan:
The time interval to complete one revolution is called the period, T.
∙
1 2 2
2 2or
ThatishowtheperiodTisrelatedtotheangularvelocity
![Page 6: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/6.jpg)
Acaristravelingaroundacircularcurveatasteady45mph.Isthecaraccelerating?
A) YesB) No
ConcepTest Car on a curve
ThereisaCentripetalaccelerationpointingtowardthecenter
raatan=0 since vtan=45mph (const)
![Page 7: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/7.jpg)
Acarisslowingdownasitdrivesoveracircularhill.Whichoftheseisthetotalaccelerationvectoratthehighestpoint?
ConcepTest Car on a curve
tanara
totala
Sincethetangentialvelocityisslowing,atan pointsintheoppositedirectionrelativetovtan
Accelerationofchangingdirection
tanv
tanvtanv
![Page 8: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/8.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Rotational Kinematic Quantities (Review)
Angular descriptionof rotation
Linear descriptionof rotation
Connecting equations
Kinematics is over
tanv
aR
![Page 9: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/9.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Lecture 7Chapter 5
Dynamics: Forces and Newton’s Laws of Motion
Physics I
Team work of force demonstration
Course website:https://sites.uml.edu/andriy-danylov/teaching/physics-i/
![Page 10: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/10.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Transition from Kinematics to Dynamics
In Kinematics we studiedHOW things move
Motion Forces
Motion Forces
Now in Dynamics we will study WHY things move
It’s time to complicate life
![Page 11: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/11.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Force
push pull
AforcewasintroducedinPhysicstodescribeinteractionsbetweentwoobjects
A force is a push or pull
Forcehasmagnitudeanddirection:VECTOR!Toquantifyapushorpull,weneedtospecifybothmagnitudeandadirection.
![Page 12: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/12.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
There are two types of forces
Contact forces:forces that act on an object by
touching it at a point of contact.
Non-contact forces (Long-range forces): forces that act on an object
without physical contact (gravity).
The bat must touch the ball to hit it.
Frictional ForceTension ForceNormal ForceSpring Force
GravityElectric force
Magnetic force
My foot must touchto share fun through
a contact force
![Page 13: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/13.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
The Major Forces
![Page 14: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/14.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
A spring can either push (when compressed) or pull (when stretched).
The pull of a planet on an object near the surface is called the gravitational force. It comes from the entire planet
Gravity acts on all objects, whether moving or at rest.The gravitational force vector always points vertically downward.
Spring ForceGravity
![Page 15: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/15.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
NormalForce
• Whenanobjectsitsonatable,thetablesurfaceexertsanupwardcontactforceontheobject.
• Thispushingforceisdirectedperpendicular tothesurface,andthusiscalledthenormalforce.
Alwaysperpendicular
Atableismadeofatomsjoinedtogetherbymolecularbondswhichcanbemodeledassprings.Normalforceisaresultofmanymolecularspringsbeingcompressedeversoslightly.
![Page 16: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/16.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Static friction is the contact force that keeps an object “stuck” on a surface, and prevents relative motion.
The static friction force is directed tangent to the surface.
Static friction points opposite the direction in which the object would move if there were no static friction.
Friction Force
Whenanobjectslidesalongasurface,thesurfacecanexertacontactforcewhichopposesthemotion.This is called kinetic friction.
Thekineticfrictionforceisdirectedtangenttothesurface,andoppositetothevelocityoftheobjectrelativetothesurface.Kinetic friction tends to slow down the sliding motion of an object in contact with a surface.
Kinetic friction Static friction
![Page 17: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/17.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Tension Force
• Whenastringorropeorwirepullsonanobject,itexertsacontactforcecalledthetensionforce.
• Thetensionforceactsalongtheropeandawayfromtheobjectinquestion.
![Page 18: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/18.jpg)
Abobsledderpusheshersledacrosshorizontalsnowtogetitgoing,thenjumpsin.Aftershejumpsin,thesledgraduallyslowstoahalt.Whatforcesactonthesledjustaftershe’sjumpedin?
ConcepTest Forces A)Gravityandkineticfriction
B)Gravityandanormalforce.
C)Gravityandtheforceofthepush.
D)Gravity,anormalforce,andkineticfriction.
E)Gravity,anormalforce,kineticfriction,andtheforceofthepush.
One of the key points:
the object has no memory of forces thatmay have been exerted at earlier times.It only responds to forces acting on it atthis instant. Once the woman stoppedpushing, her force disappeared from ourdiagram. An effect of that force is in adifferent velocity.
End of the class
![Page 19: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/19.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Principle of superposition
F1F2
F3
+ +
If multiple forces are present, the net force on an object is given by the vector sum of all the forces
F1
F2
F3
![Page 20: LECTURE 7 Ch5 F18 Forces](https://reader033.vdocument.in/reader033/viewer/2022061513/629f01f2444891282d27da03/html5/thumbnails/20.jpg)
DepartmentofPhysicsandAppliedPhysicsPHYS.1410Lecture7A.Danylov
Thank you