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Newton’s First & Second Law
AP Physics C
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Facts about FORCE• Unit is the Newton(N) or pound (lb)• Is by definition a ….. push or a pull• Can exist during physical contact(Tension, Friction, Applied Force)• Can exist with NO physical contact• called Fundamental Forces
(gravitational, electric, nuclear FIELDS)
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Newton’s First Law – The Law of Inertia
INERTIA – the more of it you have, the harder it is to get you moving.
Modern definition: a quantity of matter, also called … MASS. Unit for MASS = kilogram. NOTE: MASS and WEIGHT are NOT the same
thing. MASS never changes when an object moves
to a different planet.
mgW
Weight is a force due to Gravity. It is how your MASS is effected by gravity.
What is the weight of an 85.3-kg person on earth? On Mars=3.2 m/s/s)?
NWNWmgW
MARS 96.272)2.3)(3.85(94.835)8.9)(3.85(
Inerte in Galileo’s Italian meant “lazy”
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Newton’s First Law is really Galileo’s Law of Inertia
An object in motion remains in motion in a straight line and at a constant speed OR an object at rest remains at rest, UNLESS acted upon by an EXTERNAL (unbalanced) force.
The bottom line: There is NO ACCELERATION (no change in velocity) unless a force acts, but you can have MOTION even if there is NO force acting.
“Common sense” told us the opposite for generations, so inertia was a real intellectual breakthrough.
EQUILIBRIUM is when there are either NO FORCES acting or those that are acting all cancel each other out.
00 Facc
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Free Body DiagramsA pictorial representation of forces complete with
labels.
W1,Fg1 or m1g
• Weight(mg) – Always drawn from the center, straight down
• Force Normal(FN) – A surface force always drawn perpendicular to a surface.
• Tension(T or FT) – force in ropes and always drawn AWAY from object.
• Friction(Ff)- Always drawn opposing the motion.
m2g
T
TFN
Ff
It helps if you first circle the object you are analyzing, and labe only the forces acting ON IT. Other than gravity, these forces must involve physical contact.
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Free Body Diagrams
mg
FNFf
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N.F.L and EquilibriumSince the Fnet = 0, a system moving at a
constant speed or at rest MUST be at EQUILIBRIUM.
TIPS for solving problems• Draw a FBD• Resolve anything at angles into
COMPONENTS• Write equations of equilibrium• Solve for unknowns
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ExampleA 10-kg box is being pulled across the table to the
right at a constant speed with a force of 50N.a) Calculate the Force of Frictionb) Calculate the Force Normal
mg
FN Fa
Ff
NFF fa 50
NFmg n 98)8.9)(10(
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ExampleSuppose the same box is now pulled at an angle of 30
degrees above the horizontal.a) Calculate the Force of Friction
b) Calculate the Force Normal
mg
FN Fa
Ff30
NFFNFF
axf
aax
3.433.4330cos50cos
Fax
Fay
NF
FmgF
mgFFmgF
N
ayN
ayN
N
73
30sin50)8.9)(10(
!
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What if it is NOT at Equilibrium?
If an object is NOT at rest or moving at a constant speed, that means the FORCES are UNBALANCED. One force(s) in a certain direction overpowers the others.
THEN THE OBJECT WILL….. ACCELERATE.
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Newton’s Second LawThe acceleration of an object is directly
proportional to the NET FORCE and inversely proportional to the mass.
maFmFa
maFa
NETNET
NET
1 FFNET
Tips:• Draw an FBD• Resolve vectors into components• Write equations of motion by adding
and subtracting vectors to find the NET FORCE. Always write larger force – smaller force.
• Solve for any unknowns
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ExampleA 10-kg box is being pulled across the table to
the right by a rope with an applied force of 50N. Calculate the acceleration of the box if a 12 N frictional force acts upon it.
mg
FN Fa
Ff
2/8.3
101250
sma
a
maFFmaF
fa
Net
In which
direction, is this object accelerating?
The X direction!
So N.S.L. is worked out using the forces in the “x” direction only
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Example
m1g
m2g
T
TFN
A mass, m1 = 3.00kg, is resting on a frictionless horizontal table is connected to a cable that passes over a pulley and then is fastened to a hanging mass, m2 = 11.0 kg as shown below. Find the acceleration of each mass and the tension in the cable.
amTamTgm
maFNet
1
22
2
21
2
122
122
212
/7.714
)8.9)(11()(
smmmgma
mmagmamamgmamamgm
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Now that we know a we can find F
amTamTgm
maFNet
1
22
NT 1.23)7.7)(3(
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RunRiseSlope
maFmaF NET
Net
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Where does the calculus fit in?
dtxdm
dtdvmamF
2
First derivative
Second derivative
DON’T WORRY ABOUT THE STUFF ON THIS SLIDE OR THE NEXT FOR NOW.
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Where does the calculus fit in?
dtxdm
dtdvmamF
2
220.03)( tttv
There could be situations where you are given a displacement function or velocity function. The derivative will need to be taken once or twice in order to get the acceleration. Here is an example.
You are standing on a bathroom scale in an elevator in a tall building. Your mass is 72-kg. The elevator starts from rest and travels upward with a speed that varies with time according to:
When t = 4.0s , what is the reading on the bathroom scale (a.k.a. Force Normal)?
)4(40.03)4(
40.03)20.03( 2
a
tdt
ttddtdva
4.6 m/s/s
)6.4)(72()8.9)(72(N
NN
net
FmgmaFmamgF
maF
1036.8 N
DON’T WORRY ABOUT THE STUFF ON THIS SLIDE UNTIL NOVEMBER
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m1g
m2g
T
TFN
A mass, m1 = 3.00kg, is resting on a frictionless horizontal table is connected to a cable that passes over a pulley and then is fastened to a hanging mass, m2 = 11.0 kg as shown below. Find the acceleration of each mass and the tension in the cable.