NEET  >  Important Formulae: Sound Waves

# Important Formulae: Sound Waves - Notes | Study Physics Class 11 - NEET

``` Page 1

Important Formulae
1.  Wave Speed
Speed of longitudinal wave

E
v ?
?

(a) In solids, E = Y = Young's modulus of elasticity

Y
v ?
?

(b) In liquids, E = B = Bulk modulus of elasticity

B
v ?
?

(c) In gases, according to Newton,
E = B
T
= Isothermal bulk modulus of elasticity = p

p
v ?
?

But results did not match with this formula. Laplace made correction in it. According to him,
E = B
S
= Adiabatic bulk modulus of elasticity = ? ?

p RT kT
v
Mm
? ? ?
? ? ?
?

2.  Effect of Temperature, Pressure and Relative Humidity in Speed of Sound in Air (or in a Gas)
(i) With temperature v ? T
(ii) With pressure Pressure has no effect on speed of sound as long as temperature remains
constant.
(iii) With relative humidity With increase in relative humidity in air, density decreases. Hence,
speed of sound increases.
3.  Sound Level (L)

10
0
l
L 10log
l
? (in dB)
Here, I
0
= intensity of minimum audible sound = 10
-12
W m
-2
. While comparing loudness of two
sounds we may write,

2
2 1 10
1
l
L L 10log
l
??
In case of point source,
2
21
2
12
lr 1
l or
r l r
??
??
??
??

Page 2

Important Formulae
1.  Wave Speed
Speed of longitudinal wave

E
v ?
?

(a) In solids, E = Y = Young's modulus of elasticity

Y
v ?
?

(b) In liquids, E = B = Bulk modulus of elasticity

B
v ?
?

(c) In gases, according to Newton,
E = B
T
= Isothermal bulk modulus of elasticity = p

p
v ?
?

But results did not match with this formula. Laplace made correction in it. According to him,
E = B
S
= Adiabatic bulk modulus of elasticity = ? ?

p RT kT
v
Mm
? ? ?
? ? ?
?

2.  Effect of Temperature, Pressure and Relative Humidity in Speed of Sound in Air (or in a Gas)
(i) With temperature v ? T
(ii) With pressure Pressure has no effect on speed of sound as long as temperature remains
constant.
(iii) With relative humidity With increase in relative humidity in air, density decreases. Hence,
speed of sound increases.
3.  Sound Level (L)

10
0
l
L 10log
l
? (in dB)
Here, I
0
= intensity of minimum audible sound = 10
-12
W m
-2
. While comparing loudness of two
sounds we may write,

2
2 1 10
1
l
L L 10log
l
??
In case of point source,
2
21
2
12
lr 1
l or
r l r
??
??
??
??

In case of line source,
21
12
lr 1
l or
r l r
??
??
??
??

4.  Doppler Effect In Sound

m0
ms
v v v
f ' f
v v v
?? ??
?
??
??
??

5. Beats
f
b
= f
1
- f
2
(f
1
> f
2
)
6.  Oscillations of Stretched Wire or Organ Pipes
(i) Open organ pipe
Fundamental tone or first harmonic (n = 1)

First overtone or second harmonic (n = 2)

Second overtone or third harmonic (n = 3)

v
fn
2l
??
?
??
??
. Here, n = 1,2, 3......
Even and odd both harmonics are obtained. Here, v = speed of sound in air.
v will be either given in the question, otherwise calculate from
RT
v
M
?
?
(ii) Closed organ pipe
Fundamental tone or first harmonic (n = 1)
Page 3

Important Formulae
1.  Wave Speed
Speed of longitudinal wave

E
v ?
?

(a) In solids, E = Y = Young's modulus of elasticity

Y
v ?
?

(b) In liquids, E = B = Bulk modulus of elasticity

B
v ?
?

(c) In gases, according to Newton,
E = B
T
= Isothermal bulk modulus of elasticity = p

p
v ?
?

But results did not match with this formula. Laplace made correction in it. According to him,
E = B
S
= Adiabatic bulk modulus of elasticity = ? ?

p RT kT
v
Mm
? ? ?
? ? ?
?

2.  Effect of Temperature, Pressure and Relative Humidity in Speed of Sound in Air (or in a Gas)
(i) With temperature v ? T
(ii) With pressure Pressure has no effect on speed of sound as long as temperature remains
constant.
(iii) With relative humidity With increase in relative humidity in air, density decreases. Hence,
speed of sound increases.
3.  Sound Level (L)

10
0
l
L 10log
l
? (in dB)
Here, I
0
= intensity of minimum audible sound = 10
-12
W m
-2
. While comparing loudness of two
sounds we may write,

2
2 1 10
1
l
L L 10log
l
??
In case of point source,
2
21
2
12
lr 1
l or
r l r
??
??
??
??

In case of line source,
21
12
lr 1
l or
r l r
??
??
??
??

4.  Doppler Effect In Sound

m0
ms
v v v
f ' f
v v v
?? ??
?
??
??
??

5. Beats
f
b
= f
1
- f
2
(f
1
> f
2
)
6.  Oscillations of Stretched Wire or Organ Pipes
(i) Open organ pipe
Fundamental tone or first harmonic (n = 1)

First overtone or second harmonic (n = 2)

Second overtone or third harmonic (n = 3)

v
fn
2l
??
?
??
??
. Here, n = 1,2, 3......
Even and odd both harmonics are obtained. Here, v = speed of sound in air.
v will be either given in the question, otherwise calculate from
RT
v
M
?
?
(ii) Closed organ pipe
Fundamental tone or first harmonic (n = 1)

First overtone or third harmonic (n = 3)

Second overtone or fifth harmonic (n = 5)

v
fn
4l
??
?
??
??
. Here, n = 1,3,5......
(a) Stationary transverse waves are formed in stretched wire and longitudinal stationary waves are
formed in organ pipes.
(b) Open end of pipe is displacement antinode, but pressure and density nodes. Closed end of pipe
is displacement node, but pressure and density antinodes.
(c) Laplace correction e =0.6r (in closed pipe) and 2e = 12 r (in open pipe)
Hence,
v
fn
2(l 12r)
??
?
??
?
??
(in open pipe) and
v
fn
4(l 0.6r)
??
?
??
?
??
(in closed pipe)
(iii) If an open pipe and a closed pipe are of same lengths then fundamental frequency of open
pipe is two times the fundamental frequency of closed pipe.
```

## Physics Class 11

127 videos|464 docs|210 tests

## Physics Class 11

127 videos|464 docs|210 tests

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