Downloaded From: cutt.ly/StudentsHelperBlog
, -
Stem
Downloaded From: cutt.ly/StudentsHelperBlog
, motion
Oscillatory
-
moves
bark &
forth repeatedly
↳
if a
body position
.
of
mean
the motion
about
pendulum vibratory
,
swinging spring
.
En to a
:
attached
mass
a
canal
that
repeats after
A motion
Motion :
Periodic
-
intervals of timea periodic
motion
.
.
is
motion
enanrlpk
Each oscillatory bird is also an
!t oscillatory
a
in
not
body moving
is
.
A but
motion ,
of periodic
pendulum
Sunny
: '
motion of simple
vibrating tuning fork motion
oscillatory
-
-
simplest form of
Its
outmagngnitudeonitof
is the
It
ofto force displace
magnitude
.
↳ where the
proportional
directly
1 %7
"'m
,
. pase
fan
• - •
←
tiding
f- O -
-
f- =0
forces
"
'T
=
propose.my
constant
we
Note :
cannot
apply
to 3 equations
← a
motion
¥ -0 of
n=O
✓ =D
↳ a
Downloaded From: cutt.ly/StudentsHelperBlog
, Kinematics
-
stem
of
f- = - kN
= -
Kk
ma
KI
differential
-
a =
the
M
This is called
sum
of
.
equation
DY team )
=
-
- Ci
( vcu ) alt)
acn)
-
→
)
nut -
- Asin lwttol) ftp.jtmmieondikpennk.at
equation
.
Iii)
in Ci) .
we
get
substituting
w =
tT4m
En :
dd¥= -
25g
d!nq=
war
Note : -
a sin ( sntcz
)
#
y
=
C, sin ( wt tcz
)
=
u
( wt +40 )
nlt) =
Asin
wat
ult) - Aw
cos ( wt too )
too)
÷ / F£alty= -
wzasin (
wt
THI
Ta a=_w
AN
Uman
Note
=
& ult)
NH)
Eliminating
t
from Aw
•
#
" "
¥
'
+
[ m=±wt¥
Downloaded From: cutt.ly/StudentsHelperBlog
, -
Stem
Downloaded From: cutt.ly/StudentsHelperBlog
, motion
Oscillatory
-
moves
bark &
forth repeatedly
↳
if a
body position
.
of
mean
the motion
about
pendulum vibratory
,
swinging spring
.
En to a
:
attached
mass
a
canal
that
repeats after
A motion
Motion :
Periodic
-
intervals of timea periodic
motion
.
.
is
motion
enanrlpk
Each oscillatory bird is also an
!t oscillatory
a
in
not
body moving
is
.
A but
motion ,
of periodic
pendulum
Sunny
: '
motion of simple
vibrating tuning fork motion
oscillatory
-
-
simplest form of
Its
outmagngnitudeonitof
is the
It
ofto force displace
magnitude
.
↳ where the
proportional
directly
1 %7
"'m
,
. pase
fan
• - •
←
tiding
f- O -
-
f- =0
forces
"
'T
=
propose.my
constant
we
Note :
cannot
apply
to 3 equations
← a
motion
¥ -0 of
n=O
✓ =D
↳ a
Downloaded From: cutt.ly/StudentsHelperBlog
, Kinematics
-
stem
of
f- = - kN
= -
Kk
ma
KI
differential
-
a =
the
M
This is called
sum
of
.
equation
DY team )
=
-
- Ci
( vcu ) alt)
acn)
-
→
)
nut -
- Asin lwttol) ftp.jtmmieondikpennk.at
equation
.
Iii)
in Ci) .
we
get
substituting
w =
tT4m
En :
dd¥= -
25g
d!nq=
war
Note : -
a sin ( sntcz
)
#
y
=
C, sin ( wt tcz
)
=
u
( wt +40 )
nlt) =
Asin
wat
ult) - Aw
cos ( wt too )
too)
÷ / F£alty= -
wzasin (
wt
THI
Ta a=_w
AN
Uman
Note
=
& ult)
NH)
Eliminating
t
from Aw
•
#
" "
¥
'
+
[ m=±wt¥
Downloaded From: cutt.ly/StudentsHelperBlog
