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4) Newton’s Law of Motion
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Newton’s Law of Motion
Newton’s Third Law:
When two objects interact, the forces on the
bodies from each other are always equal in
magnitude and opposite in direction.
Example:
10 and 5 Kg masses are attached at the ends of a
massless cord that goes over a massless and
frictionless pulley as shown, find the acceleration
of the system and the tension in the card.
If the two masses start from rest 10m above the
ground, find the maximum height reached by the
5Kg mass.
σ 𝑭 = ma
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Newton’s Law of Motion
Apply this law on m1
-m1g+T = −π’Ž′ a
m1g-T = m1a
m1 moves upward10m with
π’Ž
acceleration 3.27 𝟐
𝒔
its velocity
2ay = π’—πŸ − π’—πŸŽπŸ , π’—πŸŽ = 𝟎
𝒗 = πŸπ’‚π’š
π’Ž
𝒗 = πŸπ’™πŸ‘. πŸπŸ•π’™πŸπŸŽ = πŸ”πŸ“. πŸ’ =8.1
𝒔
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Newton’s Law of Motion
Now m2 is projected upward against
π’Ž
gravity with velocity 8.1
𝒔
-2gyο‚’= π’—πŸ − π’—πŸŽπŸ 𝒗 = 𝟎 , π’—πŸŽπŸ = πŸ”πŸ“. 𝟏
∴ height reached by m2is:
𝒉 = 𝟐𝟎 + πŸ‘. πŸ‘πŸ’ = πŸπŸ‘. πŸ‘πŸ’π’Ž
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Newton’s Law of Motion
Apply Newton’s second law on m2
𝑻 − π’ŽπŸ π’ˆ = π’ŽπŸ 𝒂
Add
+
π’ŽπŸ π’ˆ = π’ŽπŸ π’ˆ = π’ŽπŸ 𝒂 = π’ŽπŸ 𝒂
π’ˆ π’ŽπŸ − π’ŽπŸ = 𝒂 π’ŽπŸ − π’ŽπŸ
𝒂=
𝟏𝟎−πŸ“
πŸπŸ“
𝒙 πŸ—. πŸ– =
From equation 2
𝑻 − π’ŽπŸ π’ˆ + 𝒂
𝑻 = πŸ“ πŸ—. πŸ– + πŸ‘. πŸπŸ•
𝑻 = πŸ”πŸ“.35 N
πŸ—.πŸ–
πŸ‘
= πŸ‘. πŸπŸ•
π’Ž
π’”πŸ
= πŸ“π’™πŸπŸ‘. πŸŽπŸ•
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Newton’s Law of Motion
Solving problems involving application of Newton’s
second law:
1. Draw a clear diagram.
2. Show all forces acting on all objects.
3. Apply Newton’s second law on all objects
separately and obtain equations.
4. Solve equations simultaneously to find unknowns.
Friction it is the resistance force opposing motion
(sliding) of an object on a surface caused by the
bonding between the body and the surface.
Friction opposed motion.
𝒇
It does not cause motion.
Where 𝝁 is the coefficient of friction.
N is the normal force.
= 𝝁𝑡
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Newton’s Law of Motion
There are two types of friction:
1. Static friction 𝒇𝒔 = 𝝁𝒔 𝑡
where 𝒇𝒔 is the static frictional force and 𝝁𝒔 is
the coefficient of static friction and N is the
normal force.
2. Kinetic friction π’‡π’Œ = ππ’Œ 𝑡
where π’‡π’Œ is the kinetic friction and ππ’Œ is the
coefficient of kinetic friction and N is the normal
force.
𝒇𝒔 > π’‡π’Œ
𝝁𝒔 𝑡 > ππ’Œ 𝑡
𝝁𝒔 > ππ’Œ
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Newton’s Law of Motion
Normal force: N
It is the force applied by the surface on
the object, perpendicular to the
surface.
N
N=mg
f
mg
Example:
A 10Kg box on a rough horizontal surface is
pulled by a force F.
If the coefficient of static friction is 0.4 and
the coefficient of kinetic friction is 0.2.
Find the frictional force if F =10N, 20Nm
50N.
𝒇𝒔 = 𝝁𝒔 𝑡 = 𝝁𝒔 π’Žπ’ˆ = 𝟎. πŸ’π’™πŸπŸŽπ’™πŸ—. πŸ– = πŸ‘πŸ—. πŸπ‘΅
π’‡π’Œ = ππ’Œ 𝑡 = ππ’Œ π’Žπ’ˆ = 𝟎. πŸπ’™πŸπŸŽπ’™πŸ—. πŸ– = πŸπŸ—. πŸ”π‘΅
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Newton’s Law of Motion
a) 𝑭 = πŸπŸŽπ‘΅ < 𝒇𝒔
∴ 𝒕𝒉𝒆 𝒃𝒐𝒙 π’˜π’Šπ’π’ 𝒏𝒐𝒕 π’Žπ’π’—π’†
∴𝒂=𝟎
πšΊπ’‡ = 𝟎
𝑭−𝒇=𝟎
𝒇 = πŸπŸŽπ‘΅
b) πŸπŸŽπ‘΅ < 𝒇𝒔 , 𝒂 = 𝟎
πšΊπ’‡ = 𝟎
𝟐𝟎 − 𝒇 = 𝟎
𝒇 = πŸπŸŽπ‘΅
c) πŸ“πŸŽ > 𝒇𝒔
∴ The box moves and friction is kinetic
𝒇 = ππ’Œ π’Žπ’ˆ = πŸπŸ—. πŸ”π‘΅
πšΊπ’‡ = 𝐦𝐚
πŸ“πŸŽ − πŸπŸ—. πŸ” = 𝟏𝟎𝐚
𝐦
𝒂 = πŸ‘. πŸŽπŸ’ 𝟐
𝒔
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Newton’s Law of Motion
Example: A 10Kg box is pulled by a force 30N inclined
at an angle of 37ο‚° to the horizontal.
If the coefficient of friction is 0.2, find the normal
force and find the acceleration of the box.
πšΊπ‘­π’š = 𝟎
𝑡 + π‘­π’”π’Šπ’πœ½ − π’Žπ’ˆ = 𝟎
𝑡 = π’Žπ’ˆ − π‘­π’”π’Šπ’πœ½
𝑡 = πŸπŸŽπ’™πŸ—. πŸ– − πŸ‘πŸŽπ’™πŸŽ. πŸ” = πŸ–πŸŽπ‘΅
πšΊπ’™ = 𝐦𝐚
π‘­π’„π’π’”πœ½ − 𝒇 = π’Žπ’‚
π‘­π’„π’π’”πœ½ − 𝝁𝑡 = π’Žπ’‚
30x0.8-0.2x80=10a
24-16=10a
𝐦
a=0.8 𝟐
𝒔
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Newton’s Law of Motion
Example: In the figure m1=5kg
m2=10Kg
the coefficient of friction between m2 and the surface is 0.2
The pulley is massless and frictionless, find the acceleration
of the system and the tension in the string.
m1g−T = m1a 1
T−𝒇 = π’ŽπŸ 𝒂
T−𝒇 = π’ŽπŸ 𝒂
T−𝝁𝑡 = π’ŽπŸ 𝒂
𝑡 = π’ŽπŸ π’ˆ
T−ππ’ŽπŸ π’ˆ = π’ŽπŸ 𝒂
Add 1 + 2
m1g−ππ’ŽπŸ π’ˆ = π’ŽπŸ + π’ŽπŸ 𝒂
πŸ“π’ˆ−π’ˆ
πŸ’π’ˆ
πŸ’π’™πŸ—.πŸ–
π’Ž
m1g−ππ’ŽπŸ π’ˆ =
= =
= 2.6 𝟐
πŸπŸ“
πŸπŸ“
πŸπŸ“
𝒔
11
Newton’s Law of Motion
𝑻 = π’ŽπŸ π’ˆ − 𝒂
𝑻 = πŸ“ πŸ—. πŸ– − 𝟐. πŸ”
𝑻 = πŸ“π‘ΏπŸ•. 𝟐 = πŸ‘πŸ”π‘΅
Inclined plane
An object is moving down in inclined planed of
angle of inclination 𝜽 at constant speed find the
coefficient of friction, between the object and the
plane.
The weight of the object is resolved in two
directions along the inclined plane and
perpendicular to the plane. Acceleration along
these two directions is zero.
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Newton’s Law of Motion
πšΊπ‘­π‘΅ = 𝟎
𝐍 − 𝐦𝐠𝐜𝐨𝐬𝜽 = 𝟎
𝐍 = 𝐦𝐠𝐜𝐨𝐬𝜽
πšΊπ‘­ = 𝟎
𝐦𝐠𝐬𝐒𝐧𝜽 − 𝒇 = 𝟎
𝐦𝐠𝐬𝐒𝐧𝜽 − 𝝁𝑡 = 𝟎
𝐦𝐠𝐬𝐒𝐧𝜽 = 𝝁𝑡
ππ’Žπ’ˆπ’„π’π’”πœ½ = 𝐦𝐠𝐬𝐒𝐧𝜽
𝝁 = π’•π’‚π’πœ½
A mass m1 = 8Kg hangs free and it is connected by
a cord over a massless and frictionless pulley.
The other end is connected to 10Kg mass.
The coefficient of friction is 0.2.
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Newton’s Law of Motion
Find the acceleration of the system and the
tension in the cord.
πšΊπ‘­ =m1a
m1a – T= m1a
𝑻 − m2gsin −𝒇 = m2a
𝑻 − m2gsin −𝝁𝑡 = m2a
𝑻 − m2gsin −𝝁𝐦𝟐𝐠𝐜𝐨𝐬 = m2a
𝑨𝒅𝒅 1 + 2
π’Ž′g= m2gsin −𝝁𝐦𝟐𝐠𝐬𝐒𝐧 = π’ŽπŸ + π’ŽπŸ 𝒂
8g-πŸ”π’ˆ − 𝟏. πŸ”π’ˆ = πŸπŸ–π’‚
𝟎.πŸ’π’ˆ
𝟎.πŸ’ 𝒙 πŸ—.πŸ–
π’Ž
a=
=
=0.22 𝟐
πŸπŸ–
πŸπŸ–
𝒔
T= m1(g − a)
T= 8(9.8 − 0.22) = 8 x 9.58 = 76.64N
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Newton’s Law of Motion
Example:
A 10kg load is weighed in a lift with a spring balance.
Find the apparent weight of this load if the lift is:
a) Stationary
b) Moving up / down with constant speed.
π’Ž
c) Moving up with acceleration of 2 𝟐
𝒔
d) Moving down with acceleration of 9.8
W
𝐦
𝐬𝟐
mg
c) σ 𝑭 = π’Žπ’‚
a) a = 0
w - mg = ma
σ𝑭 = 0
w = m ( g + a ) = 10 (9.8 + 2) =10x 11.8 = 118 N
w - mg = 0
w = mg = 98 N
d) σ 𝑭 = −π’Žπ’‚
w - mg = - ma
b) a = 0
w = m (g – a)
σ𝑭 = 𝟎
w=0
w - mg = 0
w = mg = 98 N This weight less- ness, it happens at free fall.
Newton’s Law of Motion
Example:
In a theme park a boy stands with his back in contact with the
wall of a cylindrical shape.
Elevated room, that rotate about its axis.
When its velocity reaches a certain value the base of the
cylinder is dropped but the boy does not fall.
If the radius of the cylinder is r and the coefficient of friction
between the boy and the wall is 𝝁 , find this velocity.
If the boy does not fall frictional force must be equal to the
weight of the boy.
𝒇 = π’Žπ’ˆ
𝝁 N = mg
N=m
𝝁
𝐯=
π’Žπ’—πŸ
=
𝒓
π’“π’ˆ
𝝁
𝐯𝟐
𝐫
π’Žπ’ˆ
Newton’s Law of Motion
Example:
In a conical pendulum the cord is 𝐿 π‘š long and the angle the cord
makes with the vertical is πœƒ.
Find the period of pendulum.
The mass revolves in a horizontal circle the Centripetal force:
π’—πŸ
𝒓
𝑭𝒄 = m = T π’”π’Šπ’ 𝜽
mg = T 𝒄𝒐𝒔 𝜽
π’—πŸ
π’”π’Šπ’ 𝜽
=
π’“π’ˆ
𝒄𝒐𝒔 𝜽
L
r = L π’”π’Šπ’ 𝜽
T = 2𝝅
𝒍 π’„π’π’”πœ½
π’ˆ
T
πœƒ
π’—πŸ
π’”π’Šπ’ 𝜽
=
𝑳 𝐬𝐒𝐧 πœ½π’ˆ
𝒄𝒐𝒔 𝜽
𝟐
π‘³π’”π’Šπ’ 𝜽 π’ˆ
π’—πŸ = 𝒄𝒐𝒔 𝜽
π‘³π’ˆ
𝒗 = π’”π’Šπ’ 𝜽
𝒄𝒐𝒔 𝜽
πŸπ…π’“
πŸπ… 𝑳 π’”π’Šπ’ 𝜽
period t = 𝒗 =
π‘³π’ˆ
π’”π’Šπ’ 𝜽 𝒄𝒐𝒔 𝜽
mg
πœƒ
Newton’s Law of Motion
Newton’s First Law:
An object at rest remains at rest and
an object moving at constant speed
in a straight line remains so, unless
acted upon by an external force.
Newton’s Second Law:
The net force on an object is equal to
the product of the object’s mass and
its acceleration.
=
𝑭𝒏𝒆𝒕
π’Žπ’‚
σ 𝑭 = ma
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