Download - Chapter 4 Dynamics: Newton’s Laws of Motion
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Chapter 4
Dynamics: Newton’s Laws of Motion
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Units of Chapter 4
• Force
• Newton’s First Law of Motion
• Mass
• Newton’s Second Law of Motion
• Newton’s Third Law of Motion
• Weight – the Force of Gravity; and the Normal Force
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• Solving Problems with Newton’s Laws: Free-Body Diagrams• Applications Involving Friction, Inclines
• Problem Solving – A General Approach
Units of Chapter 4
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4-1 ForceA force is a push or pull. An object at rest needs a force to get it moving; a moving object needs a force to change its velocity.
The magnitude of a force can be measured using a spring scale.
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4-2 Newton’s First Law of Motion
Newton’s first law is often called the law of inertia.
Every object continues in its state of rest, or of uniform velocity in a straight line, as long as no
net force acts on it.
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4-2 Newton’s First Law of Motion
Inertial reference frames:
An inertial reference frame is one in which Newton’s first law is valid.
This excludes rotating and accelerating frames.
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4-3 Mass
Mass is the measure of inertia of an object. In the SI system, mass is measured in kilograms.
Mass is not weight:
Mass is a property of an object. Weight is the force exerted on that object by gravity.
If you go to the moon, whose gravitational acceleration is about 1/6 g, you will weigh much less. Your mass, however, will be the same.
mgW Find the weight of a 10 kg object.
NskgmsmkgW 98/98/8.910 22
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4.3 Newton’s Second Law of Motion
SI Unit for Force
22 smkg
smkg
This combination of units is called a newton (N).
1 Newton is about a quarter of a pound
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4-4 Newton’s Second Law of Motion
Newton’s second law is the relation between acceleration and force. Acceleration is proportional to force and inversely proportional to mass.
(4-1)
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4-4 Newton’s Second Law of Motion
Force is a vector, so is true along each coordinate axis.
The unit of force in the SI system is the newton (N).
Note that the pound is a unit of force, not of mass, and can therefore be equated to newtons but not to kilograms.
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4.3 Newton’s Second Law of Motion
A free-body-diagram is a diagram that represents the object and the forces that act on it.
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4.3 Newton’s Second Law of Motion
The net force in this case is:
275 N + 395 N – 560 N = +110 N
and is directed along the + x axis of the coordinate system.
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4.3 Newton’s Second Law of Motion
If the mass of the car is 1850 kg then, by Newton’s second law, the acceleration is
2sm059.0kg 1850N110
mF
a
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4-5 Newton’s Third Law of MotionAny time a force is exerted on an object, that force is caused by another object.
Newton’s third law:
Whenever one object exerts a force on a second object, the second exerts an equal force in the
opposite direction on the first.
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4-5 Newton’s Third Law of Motion
A key to the correct application of the third law is that the forces are exerted on different objects. Make sure you don’t use them as if they were acting on the same object.
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4-5 Newton’s Third Law of MotionRocket propulsion can also be explained using Newton’s third law: hot gases from combustion spew out of the tail of the rocket at high speeds. The reaction force is what propels the rocket.
Note that the rocket does not need anything to “push” against.
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4-5 Newton’s Third Law of MotionHelpful notation: the first subscript is the object that the force is being exerted on; the second is the source. This need not be done indefinitely, but is a good idea until you get used to dealing with these forces.
(4-2)
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4-6 Weight – the Force of Gravity; and the Normal Force
Weight is the force exerted on an object by gravity. Close to the surface of the Earth, where the gravitational force is nearly constant, the weight is:
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4-6 Weight – the Force of Gravity; and the Normal Force
An object at rest must have no net force on it. If it is sitting on a table, the force of gravity is still there; what other force is there?
The force exerted perpendicular to a surface iscalled the normal force. It is exactly as large as needed to balance the force from the object (if the required force gets too big, something breaks!)
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4-7 Solving Problems with Newton’s Laws – Free-Body Diagrams
1. Draw a sketch.
2. For one object, draw a free-body diagram, showing all the forces acting on the object. Make the magnitudes and directions as accurate as you can. Label each force. If there are multiple objects, draw a separate diagram for each one.
3. Resolve vectors into components.
4. Apply Newton’s second law to each component.
5. Solve.
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4-7 Solving Problems with Newton’s Laws – Free-Body Diagrams
When a cord or rope pulls on an object, it is said to be under tension, and the force it exerts is called a tension force.
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4-8 Applications Involving Friction, InclinesOn a microscopic scale, most surfaces are rough. The exact details are not yet known, but the force can be modeled in a simple way.
For kinetic – sliding – friction, we write:
is the coefficient of kinetic friction, and is different for every pair of surfaces.
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4-8 Applications Involving Friction, Inclines
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4-8 Applications Involving Friction, Inclines
Static friction is the frictional force between two surfaces that are not moving along each other. Static friction keeps objects on inclines from sliding, and keeps objects from moving when a force is first applied.
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The static frictional force increases as the applied force increases, until it reaches its maximum.
Then the object starts to move, and the kinetic frictional force takes over.
4-8 Applications Involving Friction, Inclines
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4.12 Nonequilibrium Application of Newton’s Laws of Motion
xx maF
yy maF
When an object is accelerating, it is not in equilibrium.
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4.11 Equilibrium Application of Newton’s Laws of Motion
Definition of EquilibriumAn object is in equilibrium when it has zero
acceleration.
0xF
0yF
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4-8 Applications Involving Friction, InclinesAn object sliding down an incline has three forces acting on it: the normal force, gravity, and the frictional force.
• The normal force is always perpendicular to the surface.
• The friction force is parallel to it.
• The gravitational force points down.
If the object is at rest, the forces are the same except that we use the static frictional force, and the sum of the forces is zero.
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4.9 Static and Kinetic Frictional Forces
The sled comes to a halt because the kinetic frictional forceopposes its motion and causes the sled to slow down.
Ffr
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4.9 Static and Kinetic Frictional Forces
Suppose the coefficient of kinetic friction is 0.05 and the total mass is 40kg. a)What is the kinetic frictional force?b)How far does the child slide before coming to a stop?
N20sm80.9kg4005.0 2
mgFF kNkfr
Ffr
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Child on a sled continuedHow far does the child slide before coming to a stop?
Calculate the deceleration of the child:
ΣFx = max
ax = ΣFx = -20N = -0.5m/s2 m 40kg
vf2 = vi
2 + 2aΔx
Δx = vf2 – vi
2 (0m/s)2 – (4m/s)2
= = 16m 2a 2(-0.5m/s2)
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4.12 Nonequilibrium Application of Newton’s Laws of Motion
The acceleration is along the x axis so 0ya
a) Find the net force acting on the barge If D=50,000N, R=35,000N, and T1=T2=20,000Nb) If the mass of the barge is 200,000kg, find the acceleration of the barge
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4.12 Nonequilibrium Application of Newton’s Laws of Motion
Force x component y component
1T
2T
D
R
0.30cos1T
0.30cos2T
0
0
D
R
0.30sin1T
0.30sin2T
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4.12 Nonequilibrium Application of Newton’s Laws of Motion
00.30sin0.30sin 21 TTFy
21 TT
x
x
ma
RDTTF
0.30cos0.30cos 21
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A student drags a crate having a 50kg mass by a rope hooked to it. The student pulls with a force 150N at an angle of 30°. The coefficient of kinetic friction between the crate and floor is 0.25.a)Calculate Ffr
b)Find the acceleration of the cratec)What happens if the coefficient of friction rises to 0.4?
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Inclined Plane Problem
For m1 (taking up the plane as positive)ΣFx = T - W1sin30 - Ffr = m1a ΣFy = FN - W1cos30 = 0 = T - W1sin30 - W1cos30 = m1a FN = W1cos30
For m2 (taking down as positive)ΣFy = W2 – T = m2a
Take the direction of motion as positive and use Newton’s Second Law to write equations
M1 = 8kgM2 = 22kg = 0.2
W = mgW1 = (8kg)(9.8m/s2) = 78.4N W2 = (22kg)(9.8m/s2)= 215.6N
Ffr
Ffr
+
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Inclined Plane ProblemT - W1sin30 - W1cos30 = m1a eq. 1
W2 – T = m2a eq. 2
W2 - W1sin30 - W1cos30 = m1a + m2a
W2 - W1sin30 - W1cos30 - = a m1 + m2
215.6N – (78.4N)(sin 30)) - (.2(78.4N)(cos30)) = 5.43m/s2
8kg + 22kg
M1 = 8kgM2 = 22kg
W = mgW1 = (8kg)(9.8m/s2) = 78.4N W2 = (22kg)(9.8m/s2)= 215.6N
Solve for T using eq. 2
215.6N – T = (22kg)(5.43m/s2)
T = 96.2N
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Summary of Chapter 4• Newton’s first law: If the net force on an object is zero, it will remain either at rest or moving in a straight line at constant speed.
• Newton’s second law:
• Newton’s third law:
• Weight is the gravitational force on an object.
• The frictional force can be written:
(kinetic friction) or (static friction)
• Free-body diagrams are essential for problem-solving
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4-9 Problem Solving – A General Approach1. Read the problem carefully; then read it again.
2. Draw a sketch, and then a free-body diagram.
3. Choose a convenient coordinate system.
4. List the known and unknown quantities; find relationships between the knowns and the unknowns.
5. Estimate the answer.
6. Solve the problem without putting in any numbers (algebraically); once you are satisfied, put the numbers in.
7. Keep track of dimensions.
8. Make sure your answer is reasonable.