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Lecture 9

This document summarizes a lecture on potential energy and conservation of energy. It discusses concepts like gravitational potential energy, elastic potential energy, conservation of mechanical energy, and examples of applying the principle of energy conservation to problems involving changes in kinetic and potential energy. Sample problems are provided to illustrate calculating work done by conservative forces and determining the minimum coefficient of friction required to stop an object.

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0% found this document useful (0 votes)
88 views9 pages

Lecture 9

This document summarizes a lecture on potential energy and conservation of energy. It discusses concepts like gravitational potential energy, elastic potential energy, conservation of mechanical energy, and examples of applying the principle of energy conservation to problems involving changes in kinetic and potential energy. Sample problems are provided to illustrate calculating work done by conservative forces and determining the minimum coefficient of friction required to stop an object.

Uploaded by

James Sergeant
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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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 2

Power
Average Power

Sample Problem 7- 7-10:


10: Two constant forces F1 and
Units: Watts F2 acting on a box as the box slides rightward across
a frictionless floor. Force F1 is horizontal, with
magnitude 2.0 N, N, force F2 is angled upward by 60º
60º
Instantaneous Power 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?
b) If the magnitude F2 is, instead, 6.0 N,
N, what is
P= ½*60kg*(5m/s)2 now the net power, and is it changing?
Lecture 9 Andrei Sirenko, NJIT 3 Lecture 9 Andrei Sirenko, NJIT 4
Work and Potential Energy
• Potential Energy and Conservation of
Energy Potential Energy

• Conservative Forces
General Form:
• Gravitational and Elastic Potential Energy
• Conservation of (Mechanical) Energy
• Potential Energy Curve
• External and Internal Forces Gravitational Potential Energy

Elastic Potential Energy

Lecture 9 Andrei Sirenko, NJIT 5 Lecture 9 Andrei Sirenko, NJIT 6

Energy and Work Conservation of Mechanical Energy


Kinetic energy Mechanical Energy

Conservation of
Units of Work and Energy: Joule
Mechanical Energy
Work done by a constant force
In an isolated system where
only conservative forces cause
energy changes, the kinetic
Work–kinetic energy theorem and potential energy can
change, but their sum, the
mechanical energy Emec of the
system, cannot change.
Lecture 9 Andrei Sirenko, NJIT 7 Lecture 9 Andrei Sirenko, NJIT 8
Kinetic Energy: Kinetic Energy:
Potential Energy: Potential Energy:
• Gravitation: • Gravitation:

• Elastic (due to spring force): • Elastic (due to spring force):

1 K=0
1 UÆK UÅÆK
y
U=0
2
mg Conservation of Conservation of
2 Mechanical Energy Mechanical Energy

Lecture 9 Andrei Sirenko, NJIT 9 Lecture 9 Andrei Sirenko, NJIT 10

Path Independence of Sample Problem


A circus beagle of mass
Conservative Forces m = 6.0 kg runs onto the left
end of a curved ramp with
Sample Problem 8-1: A 2.0 kg block slides speed v0 = 7.8 m/s at height
along a frictionless track from a to point b. The y0 = 8.5 m above the floor. It
block travels through a total distance of 2.0 m, then slides to the right and
and a net vertical distance of 0.8 m. How much
work is done on the block by the gravitational comes to a momentary stop
force? 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?
Lecture 9 Andrei Sirenko, NJIT 11 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°
Lecture 9 Andrei Sirenko, NJIT 13 Lecture 9 Andrei Sirenko, NJIT 14

Example of the 3rd Common Exam

V1 =4.0 m/s Kf = 0
1 V2 =8.6 m/s

10 m
What minimum coefficient of Kf - Ki = Wfriction = -mgµkd
kinetic friction µk is required to 0- ½mv2 = -mgµkd
bring the crate to a stop over a
distance of ½mv2 = mgµkd; µk= v2/2gd =
10 m along the lower surface ? (8.6m/s)2/(2·10m/s2 ·10m) = 0.37
Lecture 9 Andrei Sirenko, NJIT 15 Lecture 9 Andrei Sirenko, NJIT 16
Lecture 9 Andrei Sirenko, NJIT 17 Lecture 9 Andrei Sirenko, NJIT 18

Perpetual Motion and “Free Energy”

Lecture 9 Andrei Sirenko, NJIT 19 Lecture 9 Andrei Sirenko, NJIT 20


Perpetuum Mobile
“Machine, which works itself forever” Example 1

English: Perpetual Motion Balance of Forces:

Balance of Torques:

Lecture 9 Andrei Sirenko, NJIT 21 Lecture 9 Andrei Sirenko, NJIT 22

More Examples: 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 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
cylinder gets when it's moving toward the greater gravity (magnetic)
(magnetic) level is needed when it is pushed back out of it.. side of each wheel is lighter than its other side. That is why the
the wheel spins.

Lecture 9 Andrei Sirenko, NJIT 23 Lecture 9 Andrei Sirenko, NJIT 24


More Examples: More Examples:

Iron Ball Iron Ball


Magnets
Pendulum

Magnet

Lecture 9 Andrei Sirenko, NJIT 25 Lecture 9 Andrei Sirenko, NJIT 26

More Examples: More Examples:


Water

Iron Ball
Magnets buoyant force of
Archimedes'
Pendulum principle: "A body
immersed in liquid
experiences and
upward buoyant
force equal to the
weight of the
displaced liquid."

Lecture 9 Andrei Sirenko, NJIT 27 Lecture 9 Andrei Sirenko, NJIT 28


Sample Problem Sample Problem
A 61 kg bungee-
bungee-cord jumper is on a 45 m bridge A 61 kg bungee-
bungee-cord jumper is on a 45 m bridge
above a river. The elastic bungee cord has a above a river. The elastic bungee cord has a
relaxed length of L = 25 m.
m. Assume that the cord relaxed length of L = 25 m.
m. Assume that the cord
obeys Hooke’s law, with a spring constant of 160 obeys Hooke’s law, with a spring constant of 160
N/m.
N/m. If the jumper stops before reaching the water, N/m.
N/m. If the jumper stops before reaching the water,
what is the height h of her feet above the water at what is the height h of her feet above the water at
her lowest point?
point? -10.5 m her lowest point?
point?
L + d + h = 45m L + d + h = 45m
(∆ K =0)
E = K + Ug + Ue = Const; (∆ (∆ K =0)
E = K + Ug + Ue = Const; (∆
∆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
Lecture 9 Andrei Sirenko, NJIT 29 Lecture 9 Andrei Sirenko, NJIT 30

+H/2
Sample Problem Sample Problem
A 61 kg bungee-
bungee-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
An elevator cab of mass m = 500 kg is descending with
obeys Hooke’s law, with a spring constant of 160 speed vi = 4.0 m/s when its supporting cable begins to
N/m.
N/m. If the jumper stops before reaching the water, slip, allowing it to fall with constant acceleration a = g/5.
what is the height h of her feet above the water at
her lowest point?
point? During the 12 m fall, what is the work WT done by
L + d + h = 45m the upward pull T of the elevator cab?

(∆ K =0)
E = K + Ug + Ue = Const; (∆ 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


– H/2
d = 18.5 m and d = – 11 m
h = 45m – 25m – 18.5m = 1.5m but H=2m …
Lecture 9 Andrei Sirenko, NJIT 31 Lecture 9 Andrei Sirenko, NJIT 32
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,
An elevator cab of mass m = 500 kg is descending with allowing it to fall with constant acceleration a = g/5,
/5, d=12 m
speed vi = 4.0 m/s when its supporting cable begins to What is the elevator’s kinetic energy at the end of the
slip, allowing it to fall with constant acceleration a = g/5. fall? Hint: Wmg = 59000 J ; WT = – 47000 J

During the fall through a distance d = 12 m, what is


the work Wg done on the cab by the gravitational
force Fg?
magnet iron
Wmg= +mgd
+mgd = 500kg · 9.8m/s2 · 12m = 59000J 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 33 Lecture 9 Andrei Sirenko, NJIT 34

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