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Department of Physics and Applied Physics PHYS.1410 Lecture 7 Danylov Lecture 7 Chapter 5 Dynamics: Forces Course website: http://faculty.uml.edu/Andriy_Danylov/Teaching/PhysicsI Physics I

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Page 1: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

Lecture 7

Chapter 5

Dynamics: Forces

Course website:http://faculty.uml.edu/Andriy_Danylov/Teaching/PhysicsI

Physics I

Page 2: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

Today we are going to discuss:

Chapter 5: Some leftovers from rotational motion Ch.4 Force, Mass: Section 5.1

Weight—the Force of Gravity; and the Normal Force/Tension:Section 5.2-5.4

Page 3: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 6 Danylov

tanv

Angular velocity

Angular acceleration

Relationship between tangential and angular velocity

Relationship between tangential and angular acceleration

Definition of radians

Rotational Kinematic Quantities (Review)

But it is not the whole story about accelerations!

tana

Tangential acceleration atan is not enough to describe all changes in vtan!

Page 4: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 6 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 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 6 Danylov

=const

A particle moves with uniform circular motion if its angular velocity is constant.

Uniform circular motion

In this case, as the particle goes around a circle one time, its angular displacement is ∆ 2 during one period

∆ . Then , the angular velocity is related to the period of the motion:

The period T is related to the speed v:

tdtd

The time interval to complete one revolution is called the period, T.

T2

Page 6: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

A car is traveling around a curve at a steady 45 mph. Is the car accelerating?

A) YesB) No

ConcepTest Car on a curve

There is a Centripetal acceleration

Page 7: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

A car is traveling around a curve at a steady 45 mph. Which vector shows the direction of the car’s acceleration?

ConcepTest Car on a curve

There is a Centripetal acceleration pointing toward the center

Page 8: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

A car is slowing down as it drives over a circular hill.

Which of these is the acceleration vector at the highest point?

ConcepTest Car on a curve

tanaRa

totala

Acceleration (slowing down) of changing speed

Acceleration of changing direction

tanv

tanv

Page 9: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

Lecture 7

Chapter 5

Dynamics: Forces and

Newton’s Laws of MotionCourse website:

http://faculty.uml.edu/Andriy_Danylov/Teaching/PhysicsI

Physics I

Page 10: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 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 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

Force

A moving object needs a force to change its velocity

push pull

A force was introduced to describe interactions between two objects

A force is a push or pull

Force has magnitude and direction: VECTOR! To quantify a push or pull, we need to specify both magnitude and a direction.

An object at rest needs a force to get it moving

Page 12: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 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

Page 13: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

The Major Forces

Page 14: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 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.

The gravitational force pulls the cat down

Spring Force

Page 15: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

Normal Force• When an object sits on a table,

the table surface exerts an upward contact force on the object.

• This pushing force is directed perpendicular to the surface, and thus is called the normal force.

Alwaysperpendicular

A table is made of atoms joined together by molecular bonds which can be modeled as springs.Normal force is a result of many molecular springs being compressed ever so slightly.

End of the lecture

Page 16: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 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

When an object slides along a surface, the surface can exert a contact force which opposes the motion.

This is called kinetic friction.

The kinetic friction force is directed tangent to the surface, and opposite to the velocity of the object relative to the surface.

Kinetic friction tends to slow down the sliding motion of an object in contact with a surface.

Page 17: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

Tension Force

• When a string or rope or wire pulls on an object, it exerts a contact force called the tension force.

• The tension force is in the direction of the string or rope.

Page 18: LECTURE 7 Ch5 F17 Forces Actually coveredfaculty.uml.edu/.../LECTURE7Ch5F17ForcesActuallycovered.pdfPHYS.1410 Lecture 7 Danylov Today we are going to discuss: Chapter 5: Some leftovers

Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov

Thank you