SlideShare ist ein Scribd-Unternehmen logo
1 von 49
Chapter 6
Work and Energy
Younes Sina
Work (W): Work is defined as the product of parallel force and
distance. W = F ll x .
F ll denotes the component of force F that is parallel to
displacement , x .
The SI unit for work is N.m called " Joule", and the American unit is
" lb-ft "
If the direction of F is parallel to that of x, the work done is simply
W = F x.
Example :
Find the work done by force F = 25N in
pushing the block a distance of 14m .
25 N force applied
Block moved by 14 m
25 N
14 m
W=F . x
W=(25N)(14 m)
W=350 Joules
Solution
If an object placed on a horizontal surface is pushed or
pulled by force F as shown below, the component of F that
is parallel to x does useful work .
The component perpendicular to x does no work.
Example : A block is pulled a distance of x = 24m
from A to B as shown via force F = 45N that makes
a 30 .0 o angle with the horizontal surface . Calculate
the work done by F.
x = 24m
30 .0 o
Solution: For θ = 30.0o, and F = 45N
F ll = 45N cos (30 .0 ) = 39N
W = F ll x
W = (39N)(24m) = 940 Nm
W = 940 J
Example : In the following figure, find
(a) the magnitude of F such that the block slides at constant
speed to the right .
(b) Find the work done by this force if the displacement is 38 m .
Example: In previous example, find the work done by
the frictional force, F k , within the same distance.
Solution: F k acts opposite to x; therefore, it does negative
work.
W friction = F k x
W = ( -45N )( 38m ) = -1700 J
Energy: Energy is defined as the ability to do work. Energy and
work are expressed in same units. Typical units are: J, cal, kcal, and eV.
Types of Energy:
Energy exists in different forms such as mechanical, electric, nuclear,
light, chemical, etc... .
In this chapter, mechanical energy will be discussed only.
Heat energy is also a will be discussed in Chapter 12 .
Mechanical Energy:
Kinetic energy, Gravitational potential energy, and elastic (spring)
potential energy are forms of mechanical energy and will be
discussed under this topic.
I ) Kinetic Energy (K.E.):
Kinetic energy is the energy that a mass (an object) has because of
its motion. As long as an object moves or has some speed, it has
kinetic energy.
K.E. is proportional to mass ( M) and proportional to the square of
velocity ( v 2 ) .
K.E. = (1/2) Mv 2
II ) Gravitational Potential Energy (P.E.):
This energy is the type that an object has due to its elevation with
respect to a reference level. This energy is significant when objects
are in the vicinity of planets, stars and other heavenly masses .
Gravitational P.E. is proportional to the acceleration of gravity ( g) of
the planet or star, the mass of the object, M, and its elevation ( h)
from a reference level.
P.E. = Mgh
Example :
Calculate the K .E . of a 2000-kg car that is moving
(a) at 10.0m/s
(b) 20.0 m/s
(c) 30.0 m/s
Solution: (3 sig. fig.)
(a) (K.E.)1 = (1/2)(2000.kg)( 10 .0m/s) 2 = 100,000 (kg m/s 2)m = 100,000 J
(b) (K.E.)2 = (1/2)(2000.kg)( 20 .0m/s) 2 = 400,000 (kg m/s 2)m = 400,000 J
(c) (K.E.)3 = (1/2)(2000.kg)( 30 .0m/s) 2 = 900,000 (kg m/s 2)m = 900,000 J
Example:
A rock of mass 6.1 kg is raised to the top of a building 13 m high.
Calculate its gravitational P .E . with respect to the ground.
Solution:
P.E. = Mgh
P.E. = (6 .1 kg)(9 .8 m/s 2)(13 m)
P.E. = 780 Nm = 780J
Example :
In the following figure, a 95-kg crate is pushed up on an incline that
is practically frictionless. The incline is 8 .0m long and makes a 31 o
angle with the horizontal floor. Calculate the P .E . Of the crate with
respect to the floor when it reaches the top of the incline.
Example : A swimming pool is on the top of a hill at an average elevation of 150m
from a certain ground level . The swimming pool has dimensions:
15 m X 25 m X 2 .4 m and is full. The mass density of water is 1.000 ton/m 3.
Determine
(a) the P .E . Of the water in the pool with respect to that level .
If the pool is allowed to empty to the ground level,
(b) how much energy is at most available for use?
(c) how much electric energy will become available? If a generator uses this energy
for electricity production, and the overall efficiency is 62%
Solution:
(a) The pool's volume is V = w l h
V = 900m 3
r = M / V
M = r V
M = (1000 kg/m 3)(900 m3) = 900,000 kg
P.E. = Mgh
P.E. = ( 900,000 kg )( 9 .8 m/s 2 )( 150m ) = 1.3 × 10 9 J
(b) 1.3 × 10 9 J
(c) 0.62 (1.3 × 10 9 J) = 8.2 × 10 8 J
100 W
2278 hr
Example : A 750-kg car is traveling at a velocity of 72 km/h eastward
and on a level road . Determine
(a) its initial kinetic energy (K .E .) i
If this car is slowed down to a speed of 36 km/h, calculate
(b) its final (K.E.) f .
(c) How much is the change in its kinetic energy and where does this
energy go ?
Vi=72 km/h Vf=36 km/h
Solution:
(a) (K.E.) i = (1/2)Mv i
2
(K.E.) i = (1/2)( 750 kg)( 20 . m/s)2 = 150,000 J
(b) (K.E.) f = (1/2)Mv f
2
(K.E.) f = (1/2)( 750 kg)( 10 . m/s)2 = 38,000 J
(c) Δ(K.E.) = (K.E.) f - (K.E.) i
Δ(K.E.) = 38,000 J - 150,000 J = - 112,000 J
This energy is consumed by force of friction (brakes force, for
example) that acts opposite to the direction of motion . In fact, it is
the work done by force of friction. Most of this energy converts to
heat and warms up the brakes. Friction does negative work .
Example: If the work done by force of friction is -112,000J .
Use the work formula to calculate the force applied by friction if brakes were used
within a distance of 56m .
Wf=-112,000J
56m
Solution:
W = F k x
- 112,000 J = F k (56m)
F k = - 2000N
Work-Kinetic Energy Theorem:
The work done by the net force acting on a mass is equal to the
change in the kinetic energy of that mass.
(ΣF ) x = Δ(K.E.)
(ΣF ) x = (K.E.) f - (K.E.) i
Example : A 900-kg car traveling at 15m/s changes its speed to
25m/s in a distance of 50 m due to a net force . Calculate
(a) the net force
(b) the engine force if the frictional forces add up to 1400N .
V=15m/s V=25m/s
X=50 m
M= 900 kg
Solution:
(a) Work-K.E. theorem :
(Σ F) ∙ x = (K.E.) f - (K.E.) i
Σ F (50 m) = (1/2)(900)(25) 2 - (1/2)(900)(15) 2
Σ F = 3600 N
(b) Σ F = F e - Ff
3600N = Fe - 1400N
F e = 5000 N
Example : A boy pulls a 45.0-kg sled (including his friend in it)
from rest for a distance of 12.0 m with a horizontal and constant
force of 165.0 N. The frictional force between the sled and snow
is 55.0 N. Calculate
(a) the work done by the boy on the sled
(b) the work done by the frictional force on the sled
(c) the work done by the net force on the sled
(d) the speed of the sled at the end of the 12.0 m distance .
12.0m
45.0 kg
165.0 N
Wf=55.0 N
v=0 m/s v=? m/s
Solution:
(a) Wboy = F ll x
W = (165 N)(12 .0 m) = 1980 J
(b) Wfriction = F k x
W = (55 .0 N)(12.0 m) = 660.0 J
(Work of friction is negative)
(c) Wnet = Fnet x
(Σ F) x = (165N - 55.0 N)(12.0 m) = 1320 J
(d) (Σ F) x = (K.E.) f - (K.E.) i
1320 J = (1/2)(45 .0kg) Vf
2 - (1/2)(45 .0kg) (0)2
Vf = + 7.66 m/s
The Law of Conservation of Energy
This law states that:
"Energy is conserved.
It is neither created nor destroyed.
It converts from one form to another".
Conservation of Mechanical Energy
Example : In the following figure, neglecting friction, find the speed
Of the 750-kg car at the bottom of the hill . Suppose the car is put in
neutral and starts from rest from the top of the hill .
V=0, M=750 kg
45 m
Conservation of mechanical energy:
Total Energy at A = Total Energy at B
(K .E .)A + (P .E .)A = (K .E .)B + (P .E .)B
(1/2)MVA
2 + M g hA = ( 1/2)MVB
2 + M g hB
VA = 0 and hB = 0
M g hA = ( 1/2)MVB
2
g hA = (1/2)VB
2
2 g hA = VB
2
VB = 30 m/s
A
BhA
hB = 0
VB
Example :
In the following figure, if 120,000 J of energy is consumed by
frictional forces, find the speed of the 750-kg car at the bottom
of the hill . Suppose the car is put in neutral and starts from rest
from the top of the hill .
frictional Energy=120,000 J
In this case, part of the available energy will be wasted by friction
Conservation of mechanical energy:
Total Energy at A - W friction= Total Energy at B
(K .E .)A + (P .E .)A - Wfriction = (K .E .)B + (P .E .)B
(1/2)M A
2 + M g hA -120,000J = ( 1/2)MV B
2 + M g hB
V A = 0 and h B = 0
M ghA -120,000J = ( 1/2)MV B
2
(750)(9 .8)(45) J - 120,000 J = 0 .5(750 kg)VB
2
562(m/s) 2 = VB
2
VB = 24 m/s
V=0, M=750 kg
Example: In the figure shown, find
(a) the work done by the frictional force on the car as it coasts
down the hill in neutral
(b) the energy loss due to friction
(c) the speed of the 750-kg car (VB) at the bottom of the hill .
400 m
Solution:
(a) The work done by friction is
W friction = F k x
W friction = ( -300N)(400m) = -120,000 J
(b) -120,000 J
(c) Conservation of mechanical energy:
Total Energy at A - Wfriction = Total Energy at B
(K .E .)A + (P .E .)A - Wfriction= (K .E .)B + (P .E .)B
(1/2)MVA
2 + M g h A - 120,000 J = (1/2)MVB
2 + M g hB
VA = 0 and hB = 0
M ghA -120,000 J = (1/2)MVB
2
(750)(9.8)(45) J - 120,000 J = 0.5(750)VB
2
[562(m/s)]2 = VB
2
VB = 24 m/s
Power is defined as the work done per units of time.
Mathematically:
The (SI) unit for power is :
The industrial unit: hp
Power
t
W
P


=
Wattcalled
s
J
s
ftlb
hphP

== 5501andwatts7461
Example : An electric motor is capable of delivering 7 .2 Million
Joules of work in one hour and 400.0 seconds. Find the power
of the motor in watts, kilowatts, and hp .
Solution:
P = W/t
P = (7 .2 x10 6 J )/(4000 s) = 1800 J/s = 1800 watts
P = 1.8 kilowatts (kw)
P = (1800/746 ) hp
P = 2.4 hp
Example:
Calculate the amount of work or energy that a 4.50 hp
electric motor can deliver in 10.0 hours.
Solution:
P = 4 .5hp = (4 .50)(746 watts) = 3360 watts or ( J /s )
P = W / t
W = Pt
W = (3360 J/s)(36,000s) = 1.21 x 10 8 J
Efficiency: When a device receives power from a source, it does not deliver all of
it in the intended form and converts a portion of it to other undesired forms. This
makes a device to be less than 100 percent efficient.
Most power plants have efficiencies of under 50 percent. A good nuclear power
plant is about 45% efficient . Early coal plants were hardly 20% efficient .
Eff. = Pout /Pin
Example : A 1.25 hp electric pump with an efficiency of 92.5% is used to perform
1 .40 Mega Joules of work.
(a) How long does it take for the electric pump to do the job ?
(b) If it was 100% efficient , how long would it take?
Solution:
A 1.25 hp electric pump means it draws 1 .25 hp of electric power from the
source.
It generally cannot give back all of it .
Make sure that you write the formulas with horizontal fraction bars .
Eff. = P out / P in
0 .925 = P out / (1 .25 hp)
P out = 0 .925(1 .25hp) = 1.16 hp
(a) P = W / t
t = W / P
t = (1 .40 x 10 6 J) / ( 1 .16 x 746 watts ) = 1620 sec
(b) P = W/t
t = W/P
t =(1 .40 x 10 6 J)/( 1 .25 x 746 watts ) = 1500 sec
Example: Calculate
(a) the necessary power to empty a swimming pool with dimensions
(12m)(25m)(2 .4m) by pumping its water to an average height of 3.5m in 2.5hrs .
The mass density of water is 1000 kg/m 3.
(Hint: The power you calculate is the power that the electric pump has to deliver
to water, Pout) .
If the efficiency of the electric pump used is 88% , calculate
(b) the electric power that the electric motor pulls from the power source, Pin .
Solution:
V = w. l. h
V = 720m3
r = M / V
M = r V
M = (1000 kg/m 3)(720 m3) = 720,000 kg
(a) P = W / t
W = F x
F = the weight of water= Mg
x = height
P = (F x) / t
P = ( Mg x) / t
P = (720,000kg )( 9 .8 m/s 2 )( 3 .5m ) / (2 .5 X 3600s ) = 2700 watts
P = 2.7kw
P = (2700 / 746) hp = 3.6 hp
(b) Eff. = P out / P in
0 .88 = 2700watts / P in
P in = 2700watts / 0 .88 = 3100 watts
Another Version of Power Formula:
P = W / t
W = F x
P = (F x) / t
(x / t )= v
P = F v
This means that power is equal to force times velocity (if both of
force and velocity are in the same direction).
As you see the product of velocity and force is a constant if a
constant power is available . When P is constant, the product F ∙v
is constant . When a greater F is needed, a smaller v is attainable
and vice versa .
Example :
A car is using 56 hp of its total power. When it is going up a steep hill, a force of
4200 N is needed for constant velocity motion of it up that hill. When it is
traveling along a level and horizontal road, a force of 1200 N is needed for its
constant velocity motion. Find the velocity of the car in each case .
P = F v
56 hp
56 hp
F= 4200 N
F=1200 N
Solution:
P = (56)(746 watts) = 42000 watts
(a) P = F v
v = P / F
v = 42000 watts / 4200N = 10 m/s
(b) P = F v
v = P / F
v = 42000watts / 1200N = 35 m/s
problems 1 through 5 chapter 6

Weitere ähnliche Inhalte

Was ist angesagt?

Polinomios de taylor
Polinomios de taylorPolinomios de taylor
Polinomios de taylorKeivin Perez
 
Calculus- Basics
Calculus- BasicsCalculus- Basics
Calculus- BasicsRabin BK
 
Benginning Calculus Lecture notes 2 - limits and continuity
Benginning Calculus Lecture notes 2 - limits and continuityBenginning Calculus Lecture notes 2 - limits and continuity
Benginning Calculus Lecture notes 2 - limits and continuitybasyirstar
 

Was ist angesagt? (6)

5 cálculo integral
5 cálculo integral5 cálculo integral
5 cálculo integral
 
Polinomios de taylor
Polinomios de taylorPolinomios de taylor
Polinomios de taylor
 
Calculus- Basics
Calculus- BasicsCalculus- Basics
Calculus- Basics
 
Benginning Calculus Lecture notes 2 - limits and continuity
Benginning Calculus Lecture notes 2 - limits and continuityBenginning Calculus Lecture notes 2 - limits and continuity
Benginning Calculus Lecture notes 2 - limits and continuity
 
Ring homomorphism
Ring homomorphismRing homomorphism
Ring homomorphism
 
Complex function
Complex functionComplex function
Complex function
 

Andere mochten auch

Andere mochten auch (10)

Chapter 11
Chapter 11Chapter 11
Chapter 11
 
Chapter 12
Chapter 12Chapter 12
Chapter 12
 
Chapter 10
Chapter 10Chapter 10
Chapter 10
 
Chapter 14
Chapter 14Chapter 14
Chapter 14
 
Chapter 7
Chapter 7Chapter 7
Chapter 7
 
Physics by Younes Sina
Physics by Younes SinaPhysics by Younes Sina
Physics by Younes Sina
 
Chapter 4
Chapter 4Chapter 4
Chapter 4
 
Chapter 5
Chapter 5Chapter 5
Chapter 5
 
Chapter 9
Chapter 9Chapter 9
Chapter 9
 
Chapter 8
Chapter 8Chapter 8
Chapter 8
 

Ähnlich wie Chapter 6

work energy theorem and kinetic energy
work energy theorem and kinetic energywork energy theorem and kinetic energy
work energy theorem and kinetic energyKharen Adelan
 
Work, energy, and power
Work, energy, and powerWork, energy, and power
Work, energy, and powerAbhay Goyal
 
Work, energy, and power
Work, energy, and powerWork, energy, and power
Work, energy, and powerAbhey Goyal
 
2 work energy power to properties of liquids
2 work energy power to properties of liquids2 work energy power to properties of liquids
2 work energy power to properties of liquidsAntony Jaison
 
2 work energy power to properties of liquids
2 work energy power to properties of liquids2 work energy power to properties of liquids
2 work energy power to properties of liquidsarunjyothi247
 
Work and energy
Work and energyWork and energy
Work and energyPratiksha
 
Chapter 4 Work energy power.pptx
Chapter 4 Work energy power.pptxChapter 4 Work energy power.pptx
Chapter 4 Work energy power.pptxKjSrikkanth1
 
02 UNIT-2 (WORK & ENERGY) .pptx
02 UNIT-2 (WORK & ENERGY) .pptx02 UNIT-2 (WORK & ENERGY) .pptx
02 UNIT-2 (WORK & ENERGY) .pptxFatimaAfzal56
 
Work, Energy Power rev.ppt
Work, Energy Power rev.pptWork, Energy Power rev.ppt
Work, Energy Power rev.pptBonPatio1
 
Work, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbn
Work, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbnWork, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbn
Work, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbnMarvinelVinuya1
 

Ähnlich wie Chapter 6 (20)

work energy theorem and kinetic energy
work energy theorem and kinetic energywork energy theorem and kinetic energy
work energy theorem and kinetic energy
 
Linear momentum and its conservation by Victor R. Oribe
Linear momentum and its conservation by Victor R. OribeLinear momentum and its conservation by Victor R. Oribe
Linear momentum and its conservation by Victor R. Oribe
 
Work, energy, and power
Work, energy, and powerWork, energy, and power
Work, energy, and power
 
Work power-energy
Work power-energyWork power-energy
Work power-energy
 
Lecture09
Lecture09Lecture09
Lecture09
 
Lecture09
Lecture09Lecture09
Lecture09
 
Work, energy, and power
Work, energy, and powerWork, energy, and power
Work, energy, and power
 
2 work energy power to properties of liquids
2 work energy power to properties of liquids2 work energy power to properties of liquids
2 work energy power to properties of liquids
 
2 work energy power to properties of liquids
2 work energy power to properties of liquids2 work energy power to properties of liquids
2 work energy power to properties of liquids
 
Every Equation
Every EquationEvery Equation
Every Equation
 
dyn-part3.ppt
dyn-part3.pptdyn-part3.ppt
dyn-part3.ppt
 
Work and energy
Work and energyWork and energy
Work and energy
 
5299254.ppt
5299254.ppt5299254.ppt
5299254.ppt
 
Chapter5
Chapter5Chapter5
Chapter5
 
Ch07 ssm
Ch07 ssmCh07 ssm
Ch07 ssm
 
Chapter 4 Work energy power.pptx
Chapter 4 Work energy power.pptxChapter 4 Work energy power.pptx
Chapter 4 Work energy power.pptx
 
02 UNIT-2 (WORK & ENERGY) .pptx
02 UNIT-2 (WORK & ENERGY) .pptx02 UNIT-2 (WORK & ENERGY) .pptx
02 UNIT-2 (WORK & ENERGY) .pptx
 
Work, Energy Power rev.ppt
Work, Energy Power rev.pptWork, Energy Power rev.ppt
Work, Energy Power rev.ppt
 
Work, energy and power
Work, energy and powerWork, energy and power
Work, energy and power
 
Work, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbn
Work, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbnWork, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbn
Work, Energy Power rev.pptbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbn
 

Mehr von Younes Sina

ICDIM 2012 presentation
ICDIM 2012 presentationICDIM 2012 presentation
ICDIM 2012 presentationYounes Sina
 
Phase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 SystemPhase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 SystemYounes Sina
 
Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3Younes Sina
 
Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)Younes Sina
 
توسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصدتوسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصدYounes Sina
 
Nuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclidesNuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclidesYounes Sina
 
Ion implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utkIon implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utkYounes Sina
 
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystalsYounes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystalsYounes Sina
 
Younes Sina, Ion Channeling
 Younes Sina, Ion Channeling  Younes Sina, Ion Channeling
Younes Sina, Ion Channeling Younes Sina
 
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...Younes Sina
 
Younes Sina's presentation on Nuclear reaction analysis
Younes Sina's presentation on  Nuclear reaction analysisYounes Sina's presentation on  Nuclear reaction analysis
Younes Sina's presentation on Nuclear reaction analysisYounes Sina
 
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...Younes Sina
 
Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry  Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry Younes Sina
 
A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry  A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry Younes Sina
 
Ion Implantation
Ion Implantation Ion Implantation
Ion Implantation Younes Sina
 
Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3Younes Sina
 

Mehr von Younes Sina (20)

Chapter 3
Chapter 3Chapter 3
Chapter 3
 
Chapter 2
Chapter 2Chapter 2
Chapter 2
 
Chapter 1
Chapter 1Chapter 1
Chapter 1
 
ICDIM 2012 presentation
ICDIM 2012 presentationICDIM 2012 presentation
ICDIM 2012 presentation
 
Phase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 SystemPhase Diagram, ZrO2 and Al2O3 System
Phase Diagram, ZrO2 and Al2O3 System
 
Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3Electron irradiation effect on Al2O3
Electron irradiation effect on Al2O3
 
Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)Line Spectra (Rydberg’s Constant)
Line Spectra (Rydberg’s Constant)
 
توسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصدتوسعه روش شكست سنجي براي تعيين درصد
توسعه روش شكست سنجي براي تعيين درصد
 
Nuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclidesNuclear Radiation, the chart of nuclides
Nuclear Radiation, the chart of nuclides
 
Ion implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utkIon implantation effects in sapphire-Poster for advisory meeting at utk
Ion implantation effects in sapphire-Poster for advisory meeting at utk
 
RBS
RBSRBS
RBS
 
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystalsYounes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
Younes Sina, Ion implantation and thermal annealing of α-Al2O3 single crystals
 
Younes Sina, Ion Channeling
 Younes Sina, Ion Channeling  Younes Sina, Ion Channeling
Younes Sina, Ion Channeling
 
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
Younes Sina ,Student Poster Competition ,The Oak Ridge Chapter of ASM, the Ma...
 
Younes Sina's presentation on Nuclear reaction analysis
Younes Sina's presentation on  Nuclear reaction analysisYounes Sina's presentation on  Nuclear reaction analysis
Younes Sina's presentation on Nuclear reaction analysis
 
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...Younes Sina's presentation about Chemical effects in zr  and co-implanted sap...
Younes Sina's presentation about Chemical effects in zr and co-implanted sap...
 
Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry  Younes Sina, Backscattering spectrometry
Younes Sina, Backscattering spectrometry
 
A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry  A presentation by Younes Sina: Backscattering spectrometry
A presentation by Younes Sina: Backscattering spectrometry
 
Ion Implantation
Ion Implantation Ion Implantation
Ion Implantation
 
Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3Ni ion-implanted α-Al2 O3
Ni ion-implanted α-Al2 O3
 

Kürzlich hochgeladen

Base editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editingBase editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editingNetHelix
 
Pests of safflower_Binomics_Identification_Dr.UPR.pdf
Pests of safflower_Binomics_Identification_Dr.UPR.pdfPests of safflower_Binomics_Identification_Dr.UPR.pdf
Pests of safflower_Binomics_Identification_Dr.UPR.pdfPirithiRaju
 
Pests of castor_Binomics_Identification_Dr.UPR.pdf
Pests of castor_Binomics_Identification_Dr.UPR.pdfPests of castor_Binomics_Identification_Dr.UPR.pdf
Pests of castor_Binomics_Identification_Dr.UPR.pdfPirithiRaju
 
GenBio2 - Lesson 1 - Introduction to Genetics.pptx
GenBio2 - Lesson 1 - Introduction to Genetics.pptxGenBio2 - Lesson 1 - Introduction to Genetics.pptx
GenBio2 - Lesson 1 - Introduction to Genetics.pptxBerniceCayabyab1
 
User Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather StationUser Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather StationColumbia Weather Systems
 
STOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptx
STOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptxSTOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptx
STOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptxMurugaveni B
 
Behavioral Disorder: Schizophrenia & it's Case Study.pdf
Behavioral Disorder: Schizophrenia & it's Case Study.pdfBehavioral Disorder: Schizophrenia & it's Case Study.pdf
Behavioral Disorder: Schizophrenia & it's Case Study.pdfSELF-EXPLANATORY
 
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCRCall Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCRlizamodels9
 
(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)
(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)
(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)riyaescorts54
 
preservation, maintanence and improvement of industrial organism.pptx
preservation, maintanence and improvement of industrial organism.pptxpreservation, maintanence and improvement of industrial organism.pptx
preservation, maintanence and improvement of industrial organism.pptxnoordubaliya2003
 
Speech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptxSpeech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptxpriyankatabhane
 
Pests of jatropha_Bionomics_identification_Dr.UPR.pdf
Pests of jatropha_Bionomics_identification_Dr.UPR.pdfPests of jatropha_Bionomics_identification_Dr.UPR.pdf
Pests of jatropha_Bionomics_identification_Dr.UPR.pdfPirithiRaju
 
《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》rnrncn29
 
basic entomology with insect anatomy and taxonomy
basic entomology with insect anatomy and taxonomybasic entomology with insect anatomy and taxonomy
basic entomology with insect anatomy and taxonomyDrAnita Sharma
 
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.PraveenaKalaiselvan1
 
Topic 9- General Principles of International Law.pptx
Topic 9- General Principles of International Law.pptxTopic 9- General Principles of International Law.pptx
Topic 9- General Principles of International Law.pptxJorenAcuavera1
 
Bioteknologi kelas 10 kumer smapsa .pptx
Bioteknologi kelas 10 kumer smapsa .pptxBioteknologi kelas 10 kumer smapsa .pptx
Bioteknologi kelas 10 kumer smapsa .pptx023NiWayanAnggiSriWa
 
Four Spheres of the Earth Presentation.ppt
Four Spheres of the Earth Presentation.pptFour Spheres of the Earth Presentation.ppt
Four Spheres of the Earth Presentation.pptJoemSTuliba
 

Kürzlich hochgeladen (20)

Base editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editingBase editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editing
 
Pests of safflower_Binomics_Identification_Dr.UPR.pdf
Pests of safflower_Binomics_Identification_Dr.UPR.pdfPests of safflower_Binomics_Identification_Dr.UPR.pdf
Pests of safflower_Binomics_Identification_Dr.UPR.pdf
 
Pests of castor_Binomics_Identification_Dr.UPR.pdf
Pests of castor_Binomics_Identification_Dr.UPR.pdfPests of castor_Binomics_Identification_Dr.UPR.pdf
Pests of castor_Binomics_Identification_Dr.UPR.pdf
 
Volatile Oils Pharmacognosy And Phytochemistry -I
Volatile Oils Pharmacognosy And Phytochemistry -IVolatile Oils Pharmacognosy And Phytochemistry -I
Volatile Oils Pharmacognosy And Phytochemistry -I
 
GenBio2 - Lesson 1 - Introduction to Genetics.pptx
GenBio2 - Lesson 1 - Introduction to Genetics.pptxGenBio2 - Lesson 1 - Introduction to Genetics.pptx
GenBio2 - Lesson 1 - Introduction to Genetics.pptx
 
User Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather StationUser Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather Station
 
STOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptx
STOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptxSTOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptx
STOPPED FLOW METHOD & APPLICATION MURUGAVENI B.pptx
 
Behavioral Disorder: Schizophrenia & it's Case Study.pdf
Behavioral Disorder: Schizophrenia & it's Case Study.pdfBehavioral Disorder: Schizophrenia & it's Case Study.pdf
Behavioral Disorder: Schizophrenia & it's Case Study.pdf
 
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCRCall Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
 
(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)
(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)
(9818099198) Call Girls In Noida Sector 14 (NOIDA ESCORTS)
 
preservation, maintanence and improvement of industrial organism.pptx
preservation, maintanence and improvement of industrial organism.pptxpreservation, maintanence and improvement of industrial organism.pptx
preservation, maintanence and improvement of industrial organism.pptx
 
Speech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptxSpeech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptx
 
Pests of jatropha_Bionomics_identification_Dr.UPR.pdf
Pests of jatropha_Bionomics_identification_Dr.UPR.pdfPests of jatropha_Bionomics_identification_Dr.UPR.pdf
Pests of jatropha_Bionomics_identification_Dr.UPR.pdf
 
《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》
 
basic entomology with insect anatomy and taxonomy
basic entomology with insect anatomy and taxonomybasic entomology with insect anatomy and taxonomy
basic entomology with insect anatomy and taxonomy
 
Hot Sexy call girls in Moti Nagar,🔝 9953056974 🔝 escort Service
Hot Sexy call girls in  Moti Nagar,🔝 9953056974 🔝 escort ServiceHot Sexy call girls in  Moti Nagar,🔝 9953056974 🔝 escort Service
Hot Sexy call girls in Moti Nagar,🔝 9953056974 🔝 escort Service
 
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
BIOETHICS IN RECOMBINANT DNA TECHNOLOGY.
 
Topic 9- General Principles of International Law.pptx
Topic 9- General Principles of International Law.pptxTopic 9- General Principles of International Law.pptx
Topic 9- General Principles of International Law.pptx
 
Bioteknologi kelas 10 kumer smapsa .pptx
Bioteknologi kelas 10 kumer smapsa .pptxBioteknologi kelas 10 kumer smapsa .pptx
Bioteknologi kelas 10 kumer smapsa .pptx
 
Four Spheres of the Earth Presentation.ppt
Four Spheres of the Earth Presentation.pptFour Spheres of the Earth Presentation.ppt
Four Spheres of the Earth Presentation.ppt
 

Chapter 6

  • 1. Chapter 6 Work and Energy Younes Sina
  • 2. Work (W): Work is defined as the product of parallel force and distance. W = F ll x . F ll denotes the component of force F that is parallel to displacement , x . The SI unit for work is N.m called " Joule", and the American unit is " lb-ft " If the direction of F is parallel to that of x, the work done is simply W = F x.
  • 3. Example : Find the work done by force F = 25N in pushing the block a distance of 14m . 25 N force applied Block moved by 14 m
  • 4. 25 N 14 m W=F . x W=(25N)(14 m) W=350 Joules Solution
  • 5. If an object placed on a horizontal surface is pushed or pulled by force F as shown below, the component of F that is parallel to x does useful work . The component perpendicular to x does no work.
  • 6.
  • 7. Example : A block is pulled a distance of x = 24m from A to B as shown via force F = 45N that makes a 30 .0 o angle with the horizontal surface . Calculate the work done by F. x = 24m 30 .0 o
  • 8. Solution: For θ = 30.0o, and F = 45N F ll = 45N cos (30 .0 ) = 39N W = F ll x W = (39N)(24m) = 940 Nm W = 940 J
  • 9. Example : In the following figure, find (a) the magnitude of F such that the block slides at constant speed to the right . (b) Find the work done by this force if the displacement is 38 m .
  • 10.
  • 11. Example: In previous example, find the work done by the frictional force, F k , within the same distance.
  • 12. Solution: F k acts opposite to x; therefore, it does negative work. W friction = F k x W = ( -45N )( 38m ) = -1700 J
  • 13. Energy: Energy is defined as the ability to do work. Energy and work are expressed in same units. Typical units are: J, cal, kcal, and eV. Types of Energy: Energy exists in different forms such as mechanical, electric, nuclear, light, chemical, etc... . In this chapter, mechanical energy will be discussed only. Heat energy is also a will be discussed in Chapter 12 . Mechanical Energy: Kinetic energy, Gravitational potential energy, and elastic (spring) potential energy are forms of mechanical energy and will be discussed under this topic.
  • 14. I ) Kinetic Energy (K.E.): Kinetic energy is the energy that a mass (an object) has because of its motion. As long as an object moves or has some speed, it has kinetic energy. K.E. is proportional to mass ( M) and proportional to the square of velocity ( v 2 ) . K.E. = (1/2) Mv 2 II ) Gravitational Potential Energy (P.E.): This energy is the type that an object has due to its elevation with respect to a reference level. This energy is significant when objects are in the vicinity of planets, stars and other heavenly masses . Gravitational P.E. is proportional to the acceleration of gravity ( g) of the planet or star, the mass of the object, M, and its elevation ( h) from a reference level. P.E. = Mgh
  • 15. Example : Calculate the K .E . of a 2000-kg car that is moving (a) at 10.0m/s (b) 20.0 m/s (c) 30.0 m/s
  • 16. Solution: (3 sig. fig.) (a) (K.E.)1 = (1/2)(2000.kg)( 10 .0m/s) 2 = 100,000 (kg m/s 2)m = 100,000 J (b) (K.E.)2 = (1/2)(2000.kg)( 20 .0m/s) 2 = 400,000 (kg m/s 2)m = 400,000 J (c) (K.E.)3 = (1/2)(2000.kg)( 30 .0m/s) 2 = 900,000 (kg m/s 2)m = 900,000 J
  • 17. Example: A rock of mass 6.1 kg is raised to the top of a building 13 m high. Calculate its gravitational P .E . with respect to the ground.
  • 18. Solution: P.E. = Mgh P.E. = (6 .1 kg)(9 .8 m/s 2)(13 m) P.E. = 780 Nm = 780J
  • 19. Example : In the following figure, a 95-kg crate is pushed up on an incline that is practically frictionless. The incline is 8 .0m long and makes a 31 o angle with the horizontal floor. Calculate the P .E . Of the crate with respect to the floor when it reaches the top of the incline.
  • 20.
  • 21. Example : A swimming pool is on the top of a hill at an average elevation of 150m from a certain ground level . The swimming pool has dimensions: 15 m X 25 m X 2 .4 m and is full. The mass density of water is 1.000 ton/m 3. Determine (a) the P .E . Of the water in the pool with respect to that level . If the pool is allowed to empty to the ground level, (b) how much energy is at most available for use? (c) how much electric energy will become available? If a generator uses this energy for electricity production, and the overall efficiency is 62%
  • 22. Solution: (a) The pool's volume is V = w l h V = 900m 3 r = M / V M = r V M = (1000 kg/m 3)(900 m3) = 900,000 kg P.E. = Mgh P.E. = ( 900,000 kg )( 9 .8 m/s 2 )( 150m ) = 1.3 × 10 9 J (b) 1.3 × 10 9 J (c) 0.62 (1.3 × 10 9 J) = 8.2 × 10 8 J 100 W 2278 hr
  • 23. Example : A 750-kg car is traveling at a velocity of 72 km/h eastward and on a level road . Determine (a) its initial kinetic energy (K .E .) i If this car is slowed down to a speed of 36 km/h, calculate (b) its final (K.E.) f . (c) How much is the change in its kinetic energy and where does this energy go ? Vi=72 km/h Vf=36 km/h
  • 24. Solution: (a) (K.E.) i = (1/2)Mv i 2 (K.E.) i = (1/2)( 750 kg)( 20 . m/s)2 = 150,000 J (b) (K.E.) f = (1/2)Mv f 2 (K.E.) f = (1/2)( 750 kg)( 10 . m/s)2 = 38,000 J (c) Δ(K.E.) = (K.E.) f - (K.E.) i Δ(K.E.) = 38,000 J - 150,000 J = - 112,000 J This energy is consumed by force of friction (brakes force, for example) that acts opposite to the direction of motion . In fact, it is the work done by force of friction. Most of this energy converts to heat and warms up the brakes. Friction does negative work .
  • 25. Example: If the work done by force of friction is -112,000J . Use the work formula to calculate the force applied by friction if brakes were used within a distance of 56m . Wf=-112,000J 56m
  • 26. Solution: W = F k x - 112,000 J = F k (56m) F k = - 2000N
  • 27. Work-Kinetic Energy Theorem: The work done by the net force acting on a mass is equal to the change in the kinetic energy of that mass. (ΣF ) x = Δ(K.E.) (ΣF ) x = (K.E.) f - (K.E.) i
  • 28. Example : A 900-kg car traveling at 15m/s changes its speed to 25m/s in a distance of 50 m due to a net force . Calculate (a) the net force (b) the engine force if the frictional forces add up to 1400N . V=15m/s V=25m/s X=50 m M= 900 kg
  • 29. Solution: (a) Work-K.E. theorem : (Σ F) ∙ x = (K.E.) f - (K.E.) i Σ F (50 m) = (1/2)(900)(25) 2 - (1/2)(900)(15) 2 Σ F = 3600 N (b) Σ F = F e - Ff 3600N = Fe - 1400N F e = 5000 N
  • 30. Example : A boy pulls a 45.0-kg sled (including his friend in it) from rest for a distance of 12.0 m with a horizontal and constant force of 165.0 N. The frictional force between the sled and snow is 55.0 N. Calculate (a) the work done by the boy on the sled (b) the work done by the frictional force on the sled (c) the work done by the net force on the sled (d) the speed of the sled at the end of the 12.0 m distance . 12.0m 45.0 kg 165.0 N Wf=55.0 N v=0 m/s v=? m/s
  • 31. Solution: (a) Wboy = F ll x W = (165 N)(12 .0 m) = 1980 J (b) Wfriction = F k x W = (55 .0 N)(12.0 m) = 660.0 J (Work of friction is negative) (c) Wnet = Fnet x (Σ F) x = (165N - 55.0 N)(12.0 m) = 1320 J (d) (Σ F) x = (K.E.) f - (K.E.) i 1320 J = (1/2)(45 .0kg) Vf 2 - (1/2)(45 .0kg) (0)2 Vf = + 7.66 m/s
  • 32. The Law of Conservation of Energy This law states that: "Energy is conserved. It is neither created nor destroyed. It converts from one form to another".
  • 33. Conservation of Mechanical Energy Example : In the following figure, neglecting friction, find the speed Of the 750-kg car at the bottom of the hill . Suppose the car is put in neutral and starts from rest from the top of the hill . V=0, M=750 kg 45 m
  • 34. Conservation of mechanical energy: Total Energy at A = Total Energy at B (K .E .)A + (P .E .)A = (K .E .)B + (P .E .)B (1/2)MVA 2 + M g hA = ( 1/2)MVB 2 + M g hB VA = 0 and hB = 0 M g hA = ( 1/2)MVB 2 g hA = (1/2)VB 2 2 g hA = VB 2 VB = 30 m/s A BhA hB = 0 VB
  • 35. Example : In the following figure, if 120,000 J of energy is consumed by frictional forces, find the speed of the 750-kg car at the bottom of the hill . Suppose the car is put in neutral and starts from rest from the top of the hill . frictional Energy=120,000 J In this case, part of the available energy will be wasted by friction
  • 36. Conservation of mechanical energy: Total Energy at A - W friction= Total Energy at B (K .E .)A + (P .E .)A - Wfriction = (K .E .)B + (P .E .)B (1/2)M A 2 + M g hA -120,000J = ( 1/2)MV B 2 + M g hB V A = 0 and h B = 0 M ghA -120,000J = ( 1/2)MV B 2 (750)(9 .8)(45) J - 120,000 J = 0 .5(750 kg)VB 2 562(m/s) 2 = VB 2 VB = 24 m/s V=0, M=750 kg
  • 37. Example: In the figure shown, find (a) the work done by the frictional force on the car as it coasts down the hill in neutral (b) the energy loss due to friction (c) the speed of the 750-kg car (VB) at the bottom of the hill . 400 m
  • 38. Solution: (a) The work done by friction is W friction = F k x W friction = ( -300N)(400m) = -120,000 J (b) -120,000 J (c) Conservation of mechanical energy: Total Energy at A - Wfriction = Total Energy at B (K .E .)A + (P .E .)A - Wfriction= (K .E .)B + (P .E .)B (1/2)MVA 2 + M g h A - 120,000 J = (1/2)MVB 2 + M g hB VA = 0 and hB = 0 M ghA -120,000 J = (1/2)MVB 2 (750)(9.8)(45) J - 120,000 J = 0.5(750)VB 2 [562(m/s)]2 = VB 2 VB = 24 m/s
  • 39. Power is defined as the work done per units of time. Mathematically: The (SI) unit for power is : The industrial unit: hp Power t W P   = Wattcalled s J s ftlb hphP  == 5501andwatts7461
  • 40. Example : An electric motor is capable of delivering 7 .2 Million Joules of work in one hour and 400.0 seconds. Find the power of the motor in watts, kilowatts, and hp . Solution: P = W/t P = (7 .2 x10 6 J )/(4000 s) = 1800 J/s = 1800 watts P = 1.8 kilowatts (kw) P = (1800/746 ) hp P = 2.4 hp
  • 41. Example: Calculate the amount of work or energy that a 4.50 hp electric motor can deliver in 10.0 hours. Solution: P = 4 .5hp = (4 .50)(746 watts) = 3360 watts or ( J /s ) P = W / t W = Pt W = (3360 J/s)(36,000s) = 1.21 x 10 8 J
  • 42. Efficiency: When a device receives power from a source, it does not deliver all of it in the intended form and converts a portion of it to other undesired forms. This makes a device to be less than 100 percent efficient. Most power plants have efficiencies of under 50 percent. A good nuclear power plant is about 45% efficient . Early coal plants were hardly 20% efficient . Eff. = Pout /Pin
  • 43. Example : A 1.25 hp electric pump with an efficiency of 92.5% is used to perform 1 .40 Mega Joules of work. (a) How long does it take for the electric pump to do the job ? (b) If it was 100% efficient , how long would it take? Solution: A 1.25 hp electric pump means it draws 1 .25 hp of electric power from the source. It generally cannot give back all of it . Make sure that you write the formulas with horizontal fraction bars . Eff. = P out / P in 0 .925 = P out / (1 .25 hp) P out = 0 .925(1 .25hp) = 1.16 hp (a) P = W / t t = W / P t = (1 .40 x 10 6 J) / ( 1 .16 x 746 watts ) = 1620 sec (b) P = W/t t = W/P t =(1 .40 x 10 6 J)/( 1 .25 x 746 watts ) = 1500 sec
  • 44. Example: Calculate (a) the necessary power to empty a swimming pool with dimensions (12m)(25m)(2 .4m) by pumping its water to an average height of 3.5m in 2.5hrs . The mass density of water is 1000 kg/m 3. (Hint: The power you calculate is the power that the electric pump has to deliver to water, Pout) . If the efficiency of the electric pump used is 88% , calculate (b) the electric power that the electric motor pulls from the power source, Pin .
  • 45. Solution: V = w. l. h V = 720m3 r = M / V M = r V M = (1000 kg/m 3)(720 m3) = 720,000 kg (a) P = W / t W = F x F = the weight of water= Mg x = height P = (F x) / t P = ( Mg x) / t P = (720,000kg )( 9 .8 m/s 2 )( 3 .5m ) / (2 .5 X 3600s ) = 2700 watts P = 2.7kw P = (2700 / 746) hp = 3.6 hp (b) Eff. = P out / P in 0 .88 = 2700watts / P in P in = 2700watts / 0 .88 = 3100 watts
  • 46. Another Version of Power Formula: P = W / t W = F x P = (F x) / t (x / t )= v P = F v This means that power is equal to force times velocity (if both of force and velocity are in the same direction). As you see the product of velocity and force is a constant if a constant power is available . When P is constant, the product F ∙v is constant . When a greater F is needed, a smaller v is attainable and vice versa .
  • 47. Example : A car is using 56 hp of its total power. When it is going up a steep hill, a force of 4200 N is needed for constant velocity motion of it up that hill. When it is traveling along a level and horizontal road, a force of 1200 N is needed for its constant velocity motion. Find the velocity of the car in each case . P = F v 56 hp 56 hp F= 4200 N F=1200 N
  • 48. Solution: P = (56)(746 watts) = 42000 watts (a) P = F v v = P / F v = 42000 watts / 4200N = 10 m/s (b) P = F v v = P / F v = 42000watts / 1200N = 35 m/s
  • 49. problems 1 through 5 chapter 6