lecture 7 ch5 f17 forces actually...
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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
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
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!
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)
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
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
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
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
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
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
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
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
Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov
The Major Forces
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
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
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.
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.
Department of Physics and Applied PhysicsPHYS.1410 Lecture 7 Danylov
Thank you