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Acoustical Engineering (Harry F. Olson).pdf
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VJ11

 

CONTENTS

 

 

 

 

CHAPTER

 

 

 

 

 

PAGE

5.15

ACOUSTICAL IMPEDANCE OF A CIRCULAR ORIFICE IN A WALL

 

 

OF INFINITESIMAL THICKNESS

••••..........

 

••••.••.....

99

5.16 ACOUSTICAL IMPEDANCE OF AN OPEN

PIPE WITH

LARGE

 

 

FLANGES ••.••.•..••..••••.•

...••.........

 

••••••••.....

99

5.17

HORNS •••••••.••.••••••••••••••••...

•.••••••••••••••••

100

5.18

FUNDAMENTAL HORN EQUATION ..•••••••.•........

•••.•

100

5.19

INFINITE

CYLINDRICAL HORN (INFINITE

PIPE) .......

•..

101

5.20

INFINITE

PARABOLIC HORN .......

•••••••••.•......

•••••

102

5.21

INFINITE CONICAL HORN •••..

•••.••••••.•••.•••••••••••

102

5.22

INFINITE EXPONENTIAL HORN •.•••..

•....

•••••••••••...

103

5.23

INFINITE HYPERBOLIC HORN ••••••...

••....

••.•••••••...

104

5.24THROAT ACOUSTICAL IMPEDANCE CHARACTERISTIC OF INFI­ NITE PARABOLIC, CONICAL, EXPONENTIAL, HYPERBOLIC AND

 

CYLINDRICAL HORNS •••.•.........

••••••••

........••..

104

5.25

FINITE

CYLINDRICAL HORN .......

•..•....

•........

•.•.•

105

5.26

FINITE

CONICAL HORN ••..•......

••.••.•.•..... ..

• •••..

 

106

5.27FINITE EXPONENTIAL HORN .•.••.••.•••••••.••••••••••• 108

5.28THROAT ACOUSTICAL IMPEDANCE CHARACTERISTICS OF FI­

 

NITE EXPONENTIAL HORNS •••••.........

•.•••••••••

....

110

5.29

EXPONENTIAL CONNECTORS .••••.••........

•.•••••••••.•

112

5.30

A HORN CONSISTING OF MANIFOLD EXPONENTIAL SECTIONS

114

5.31

CLOSED PIPE WITH A FLANGE .....••.•.•••..........

••.•

115

5.32

SOUND TRANSMISSION IN TUBES

•..••...

•.•........

•..

••

116

5.33

TRANSMISSION FROM ONE PIPE TO ANOTHER PIPE OF DIF­

 

 

FERENT CROSS-SECTIONAL AREA ......

•..

•..........

•••.•.

117

5.34

TRANSMISSION THROUGH THREE PIPES .....•••••••••....

 

119

5.35

TRANSMISSION FROM ONE MEDIUM TO ANOTHER MEDIUM..

120

5;36

TRANSMISSION THROUGH THREE

MEDIA

....•••••.•••..

• .

121

5.37TUBES LINED WITH ABSORBING MATERIAL •••••••••••...• 121

5.38RESPONSE OF A VIBRATING SYSTEM OF ONE DEGREE OF FREE­

 

DOM ..• ............

•.•..........

•....

.. • ...........

 

••

122

VI. DIRECT RADIATOR LOUDSPEAKERS

 

 

 

 

 

6.1

INTRODUCTION ••........

•••••••.•.....

... ••• . ••

..••...

124

6.2

SINGLE-COIL, SINGLE-CONE LOUDSPEAKER ....•.••.••.....

125

6.3

MULTIPLE, SINGLE-CONE, SINGLE-COIL LOUDSPEAKER •••...

137

6.4

SINGLE-COIL, DOUBLE-CONE LOUDSPEAKER

• .. ••• . •••••....

141

6.5

DOUBLE-COIL. SINGLE-CONE LOUDSPEAKER

• .........

 

••.••

143

6.6

DOUBLE-COIL. DOUBLE-CONE

LOUDSPEAKER .....

••

•..

••••.

143

6.7MECHANICAL NETWORKS FOR CONTROLLING THE HIGH FRE­

QUENCY RESPONSE OF A LOUDSPEAKER ••••••.•...•••.••••

147

A. Conventional Single-Coil Loudspeaker .. . . . . . . . . . . . ..

147

B. Loudspeaker with a Compliance Shunting the Cone

 

Mechanical Impedance ............................

148

C. Loudspeaker with a Compliance Shunting; a Compli­

 

ance and Mass in Parallel. Connected in Series with

 

the Cone Mechanical Impedance ...................

148

D.Loudspeaker with a "T" Type Filter Connecting the Voice Coil Mass and the Cone Mechanical Impedance 148

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