PHYSICS 5B Lecture Notes - Lecture 19: Normal Mode, Standing Wave, Sound

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9 Jun 2018
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Standing waves on astring
n =3 anti
nodes
§§÷"f¥¥
.tl?Eef..fMni#otnoaes=nti
nodes
L= nat
Xn= ¥
,
n=1,2 ,3,
... .
fn =¥
fn =n=L fundamental mode
wave motion on astretched string (ch 15 .3)
fgti |-
~
÷%ltt
"Tension
In the string ts
v=¥
mass per unit length
the 'Tis tangent to the are .
View as apart of acircle
Fr =The centripetal force
=2T Sino =2To small 0
S=20 .R
m= µ.s=µ1220
.:G =M2Rµ
Fr =2To =
ITTRIM
=IT
Fr =Ma =
M¥2
=
Ii
/
v2= F- v= FF
ex .In an experiment on Standing waves ,astring 92.4 cm long Is attitude to The prong of an electrically driven
tuning tork ,which vibrates perpendicular to the length of the string at frequency of 60 Hz .The mass of the string
is 44.2 g. .
How much Tension must the string under if it Is vibrated with 5nodes
tffhj :
"In's =421=2 ,
x= tz =92¥ =46.2 cm
V=If =0.462 ×60 =27.22 (%)
v= ,µ= It =80.942¥ =0.0478 lm
T= V2µ =(27.725 ×0.0478=36 .8N
Standing wave In music instruments
String :oscillations on
Strings
(guitar .piano ,violin ,harp )
.
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Document Summary

Standing waves on a string n =3 nodes anti. =l fundamental mode wave motion on a stretched string ( ch. In an experiment on standing waves a string. The prong of an electrically driven tuning tork which vibrates perpendicular to the length of the string at frequency of. 5 nodes n "s = 421=2 , x= tz = 92 = Strong standing waves pushthe surrounding air back and forth to produce sound wave f wind instruments. : standing waves in air columns flute . organs) i. mg@mnd. i. Xn= n pipe has a length of. The pipe is open at each end . what are. The three frequency determine in (a) if the pipe is closed at one end . The periodic varies in intensity at a given point of space due to the superposition of two waves having slightly different. Y , ( t ) yzlt ) sin. 2=2 sin ( a ) ( os ( a )

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