Transcript PPTX

•
•
•
•
MedAdvance Internship Program
MedAdvance is an internship program based out of the Scientific Education and
Research Institute in Thornton, CO.
As a member you may lead and participate in Anatomy/Suture labs and Shadow
Doctors. In addition to these opportunities, the Scientific Education and Research
Institute is a medical device training facility that has doctors visit from all around
the world to learn about new medical technology. This gives interns the
opportunity to, not only meet health professionals from around the nation, but
also to become familiar with the latest medical technology!!!
MedAdvance is having an Open House on Thursday September 29th at 6-8:30pm
at the Scientific Education and Research Institute. The address is 9005 Grant st.
Thornton, CO 80229.
If you have any more questions about the internship or would like to RSVP for the
Open House, please feel free to contact [email protected].
Announcements
• CAPA Set #5 due Friday at 10 pm
• This week in Section 
Assignment #3: Forces, Newton’s Laws, Free-Body Diagrams
Print out and bring the assignment to your section…
• Complete reading all of Chapter 4
Step 1: Draw a free-body diagram
Note that “Normal Force” is
always Perpendicular
(i.e. normal) to the surface.
Fg = mg
In this case, it is not in the
opposite direction to the
gravitational force.
Step 2: Choose a coordinate system
Fg = mg
y
x
We could choose our “usual” axes.
However, we know that we will have motion
in both the x and y directions.
If we pick these rotated axes, we know that
the acceleration along y must be zero.
Step 3: Write down the equations
Σ Fx = m ax , Σ Fy = m ay
Fg = mg
Problem:
Fg doesn’t point in a
coordinate direction.
Must break it into its
x- and y-components.
Room Frequency BA
Clicker Question
F(gravity)y
F(gravity)x
90 – q
a 90
|F(gravity)| = mg
What is the angle a labeled above?
A) a = 90 degrees
B) a = q
C) a = 90 – q
D) Cannot be determined
Step 3: Write down the equations
Σ Fx = m ax , Σ Fy = m ay
N
Fx = mg sin(q)
Fy = N – mg cos(q)
Fg = mg
We also know that ay = 0,
there is no motion in that
direction.
Fy =may=0= N – mg cos(q)
Step 4: Solve the Equations
Fx  ma x  mg sin(q )
a x  g sin(q )
Fy  may  N  mg cos(q )
N
a y   g cos(q )  0
m
N  mg cos(q )
As expected,
maximum
acceleration if
straight down
(q=90 degrees),
ax = g.
Recall x-y
definition
Room Frequency BA
Clicker Question
A mass m accelerates down a frictionless inclined plane.
+y
-mg cos θ
θ
+x
θ
-
Which statement is true?
A) N < mg
0 = Fy = N – mg cos θ
B) N > mg
N = mg cos θ < mg
C) N = mg
Clicker Question
Room Frequency BA
The driver of a car parked on
a hill releases the brake and
puts the car in neutral
Let
N = normal force
F g = force of gravity
Which of the following is true? a = acceleration of the car.
A) A  a, E  N, B  F g
B) E  N, D  a,C  F g
C) E  N, D  Fg ,C  a
D) A  a, B  Fg , E  N
Room Frequency BA
Clicker Question
Two boxes with masses M and m are glued together.
Force F is applied to Box 1.
Force fc is the “contact force” that Box 1 exerts on Box 2.
M
fc
F
A)F = fc
m
Box 1
+x
Box 2
* Frictionless surface
B) F > fc
C) F < fc
D)Indeterminate from information given
Draw the free-body diagram for each box!
Box 1
F
Box 2
fc m
M
m
+x
F
M
fc
fc
m
What other forces are acting on either box?
Gravitational force down on both boxes, and
Normal force up on both boxes.
However, since there is no vertical motion
we sometimes do not bother to write them down.
What about Newton’s Third Law?
F
M
fc
fc
m
Apply Σ Fx = ma. (ignore vertical forces, no vertical motion)
F-fc = MaM
fc = mam
Since the boxes are fixed (glued) together  aM = am
aM=(F-fc)/M = am =fc/m
Fm  f c m  f c M
f c ( M  m)  Fm
m
fc 
F
M m
fc  F
Room Frequency BA
Clicker Question
Box 1
F
M
 m 
fc  
F

 M  m
Box 2
fc
m
+x
Assume Box 1 has a mass of 2 kg and Box 2 has a mass
of 1 kg. If a force of 1 N is applied to Box 1,
what is the contact force between the boxes?
A)
B)
C)
D)
E)
1N
½N
1/3 N
2N
3N
 1kg 
1
 m 
fc  
F
1N  N


 M  m
 2kg  1kg 
3
Room Frequency BA
Clicker Question
F
Box 1
F sinθ
θ
F cosθ
M
Previous equation:
Box 2
fc m
 m 
fc  
F

 M  m
m
+x
Assume a force F is applied to Box 1 at an angle θ from the
horizontal. What will be the equation for the contact force fc?
mM
A) fc  
F tan q

 m 
 m 
B) fc  
F sin q

 M  m
 m 
C) fc  
F cosq
 M  m 
 m(M  M ) 
D) fc  
 F cosq 
The horizontal component of F
produces horizontal motion.