work energy and power - national chiao tung...
TRANSCRIPT
p. 1
交通大學 李威儀
Work
Energy
And Power
功,能量及功率
p. 2
交通大學 李威儀 黃河壺口瀑布
QUIZ #2
(1) An xx-kg man ascends a 10 m high staircase in yy sec. What is
his horsepower? ( g = 9.8 m/sec2 , 1 hp = 746 W )
p. 3
交通大學 李威儀 黃河壺口瀑布
QUIZ #2
(2) 請問:一個原點固定於地球表面上的參考座標是不是一個慣性座標?
如果不是,請問為什麼不是?
p. 4
交通大學 李威儀
p. 5
交通大學 李威儀
甚麼是 “能量” ?
p. 6
交通大學 李威儀
• W = F cos q • s ( Joule, a scalar )
= F • s or F • Dx
F : force , s : displacement , W : work
1 J = 1 N • 1 m = 1 ( kg m2 ) / s2
F
s
F
F cosq
q
要有出力才有“功”勞
造成位移才有“功”勞
常力所作的功 ( Work Done by a Constant Force )
p. 7
交通大學 李威儀
• W = F • s = ( Fx i + Fy j + Fz k ) • (Dx i + Dy j + Dz k )
= Fx Dx + Fy Dy + Fz Dz
W : mechanical work ( different from chemical work )
• F s W = 0
• negative work
FAB = – FBA , W = F • s
Won A by B ( negative work ) = – Won B by A ( positive work )
fk (friction on B)
A
B
s FBA
FAB
p. 8
交通大學 李威儀
• work done by kinetic friction
Wf = fk s cos180o = – fk s
• kinetic friction can also do positive work
fk (friction on B)
A
B
s FBA
FAB
B
A fk ( fk moves block A to the right also )
p. 9
交通大學 李威儀
DW = F • Dx = Fx • Dx
W = DW = Fx1 Dx + Fx2 Dx + …… + Fxn Dx
= Fxi Dx
as Dx 0
W = Fx dx or more generally W = F • ds
i =1
n
b
a
b
a
x
Fx
a b Dx
Fx1
Fx2
Fx3
等速率圓周運動
非常力所作的功 ( Work Done by Variable Force in 1-Dim )
p. 10
交通大學 李威儀
http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html
p. 11
交通大學 李威儀
F cause v change
v cause x change
W cause ? change
in one-dim. , const. force :
W = Fx Dx = ma Dx
v2 = vo2 + 2a Dx
a Dx = ½ (v2 – vo2 )
W = ½ mv2 – ½ mvo2
define kinetic energy ( K.E. ) : Ek = ½ mv2 ( joule, scalar )
Wnet = DEk : Work – Energy Theorem ( 功能定律 )
( Work-Energy Theorem still valid in 3-dim. space and with non-constant
forces. )
功與動能
動能 ( Kinetic Energy )
p. 13
交通大學 李威儀
Ex.
F
F cosq q
N
mg
m = 4 kg , q = 53o
F = 3 N , Dx = 2 m
vo = 3 m/s , mk = 1/8
Find (1) DEk , (2) vf
f
(1) Fy = 0 N = mg – Fsinq
DEk = WNet = WF + Wf
= Fx•s – mk N•s
= F cosq •s – mk ( mg – Fsinq )•s
= …… = 32 J
(2) D Ek = ½ mvf2 – ½ mvo
2 = 32 J , vo = 3 m/s
vf = 5 m/s
p. 14
交通大學 李威儀
p. 15
交通大學 李威儀
• An experiment by Galileo Galilei :
raise ball from C A , do work W
AC , gain K.E. = W, reach vmax
CB , K.E. = 0 ( A and B same height )
BCA, K.E. = 0
where does K.E. go at A and B ?
A B
C
位能 ( Potential Energy )
p. 16
交通大學 李威儀
vf vo
v = 0 , K.E. = 0
vo = vf
p. 17
交通大學 李威儀
vf vo
v = 0 , K.E. = 0
vo = vf
• potential energy ( P.E., Ep) : energy associated with the relative
positions of two or more interacting particles
Earth
p. 18
交通大學 李威儀
Example :
do work ( W ) to raise the apple
Changes the apple-earth
relative position
Changes the apple-earth
system’s potential ( or
the apple’s potential )
vmax
Fext
earth surface
release the apple
stored P.E. K.E.
If one raises the apple at const. speed ( K.E. unchanged )
Wext = D ( P.E. ) = Epf - Epo
p. 19
交通大學 李威儀
Wext
changes particles’ relative position
( pendulum and earth )
P.E. changed
K.E. ( 1/2 mvmax )
positive work increase in P.E. ( Ep )
Only changes in P.E. are important
Freedom to assign Ep = 0 configuration
Once the initial configuration for Ep=0 is defined :
The P.E. of a system is the external work needed to bring the
particles from the Ep=0 configuration to the given position at a
const. velocity ( or speed ).
2 A B
C
earth
如何計算一個系統中的位能 ?
p. 20
交通大學 李威儀
• Gravitational Potential Energy (near the earth’s surface)
external work done to move m
from yi to yf at a const. velocity
( Wnet = Wext + Wg = 0 = DEk )
Wext = Fext • s , | Fext | = mg
( mg 為此 apple/earth 雙粒子系統內力 )
Wext = Fext • s , | Fext | = mg
= mg ( yf – yi ) = mgyf – mgyi = DEp
= Ep( yf ) – Ep( yi )
Define Ep = 0 at yi = 0 Ep( yf ) = mg yf Ep(y) = mg y
Fext
yi
yf
mg
earth surface
p. 21
交通大學 李威儀
• Spring Potential Energy
Hooke’s Law : Fsp = - k x , k : spring constant
x xf
kxf
F
p. 22
交通大學 李威儀
伽利略
看遠處的大東西
虎克
看身邊的小東西
http://micro.magnet.fsu.edu/optics/timeline/people/hooke.html
http://s593.photobucket.com/albums/tt16/shernap05_bucket/DPS/?action=view&
current=hooke.jpg&newest=1
p. 23
交通大學 李威儀
p. 24
交通大學 李威儀
Move the spring from x = 0 to xf at a constant speed :
W = F • ds = ½ k xf2
define Ep,sp = 0 at x = 0 Ep,sp = ½ k xf2
Ep,sp = ½ k x2
• Spring Potential Energy
Hooke’s Law : Fsp = - k x , k : spring constant
Fsp
b
a
x xf
kxf
F
http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html
p. 25
交通大學 李威儀
• Work changes
the velocity of the particle DEk
the relative positions of particles DEp
• Inversely :
Energy is a measure of the particle’s, or
the particle system’s, capability to perform work ( on others )
甚麼是 “能量” ?
p. 26
交通大學 李威儀
• mechanically conservative system ( 機械守恆系統 ) : no energy enters
or leaves the system ( e.g. heat, radiation, work by external force,
work done by internal chemical reaction )
能量守恆 ( Energy Conservation )
p. 27
交通大學 李威儀
• mechanically conservative system ( 機械守恆系統 ) : no energy enters
or leaves the system ( e.g. heat, radiation, work by external force,
work done by internal chemical reaction )
• In a mechanically conservative system :
Ek + Ep = const.
( Ek + Ep )initial = ( Ek + Ep )final
½ mv22 + mg y2 = ½ mv1
2 + mg y1 y1
y2
v2
v1
earth
A system of 2 particles ( apple & earth)
能量守恆 ( Energy Conservation )
p. 28
交通大學 李威儀
p. 29
交通大學 李威儀
There are other forms of energy : e.g. thermal energy
( Actually, in microscopic scale, thermal energy may also be a kind
of kinetic energy )
摩擦力與功能定律
A B
C
earth
p. 30
交通大學 李威儀
從位能
轉換為動能
動能
再轉換為電能
2003 三峽大壩
p. 31
交通大學 李威儀
The ball on which track will hit the finish line earlier ?
p. 32
交通大學 李威儀
• mechanical power
Pav = DW / Dt ( J / s ) , 1 J/s = 1 watt ( W ) , 1 hp = 746 W
lim DW/Dt = P = dW/dt
DW = F • Ds dW = F • ds
v = ds / dt
P = dW / dt = F • ds / dt = F • v
Ex. A tractor exert 3 x 104 N, moving at 5 m/s. What is its horsepower ?
Dt0
功率,機械功率 ( Mechanical Power )
P = F • v = 3 x 104 x 5 = 1.5 x 105 ( W ) 200 ( hp )