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Transcript
Lecture 9
Potential Energy and Conservation
of Energy
(HR&W, Chapter 8)
http://web.njit.edu/~sirenko/
Physics 105 Summer 2006
Lecture 9
Andrei Sirenko, NJIT
1
Lecture 9
Andrei Sirenko, NJIT
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Power
Average Power
Units: Watts
Instantaneous Power
Sample Problem 77-10:
10: Two constant forces F1 and
F2 acting on a box as the box slides rightward across
a frictionless floor. Force F1 is horizontal, with
magnitude 2.0 N,
60º
N, force F2 is angled upward by 60º
to the floor and has a magnitude of 4.0 N.
N. The speed
v of the box at a certain instant is 3.0 m/s.
m/s.
a) What is the power due to each force acting
on the box? Is the net power changing at that
instant?
P=
Lecture 9
b) If the magnitude F2 is, instead, 6.0 N,
N, what is
now the net power, and is it changing?
½*60kg*(5m/s)2
Andrei Sirenko, NJIT
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Lecture 9
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• Potential Energy and Conservation of
Energy
• Conservative Forces
• Gravitational and Elastic Potential Energy
• Conservation of (Mechanical) Energy
• Potential Energy Curve
• External and Internal Forces
Work and Potential Energy
Potential Energy
General Form:
Gravitational Potential Energy
Elastic Potential Energy
Lecture 9
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Energy and Work
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Conservation of Mechanical Energy
Kinetic energy
Mechanical Energy
Conservation of
Mechanical Energy
Units of Work and Energy: Joule
Work done by a constant force
In an isolated system where
only conservative forces cause
energy changes, the kinetic
and potential energy can
change, but their sum, the
mechanical energy Emec of the
system, cannot change.
Work–kinetic energy theorem
Lecture 9
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Lecture 9
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Kinetic Energy:
Kinetic Energy:
Potential Energy:
Potential Energy:
• Gravitation:
• Gravitation:
• Elastic (due to spring force):
• Elastic (due to spring force):
1
1
mg
Lecture 9
y
UÆK
UÅÆK
Conservation of
Mechanical Energy
2
K=0
Andrei Sirenko, NJIT
9
U=0
2
Conservation of
Mechanical Energy
Lecture 9
Andrei Sirenko, NJIT
Sample Problem
Path Independence of
Conservative Forces
A circus beagle of mass
m = 6.0 kg runs onto the left
end of a curved ramp with
speed v0 = 7.8 m/s at height
y0 = 8.5 m above the floor. It
then slides to the right and
comes to a momentary stop
when it reaches a height
y = 11.1 m from the floor.
The ramp is not frictionless.
What is the increase ∆Eth in
the thermal energy of the
beagle and the ramp because
of the sliding?
Sample Problem 8-1: A 2.0 kg block slides
along a frictionless track from a to point b. The
block travels through a total distance of 2.0 m,
and a net vertical distance of 0.8 m. How much
work is done on the block by the gravitational
force?
Lecture 9
Andrei Sirenko, NJIT
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Lecture 9
Andrei Sirenko, NJIT
Answer: 30J
12
Examples for Energy Conservation
+
+
Problems:
Kinetic Energy changes
Gravitational Potential Energy
Elastic Potential Energy
__________________________________
Total Mechanical Energy = Const.
Kf - Ki = W = mgy - |Wfriction|
Wfriction
Ef - Ei = Kf –(Ki + mgy) = -|Wfriction|=fk⋅d ⋅cos180 ° =
= - fk⋅d =-mg µ⋅ d ⋅ cos18°
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Lecture 9
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Example of the 3rd Common Exam
V1 =4.0 m/s
1
V2 =8.6 m/s
Kf = 0
2
What minimum coefficient of
10 m
kinetic friction µk is required to
bring the crate to a stop over a
distance of
10 m along the lower surface ?
Lecture 9
Kf - Ki = Wfriction = -mgµkd
0- ½mv2 = -mgµkd
½mv2 = mgµkd; µk= v2/2gd =
(8.6m/s)2/(2·10m/s2 ·10m) = 0.37
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Lecture 9
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Lecture 9
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Perpetual Motion and “Free Energy”
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Perpetuum Mobile
“Machine, which works itself forever”
Example 1
Balance of Forces:
English: Perpetual Motion
Balance of Torques:
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Lecture 9
More Examples:
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More Examples:
Iron Disk
Water
Magnet
All parts of the cylinder that fall in the greater gravity (magnetic)
(magnetic) level must be pushet out, as well. All the work, that a part of
cylinder gets when it's moving toward the greater gravity (magnetic)
(magnetic) level is needed when it is pushed back out of it..
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Put an innertube on a wheel. Fill it two thirds with wather.
wather. Put an axle through it so it can spin. Now make another one like
like it. Now hold
the axels and push the wheel up against each other so that they can squeez each others wather to the outside. The results are that one
side of each wheel is lighter than its other side. That is why the
the wheel spins.
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More Examples:
More Examples:
Iron Ball
Iron Ball
Magnets
Pendulum
Magnet
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Lecture 9
More Examples:
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More Examples:
Water
Iron Ball
buoyant force of
Archimedes'
principle: "A body
immersed in liquid
experiences and
upward buoyant
force equal to the
weight of the
displaced liquid."
Magnets
Pendulum
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Sample Problem
Sample Problem
A 61 kg bungeebungee-cord jumper is on a 45 m bridge
above a river. The elastic bungee cord has a
relaxed length of L = 25 m.
m. Assume that the cord
obeys Hooke’s law, with a spring constant of 160
N/m.
N/m. If the jumper stops before reaching the water,
what is the height h of her feet above the water at
her lowest point?
point?
Lecture 9
– H/2
L + d + h = 45m
L + d + h = 45m
E = K + Ug + Ue = Const; (∆
(∆ K =0)
E = K + Ug + Ue = Const; (∆
(∆ K =0)
∆Ug = – mgy = – 61 kg · 9.8m/s2 · * (L+d)
∆Ug = – mgh = – 61 kg · 9.8m/s2 · (L+d)
∆Ue = kd2/2 = 160 N/m · d2/2
∆Ue = kd2/2 = 160 N/m · d2/2
80d2 – 600d – 15000 = 0; (d2 – 7.5d – 187.5 = 0)
80d2 – 600d – 15000 = 0; (d2 – 7.5d – 187.5 = 0)
d = 18 m and d = -10.5 m
d = 18 m and d = -10.5 m
h = 45m – 25m – 18m = 2m
h = 45m – 25m – 18m = 2m
Andrei Sirenko, NJIT
+H/2
-10.5 m
A 61 kg bungeebungee-cord jumper is on a 45 m bridge
above a river. The elastic bungee cord has a
relaxed length of L = 25 m.
m. Assume that the cord
obeys Hooke’s law, with a spring constant of 160
N/m.
N/m. If the jumper stops before reaching the water,
what is the height h of her feet above the water at
her lowest point?
point?
29
Lecture 9
Sample Problem
A 61 kg bungeebungee-cord jumper is on a 45 m bridge
above a river. The elastic bungee cord has a
relaxed length of L = 25 m.
m. Assume that the cord
obeys Hooke’s law, with a spring constant of 160
N/m.
N/m. If the jumper stops before reaching the water,
what is the height h of her feet above the water at
her lowest point?
point?
Andrei Sirenko, NJIT
30
Sample Problem
An elevator cab of mass m = 500 kg is descending with
speed vi = 4.0 m/s when its supporting cable begins to
slip, allowing it to fall with constant acceleration a = g/5.
L + d + h = 45m
During the 12 m fall, what is the work WT done by
the upward pull T of the elevator cab?
E = K + Ug + Ue = Const; (∆
(∆ K =0)
T – mg = – ma = – mg/5
∆Ug = – mgh = – 61 kg · 9.8m/s2 · (L+d+H)
T=0.8·
T=0.8·mg;
∆Ue = kd2/2 = 160 N/m · d2/2
W= – 0.8mgd = – 0.8 · 500kg · 9.8m/s2 · 12m =
80d2 – 600d – 15000 = 0; (d2 – 7.5d – 202.5 = 0)
= – 47,000 J
d = 18.5 m and d = – 11 m
h = 45m – 25m – 18.5m = 1.5m but H=2m …
Lecture 9
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Lecture 9
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QZ#9:
Sample Problem
1. An elevator cab of mass m = 500 kg is descending with
speed vi = 4.0 m/s when its supporting cable begins to slip,
allowing it to fall with constant acceleration a = g/5,
/5, d=12 m
What is the elevator’s kinetic energy at the end of the
fall? Hint: Wmg = 59000 J ; WT = – 47000 J
An elevator cab of mass m = 500 kg is descending with
speed vi = 4.0 m/s when its supporting cable begins to
slip, allowing it to fall with constant acceleration a = g/5.
During the fall through a distance d = 12 m, what is
the work Wg done on the cab by the gravitational
force Fg?
Wmg= +mgd
+mgd = 500kg · 9.8m/s2 · 12m = 59000J
Lecture 9
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magnet iron
2 We are not using this type of vehicle because
a) perpetual motion is forbidden by the
Newton's Laws
b) police does not allow it
c) sitting next to a strong magnet is not good for the driver’s health
d) there are no such strong magnets so far
e) this vehicle is not going to start moving by itself, so it is not very
practical for plane roads. Can be only used to go down the hill.
Lecture 9
Andrei Sirenko, NJIT
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