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文檔簡介
Lectures
3
and
4(第三,四講)Newtonian
Mechanics
(
力學(xué))【
or
Newtonian
dynamics
(
動(dòng)力學(xué))】In
Newtonian
dynamics(動(dòng)力學(xué))------------Chapters
5-6:the
effect
offorces
acting
on
objects(作用在物體上的力)will
be
the
main
concern.Newtonian
Kinematics(運(yùn)動(dòng)學(xué))-------------chapters
2-4:Only
Dealswiththe
relationships
among
position(x),velocity(v),and
acceleration(a)andtime
(t).
Four
variables
(x,
v,
a,
t).Under
what
circumstances
Newton’s
2nd
law
holds:??
=
??????
≠
????---------------------inertial
reference
frame (慣性參考系中成立)---------------------Non-inertial
reference
frame(非慣性參考系中不成立)University
Physics
I1Q:
What
is
the
cause
for
the
changeof
the
status
of
motion
of
an
object?A:
It
is
the
force
exerting
on
it.In
Newtonian
dynamics(動(dòng)力學(xué),Chapters
5-6):the
effect
of
forcesacting
on
objects(作用在物體上的力)will
be
the
main
concern.University
Physics
I2Lectures
3(第三講):If
objects
are
very
small
(at
atomic
10-10
m
or
nano
10-9m
scale),Newtonian
mechanics
must
be
replaced
byquantum
mechanics(量子力學(xué)).Chapter
5
Force
and
Motion
(I)
Newtonian
Mechanics
describes
therelationship
between
force
and
motion
basedon
the
laws
discovered
by
British
physicistSir
Isaac
Newton
(1642-1727,明末清初).《自然哲學(xué)的數(shù)學(xué)原理》1687(
)At
very
high
speeds
(an
appreciable
fraction
of
the
speed
oflight
c),
Newtonian
mechanics
must
be
replaced
byEinstein’s
special
theory
of
relativity(
狹義相對論).University
Physics
I3ForceForce
causes
the
acceleration
of
an
object(or
changes its
momentum).Force
can
be
exerted
on
an
object
by
otherobjects,either
physically
touched(如繩子拉力)or
at
a
distance(如電磁力).Force
is
a
vector
tywith
bothmagnitudeand
direction.University
Physics
I4Net
Force(凈力)University
Physics
I5Net
force
is
the
sum
of
allforces
on
a
body.Net
force
is
an
overall
effect,
not
a
real
force.In
the
case
of
??net
=0,the
forces
cancel
with
each
other;a
status
called
equilibrium(平衡狀態(tài)).But
each
individual
force
still
exists.Only
the
net
effect
on
the
body
is
like
no
forces
on
it
atall.Principle
of
superposition
for
force(力的疊加原理)1.Newton’s
Law
(Law
of
Inertia,慣性定律)If
no
net
force
acts
on
a
body
(
??net
=
0
),
then
the
body‘svelocity willnot
change(or
to
say
its
momentum,
p=mv,
will
not
change);
that
is,
the
body
cannot
beaccelerated.Newton’s
Law
(
第一定律--Law
of
Inertia,慣性定律):Given
all
forces
on
a
body
balance
one
another,if
the
body
is
at
rest
(stationary ),
it
stays
at
rest;if
it
is
moving(運(yùn)動(dòng)),it
continues
to
move
at
constant
velocity.In
such
cases,
thebody
is
called
in
equilibrium(平衡).University
Physics
I67Draw
Free-Body
Diagram(分析受力圖)In
a
coordinate
system,
we
represent
the
body
as
a
dot,
eachforce
on
the
body
is
a
vector
arrow
with
its
tail
on
the
body.External
force(外力):A
collection
of
two
or
more
bodies
iscalled
a
system(質(zhì)點(diǎn)系),and
any
force
on
the
bodies
insidethe
system
from
bodies
outside
the
system
is
called
anexternal
force.Internal
force(內(nèi)力):are
forces
between
two
bodies
inside
thesystem.Internal
forces
cannot
accelerate
the
system.If
the
bodies
are
rigidly
connected,
then
we
can
treat
thesystem
as
one
composite
body,
and
the
net
force
??net
on
it
isthe
vector
sum
of
all
external
forces.University
Physics
I8Sample
ProblemIn
a
two-dimensional
tug-of-war(拉力比賽,拔河),Alex,
Betty,and
Charles
pull
horizontally
on
an
automobile
tire
at
theangles
shown
in
the
overhead
view
of
the
figure.The
tire
remains
stationary( )
in
spite
ofthe
three
pulls.Alex
pulls
with
force
????
of
magnitude
220
N,and
Charles
pulls
with
force
????
ofmagnitude
170
N.The
direction
of
????
is
not
given.What
is
the
magnitude
of
Betty's
force
????
?Solution:
equilibrium(平衡狀態(tài))
FB
FA
FCFA
FB
FC
0A
C0
F
cos
133
F
cos
Force
components
in
x-axis:FBX
FAX
FCX0
(
220
N)(cos133
)
(170
N)
cos 170
N
91
(220
N)(cos133
)
cos
28.04F.B.D.Force
components
in
y-axis:A
CF
sin
133
F
sin
,90
)
F
sin(B
FB
(220
N)(sin
133
)
(170
N)sin
28.04FB
241
NTherefore,FBy
FAy
FCyF.B.D.University
Physics
I10Some
Particular
ForcesGravitational
force(引力or
重力),Normal
force(法向支撐力or正壓力),Frictional
force(摩擦力),Tension(
張力).University
Physics
I11The
Gravitational
Force(地球引力,重力)Magnitude:Direction:Fg
mgPointing
towards
the
center
of
EarthThe
gravitational
force
????
on
a
body
is
the
forceexerted
by
Earth
to
pull
the
body
down
to
the
ground.General
Physics
I12Weight(重量):The
weight
W
of
a
body
is
equal
to
the
magnitude
of
thegravitational
force
on
the
body.The
Normal
Force
(法向支撐力or正壓力)When
a
body
presses
against
asurface(表面),the
surface
(even
a
seemingly
rigid
surface)deforms(形變)and
pushes
on
thebody
with
a
normalforce,which
isperpendicular
to
the
surface.F.B.D.The
surface
deforms這個(gè)表面發(fā)生形變The
normal
forceis
perpendicular
tothesurfaceUniversity
Physics
I13Frictional
Force(or
friction
摩擦力)If
we
slide
or
attempt
to
slide
a
body
over
a
surface,
the
motion
isresisted
by
a
bonding
between
the
body
and
the
surface.
Theis
considered
to
be
a
single
force
??,
called
thefrictional
force,
or
simply
friction.This
force
is
directed
along
the
surface,
opposite
the
direction
ofthe
intended
motion.In
ideal
cases,to
simplify
situation,friction
is
assumed
to
benegligible(namely
“the
surface
is
frictionless”,稱作“光滑表面”).University
Physics
I14Tension
(張力)The
tension
force
pulls
on
a
bodyalong
a
taut
cord(繃緊的繩子).The
cord
is
often
assumed
to
be
massless
and
un-stretchable(不可拉伸).A
string
has
a
single
tension
force
.The
direction
depends
on
thebody
on
which
this
force
acts
upon.We
usually
assume
a
pulley(滑輪)to
be
frictionless
and
massless.The
tension
forces
at
the
two
ends
of
thecord
are
equal
in
magnitude152.
Newton’s
Second
Lawalong
that
same
axis,
and
not
by
forcecomponents
along
any
other
axis.The
netforce
on
abody
is
equal
tothe
product
of
the
body's
mass
and
the
acceleration
of
the
body.Fnet
ma
(Newton's
second
law)
.??net,??
=
??????,??net,??
=
??????
,??net,??
=
??????The
acceleration
component
along
agivenorthogonal
axis
iscaused
onlyby
the
sum
of
the
force
componentsThis
expression
of
Newton’s
2ndlaw
in
the
right
is
what
welearned
in
high
school
physics.More
scientifically,
we
can
say:Net
force
acting
on
an
objectchanges
its
momentum??
=
????,
or
force
equals
thechanging
rate
of
momentumwith
respect
to
time,
i.e.????【??
=????
=??????(????)????=
??
????
=
??????
=
????????第二定律16University
Physics
I17Unit
of
Force(力的單位)In
SI
unit,the
unit
of
force
is
newton.1N
(1kg)
(1
m/
s2
)
1
kgm/
s2General
Physics
I18MassThe
mass
of
a
body
is
an
intrinsic
characteristicthat
relates
a
force
on
the
body
to
the
resultingacceleration.Mass
is
a
scalar.It
is
a
measurement
of
an
object’s
inertia.The
greater
an
object’s
mass,
the
more
the
objectresists
being
accelerated.University
Physics
I193.
Newton’s
Third
LawWhen
two
bodies
interact,
the
forces
on
the
bodies
from
eachother
are
always
equal
in
magnitude
and
opposite
in
direction.Third-law
force
pair:
FBC
FCB??????
is
the
force
on
book
from
crate.??????
is
the
force
on
crate
from
book.Action
(force)equals
reaction
(force)---作用力等于反作用力General
Physics
I20Conceptual
Question:How
dose
a
horsetry
to
use
physicsto
esc
work!Applying
Newton’s
Laws
to
solve
problemsStep
1:
yze
the
forces
exerted
on
the
object
of
the
study.Draw its
free-body-diagram(畫受力圖)Step
3:
yze
its
status
of
motion(including
its
v,
a)
andfind
out
the
initial
conditions(找出初始條件)Step
2:Construct
a
coordinate
system(建立坐標(biāo)系)convenient
forposition
to
get
????
,
????Step
4:
Apply
Newton’s
2nd
law,to
establish
equationsforx-direction,
and
y-direction
to
get
????,
????University
Physics
I21Sample
Problem
5-3The
hanging
block
H
falls
as
the
sliding
block
S
accelerates
to
the
right.University
Physics
I22The
figure
shows
a
block
S
(the
Slidingblock)
with
mass
M
=
3.3
kg.
The
blockis
free
to
move
along
a
horizontalfrictionless
surface
such
as
an
air
table.The
block
on
the
table
is
connected
bya
cord
that
wraps
over
a
frictionlesspulley
to
a
second
block
H
(theHanging
block),
with
mass
m
=
2.1
kg.The
cord
and
pulley
have
negligiblemasses
compared
to
the
blocks
(theyare
“massless”).HS23Find
(a)
the
acceleration
of
the
sliding
block,the
acceleration
of
the
hanging
block,
andthe
tension
in
the
cord.SOLUTION:F.B.D.The
cord
is
taut.
Therefore,
twoblocks
have
the
same
magnitudeof
acceleration
??
along
the
cordat
any
moment.The
Acceleration
of
block
S
pointsto
the
right;
acceleration
of
blockH
points
downward.Tensions
at
two
ends
of
the
cordhave
the
same
magnitude
??.University
Physics
I24T
Maponent
of
block
S:g
13
NM
mM
mT
M
ma
m
g
3
.
8
m
/
s
2If
??
→
0,
??
and
?? →
0.ponent
of
block
H:T
mg
m(a)Two
unknown
variables
,T
and
??,can
be
solved??
→
0,
??
→
0,
and
??
→
??.25Sample
Problem
5-4Like
ndulum(單擺),a
small
ball
withmass
of
m
connected
to
a
cord
of
length
lis
released
from
horizontal
level(??=0°).??
=
0°????????????????
cos
??
=
??????
=
??????????-------Eq1Along
tangent(切向):Along
normal(法向)(or
radial徑向):??
???? ?
????
sin
??
=
???? =
????2??----Eq2??
=
??1What
will
be
the
speed
of
the
ball
whenthe
cord
sweeps
an
angle
of
??
=
??1?What
is
the
tension
force
of
the
cord
atthis
angle
of
??
=
??1From
Eq.1,
we
can
obtain
how
the
speed
varies
with
the
angle??
=
0°????????????Along
tangent(切向):
????
cos
??
=
??????
=
????????????
=
??1So
that
????
= ??
cos
??
????????
=
??????
=
??????????????
= ??
cos
??
????
= ??
cos
??????
=??
cos
??????????So
that
??????
=
????
cos
??
??????Integrate
both
sides:??
??????
=0??
????
cos
??
????02We
get:
1??2
=
????
sin
??,→
??
= 2????
sin
??1.
What
will
be
the
speed
of
the
ball
when
the
cord
sweeps
an
angle
of
??
=
??1?26Since
????
=
?????? →
????
=
????/??,also
the
arc
length
????
=
??????From
Eq.2,
we
can
obtain
how
the
tension
of
thecord
at
the
angle
of
θ??
=
0°??????????????
=
??1????
=
??????
=
??????????Replace
v
by
the
previous
result
??
=2????
sin
??Along
normal(法向),or
radial(徑向):??
???? ?
????
sin
??
=
???? =
????2??We
get:
????
=
3????
sin
?????? =
????
sin
??
+
????2??2.
What
is
the
tension
force
of
the
cord
at
this
angle
of
??
=
??1When
??
=
0°, ????
=
0When
θ
=
90°,
????
=
3????27General
Physics
I28Sample
Problem
5.06 Force
withinan
elevator
cabIn
the
figure, senger
of
mass
??
=
72.2
kgstands
on
a
platform
scale
in
an
elevator
cab.
Weare
concerned
with
the
scale
readings
when
thecab
is
stationary,
and
when
it
is
moving
up
ordown.F.B.D.Find
a
general
solution
for
the
scale
reading,
whateverthe
vertical
motion
of
the
cab.Fnet
N
mg
maN
m
(g
a)??
=
??,??
=
????,when
the
cab
is
stationary
or
moving
at
constant
velocity??
>
??,??
>
????,when
the
cab
is
accelerating
upward.??
<
??,??
<
????,when
the
cab
is
accelerating
downward.(4)
??
=
???,??
=
??,which
is
called
weightless(失重).N
m
(g
a)The
scale
reading
isWhat
if
??
????
????????
????????
?
??
?
(??
<
???)University
Physics
I29Setting
up
rectangular
coordinate
systems
and
solving
problemsUniversity
Physics
I30Coordinate
systems
can
be
arbitrarily
(or
intentionally)
set
upto
solve
physical
problems.But
selecting
a
correct
one
should
be
more
convenient
insolving
problems.Physical
phenomena
(results
or
solutions)should
beindependent
on
the
intentionally
selected
coordinate
systems.物理結(jié)果與怎樣選取坐標(biāo)系應(yīng)該是無關(guān)的!Sample
ProblemA
cord
holdsstationary
a
blockof
mass
m
=
15
kg,on
a
frictionlessplane
that
isinclined
at
angleθ=
27°F.B.D.We
now
cut
the
cord.As
the
block
then
slides
down
the
inclined
plane(斜面),does
itaccelerate?If
so,what
is
itsacceleration?Think?There
is
no
movement
of
the
sliding
block
perpendicularto
the
inclined
plane.
Therefore,
Acceleration
must
beparallel
to
inclined
plane.31Fx
mg
sin
maxax
gsin
(9.8
m/s2
)
(sin
27
)=?4.4
m/s2The
acceleration
points
down
along
the
inclined
plane.ponent(Method
1)
We
choose
our
coordinate
system
with
axes
parallel
and
perpendicular
to
theinclined
plane.The
arrangement
aligns
mostforces
along
axes,
simplifying
theforceresolving
procedure32Method-2
Alternatively,
We
set
up
our
rectangular
coordinate
system
with
axes
along
horizontal
and
vertical
directions.There
is
no
movement
perpendicular
to
the
inclinedplane.Therefore,acceleration
??
must
be
along
theramp(斜坡),assuming
down
along
ramp.ponent????
=
????
=
???
sin
??????
=
???
cos
??ponent????
=
????
?
????
=
??
cos
??
?
????????
=
???
sin
????xy????University
Physics
I33??????We
get
the
same
answer
for
acceleration
as
we
did
in
method-1.ponent????
=
?????????
sin
??
=
?????
cos
??(1)??
cos2
??
+
sin2
?? =
??
sin
????
=
??
sin
??(1)?
cos
??
+(2)?sin
????xySolving
in
horizontal-vertical
coordinate
systemUniversity
Physics
I34ponent(2)????
=
????????
cos
??
?
????
=
??(???
sin
??)??
????????Under
what
circumstances
Newton’s
2nd
law
holds:1.
??
=
????---------------------inertial
reference
frame
(慣性參考系中成立)2.
??
≠
????---------------------Non-inertial
reference
frame(非慣性參考系中不成立)University
Physics
I3536Inertial
Reference
Frames(慣性參考系)An
inertial
reference
frame
is
one
in
which
Newton's
laws
hold.(??
=
????)A
reference
framewith
acceleration【有加速度的參考系,
including
rotatingframe(旋轉(zhuǎn)的參考系,即是有向心加速度)】is
anon-inertial
reference
frame(非慣性參考系)e.g.
an
accelerating
elevator
is
a
non-inertial
frame.A
reference
frame
at
rest(
的)orwith
constant
velocity(或勻速運(yùn)動(dòng)的)is
an
inertial
reference
frame(慣性參考系).Ground
is
usually
assumed
as
an
inertial
frame,
neglecting
Earth’sastronomical
motion.Observing
from
a
non-inertial
referenceframe(非慣性參考系),Newton‘s
laws
do
not
hold(
定律不成立)-----to
discuss
it
laterUniversity
Physics
I37As
the
saying
goes:水火不相容?Conclusion:There
is
no
absolute
correctness
or
absolute
truth,except
this
statement(沒有絕對真理).Correctness
is
relative(真確性都是相對的)Newton‘s
2nd
law
is
true
(??
=
????),if
it
is
observed
in
inertial
frame(
定律在慣性參考系中是真理)In
non-inertial
reference
frame,it
is
not
true!(在非慣性參考系中,
定律不是真理)True
gold
does
not
fear
the
fiery
真金不怕火煉?Observing
from
a
non-inertial
reference
frame(非慣性參考系),Newton‘s
laws
do
not
hold(
定律不成立)What
does
“Newton‘s
laws
do
hold”
mean(
定律成立是什么意思)?If
there
is
a
net
force,there
is
an
acceleration----------有力就有加速度!(無力就無加速度)e.g.
Look
into
Newton’s
2nd
lawWhat
does
“Newton‘s
laws
do
not
hold”
mean(
定律不成立是什么意思)?2.
If
there
is
a
net
force,there
is
no
acceleration----------有力卻沒加速度(有受到凈力但不動(dòng))!1.If
there
is
no
force,there
is
an
acceleration---------------沒力卻有加速度(不受力卻會(huì)動(dòng))38Observing
from
a
non-inertial
reference
frame(非慣性參考系),Newton‘s
laws
do
not
hold(
定律不成立)e.g.
Look
into
Newton’s
2nd
law1.
If
there
is
no
force,there
is
an
acceleration---------------沒力有加速度!Bus
StopNo
horizontal
????
Observing
????Conclusion:without
force,
but
acceleratingi.e.
Newton’s
2nd
law
breaksNo
horizontal
????
Conclusion:without
force,
but
acceleratingi.e.
Newton’s
2nd
law
breaks39Observing
from
a
non-inertial
reference
frame(非慣性參考系),Newton‘s
laws
do
not
hold(
定律不成立)e.g.
Look
into
Newton’s
2nd
law2.If
there
is
a
net
force,there
is
no
acceleration----------有力沒加速度!AlexBettyCharlesAlex
asks
:
what
do
you
feel
at
the
bottom
of
your
feet?Betty
answers:
I
feel
some
force
acting
on
thebottom
of
my
feet?Alex:
Then
why
you
are
not
moving
towards
me?
Newton’s
law
does
not
hold?40General
Physics
I41
??
MGroundWedgeBlockmGiven
the
inclined
surface
ofthe
wedge
and
the
groundsurface
are
both
frictionless,wedge
and
the
blockfind
accelerations
of
thewithrespect
to
the
ground.Tutorial
problem
1(相對運(yùn)動(dòng)---chapter4)As
shown
in
figure,
a
block
of
mass
m
is
placed
on
the
inclinedplane
of
a
wedge.
The
wedge
is
then
placed
on
the
ground.The
mass
of
wedge
is
M
and
the
angle
between
its
inclinedsurface
and
ground
is
??.What
about
the
case
that
two
objects
move
with
a
relative
acceleration?University
Physics
I
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