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Sound Absorption Treatment for Transformer Substations
NA'I'IOEiAT, FESE.AhCId COTJJ.ICIL
CAN
AT!AD I V I S J O N Ob' H i T I L D I A ~ G RESUI4BCH
SOUIiD ABSOftPTICPI 'llHEAT~d~hMT
F O R TRAN SF(jHMi3R 51SBST14TICbS
by
T.D,
Northwood R e p o r t No,74
o f t h e D i v i s i o n o f B u i l d i n g Research Ottawa August 1955The Division of Building Research was requested
by a large public utility to investigate ways in which sound
absorbing materials and constructions might be used
In
the
control of the noise produced by substation power trans-
formers. The Building Physics Section has demonstrated that
the Helmholtz Resonator Principle can be employed and has
proposed several constructions which have now been evaluated
in the laboratory. Data on
a
number of practical forms of
materials have been obtained. The materials and construc-
tions evaluated were selected in the first irastance with
the practical requirements of the specific problem
in
mind.
The results obtained may be of interest iri connection with
similar problems elsewhere as well
as
in a number of other
cases in which noises arising from sixty-cycle power
are
involved.
Ottawa,
August 1955.
N.B. Hutcheon,
SOUND ABSORPTION TREATMENT
FOR
TRANSFORMER SUBSTATIONS by T. D. NorthwoodThe n o i s e produced by s u b s t a t i o n power t r a n s f o r m e r s c o n s t i t u t e s a s p e c i a l a c o u s t i c a l problem f o r two r e a s o n s :
a ) t h e most i m p o r t a n t components i n t h e n o i s e a r e a t 120 c y c l e s p e r second and i t s lower harmonics, a r e g i o n f o r which c o n v e n t i o n a l a c o u s t i c a l m a t e r i a l s a r e i n e f f i c i e n t ;
b ) t o f a c i l i t a t e c o o l i n g t h e t r a n s f o r m e r s t h e y a r e u s u a l l y o n l y p a r t i a l l y e n c l o s e d , s o t h a t any a c o u s t i c a l t r e a t m e n t
i n t r o d u c e d s h o u l d be w e a t h e r p r o o f .
The o b j e c t of t h i s s t u d y was t o develop sound a b s o r b i n g systems t o meet t h e s e s p e c i a l r e q u i r e m e n t s .
DESIGN
PROCEDUREA b s o r p t i o n a t low f r e q u e n c i e s i s most r e a d i l y o b t a i n e d w i t h some t y p e of r e s o n a n t system t u n e d t o t h e f r e q u e n c y r a n g e
i n which a b s o r p t i o n i s r e q u i r e d , The system a d o p t e d i n t h i s
p r o j e c t f o l l o w e d t h e p r i n c i p l e of t h e Helmholtz Hesonator, employ- i n g a n a i r c a v i t y coupled t o t h e sound f i e l d by means o f a n
o r i f i c e .
I n p r i n c i p l e one might t a k e c a r e of a few d e f i n i t e f r e q u e n c i e s by u s i n g r e s o n a n t e l e m e n t s s h a r p l y t u n e d t o e a c h o f t h e f r e q u e n c i e s , However, s e v e r a l f a c t o r s make c r i t i c a l t u n l n g a n i m p r a c t i c a l p r o c e d u r e . The a l t e r n a t i v e i s t o i n t r o d u c e enough damping i n t h e system t o p r o v l d e moderate a b s o r p t l o n o v e r t h e r e q u i r e d f r e q u e n c y r a n g e , I n t h e p r e s e n t work t h e r a n g e 120 t o
360
c y c l e s was c o n s i d e r e d i m p o r t a n t , w i t h s p e c i a l a t t e n t i o n t o 120 c y c l e s . Damping was a c h i e v e d by u s i n g m o d e r a t e l y porous m a t e r i a l s f o r c o n s t r u c t i n g t h e r e s o n a t o r .Four s t r u c t u r e s were examined a s p o s s i b l e a b s o r b e r s : Type A c o n s i s t e d of a s e r i e s of c a v i t i e s f a c e d w i t h a porous membrane, t h e p o r o s i t y of t h e membrane b e i n g i n t e n d e d t o a c t a s a n o r i f i c e and a l s o a s a damping e l e m e n t . It was
proposed t o u s e a t h i n l a y e r o f Limpet s p r a y e d on expanded m e t a l l a t h . However, i t was found d i f f i c u l t t o o b t a i n t h e r e q u i r e d p r o p e r t i e s w i t h Limpet, and t h e system was abandoned;
-e B c o n s i s t e d of a c a v i t y w a l l i n which t h e i n n e r l e a f c o n s i s t e d of
4-
by8-
by 1 6 - i n c h b u i l d i n g b l o c k s . The ends of t h e b l o c k s , i . e , t h e v e r t i c a l j o i n t s , were l e f t s p a c e dDamping i s provided by making t h e i n n e r l e a f of expanded s l a g o r o t h e r p o r o u s b l o c k s . For b e s t performance i n a random sound f i e l d t h e c a v i t y s h o u l d be p a r t i t i o n e d i n t o c e l l s
4
f e e t s q u a r e o rs m a l l e r , During t h e development i t was found t h a t c a v i t y b e a r i n g w a l l s a r e n o t a c c e p t a b l e i n some c i t i e s , i n c l u d i n g Toronto, and
t h e development was, t h e r e f o r e , c u t s h o r t , However, t h e system may be u s e f u l a s a l i n i n g i n e x i s t i n g s t a t i o n s where b e a r i n g w a l l r e q u i r e m e n t s a r e a l r e a d y met, R e v e r b e r a t i o n t e s t s
( 1 1 ,
2 ( b ) and 2 ( c ) ( T a b l e 11) e x e m p l i f y t h i s t y p e of s t r u c t u r e ; !LJpe C c o n s i s t e d o f hollow b u i l d i n g b l o c k s w i t h h o l e s d r i l l e d i n t o t h e i n d i v i d u a l c e l l s . The p r o c e d u r e was t r i e d s u c c e s s f u l l y w i t h s e v e r a l t y p e s of expanded s l a g and c i n d e r b l o c k s o R e s u l t s a r e g i v e n i n T a b l e s I1 and 111; T e D was s i m i l a r t o Type C e x c e p t t h a t t h e p a r t i c u l a r%--
block, a l i g t w e i g h t c i n d e r block, was s o porous t h a t i t w a s
u n n e c e s s a r y t o d r i l l h o l e s i n t o t h e c e l l s , R e s u l t s a r e g i v e n i n T a b l e 11, t e s t No.
3 ,
( U n f o r t u n a t e l y t h e block was found t o be n o t s t r o n g enough f o r b e a r i n g w a l l p u r p o s e s ) .T e s t R e s u l t s
Impedance t u b e t e s t s were made on n i n e samples o f b u i l d i n g b l o c k s t o p r o v i d e d e s i g n d a t a and a l s o t o p r o v i d e com- p a r a t i v e i n f o r m a t i o n on a v a i l a b l e b l o c k s ,
I
F o r a d e s c r i p t i o n of t h e samples s e e Table I ) . C i r c u l a r d i s c s 2* i n c h e s i n d i a m e t e r were t a k e n from e a c h sample and f i t t e d i n t o a h o l d e r a t t a c h e d t o t h e impedance t u b e , Absorption measurements were t a k e n on t h e d i s c i t s e l f , on a p a i r of d i s c s w i t h a c a v i t y between them, t o s i m u l a t e a h o l l o w b l o c k , and on t h e same arrangement w i t h a h o l e t h r o u g h t h e f r o n t d i s c , The impedance t u b e d a t a a r e summarized i n T a b l e 111,C o n c u r r e n t l y w i t h t h e impedance t u b e t e s t s a few l a r g e - s c a l e t e s t s were made i n t h e r e v e r b e r a t i o n chamber, These r e s u l t s
a r e g i v e n i n Table 11,
There a r e s e v e r a l d i s t i n c t i o n s between t h e impedance t u b e measurements and r e v e r b e r a t i o n chamber measurements, The former measures a b s o r p t i o n f o r waves a t normal i n c i d e n c e o n l y , whereas t h e l a t t e r measures a b s o r p t i o n f o r waves a t a l l a n g l e s of
i n c i d e n c e , Also, t h e s i m u l a t e d c e l l s t e s t e d on t h e t u b e a r e o n l y a n a p p r o x i m a t i o n t o t h e f u l l - s c a l e s i t u a t i o n , s i n c e a b l o c k p r e s e n t s s o l i d web s e c t i o n s t o t h e sound f i e l d a s w e l l a s t h e hollow s e c t i o n s , F i n a l l y t h e r e may be d i f f e r e n c e s between t h e r e v e r b e r a t i o n measurements and a c t u a l i n s t a l l a t i o n s s l n c e t h e former were done w i t h o u t a c t u a l l y m o r t a r i n g t h e b l o c k s , For
example t h e r e may be a s i g n i f i c a n t r e d u c t i o n i n c e l l volume due t o m o r t a r f a l l i n g i n t o t h e c a v i t i e s ,
d a t a t h a t s t r u c t u r e s s i m i l a r t o T.ype
B,
C o r p o s s i b l y D can be d e s i g n e d u s i n g any s i m i l a r b u i l d f n g block, on t h e b a s i s of impedance t u b e measurements a l o n e , Recommendations 1) F o r new c o n s t r u c t i o n i t i s recommended t h a t b l o c k s s i m i l a r t o Samples No,4
t o 9 be i n c o r p o r a t e d fn t h e i n n e r f a c e of b e a r i n g w a l l s , and t h a t e a c h c e l l of e a c h b l o c k be p e r f o r a t e d w i t h a6
i n c h d i a m e t e r h o l e , Impedance t u b e t e s t s i n d i c a t e t h a t any of t h e b l o c k s t e s t e d have s a t i s f a c t o r y a b s o r p t i o n p r o p e r t i e s , Samples No,6
and No,4
head t h e l i s t ; sample No, 9 a p p e a r ss l i g h t l y i n f e r i o r , T h i s system s h o u l d p r o v i d e a b s o r p t i o n s a p p r o x i m a t e l y a s f o l l o w s : Frequenc y 1 2 0 240 360 A b s o r p t i o n c o e f f f c f e n t
.SO
t o ,a0 e 2 5 t o.35
,15
t o .20 2 ) A s a r u l e , f o r s i m i l a r a c o u s t i c a l m a t e r i a l s , t h e r e i s a c o r r e l a t f o n between h i g h a b s o r p t i o n and low d e n s i t y , However, t h e r u l e does n o t seem t o a p p l y h e r e , and i t i s recommended t h a t a n impedance t u b e t e s t be made b e f o r e a d o p t i n g a new b l o c k ,3 )
F o r non-bearing w a l l s a b l o c k s u c h a s Sample No,3
might be used w i t h o u t m o d i f i c a t i o n o r Sample No, 2 might be used i n a s t r u c t u r e o f Type B o r Type C,
4)
I n a l l c a s e s t h e w a l l s s h o u l d be c o n s t r u c t e d w i t h a break i n c e l l communication a t i n t e r v a l s of&
f e e t o r l e s s . T h i s c o u l d s i m p l y be done i n a T y p e C s t r u c t u r e , by i n c o r p o r a t i n g a s t r i p of w i r e mesh i n t h e o c c a s i o n a l m o r t a r j o i n t , c o v e r i n g t h e whole s u r f a c e w i t h m o r t a r . -TABLE
I
DESCRIPTION OF SAl'iPLES
sample 1 P e r l i t e b l o c k s
4"
x8" x
16";3
c e l l s ; weight p e r block 1 8 , s l b , Area c o r r e c t i o n a p p l i e d t o r e v e r - b e r a t i o n chamber d a t a t o make them comparable w i t h s t a n d a r d sample a r e a ,Sample 2 Cooper s l a g b l o c k s
4"
x8"
x 16";3
c e l l s ; weight p e r block1 7
o o
~ b ,Sample
3
Cooper l i g h t - w e i g h t c i n d e r b l o c k ,8" x
8" x 1611;3
c e l l s ; weight p e r block 25.5 l b ,Sample
4
Cooper c i n d e r block, 8" x8"
x 16";3
c e l l s ; weight p e r block 33.6 l b , One block t e s t e d .Sample
5
Hayley c i n d e r block,8"
x 8" x 16";3
c e l l s ; weight p e r b l o c k33.5
l b .Sample 6 Cooper s l a g b l o c k 8" x 8If x 16";
3
c e l l s , weight p e r b l o c k 37.2 l b o One b l o c k t e s t e d ,Sample
7
Maple c i n d e r b l o c k , 8"x
8"x
16";3
c e l l s ; weight p e r b l o c k 37*2 l b .Sample 8 Maple s l a g b l o c k , 8"
x
8"x
16";3
c e l l s ; weight p e r b l o c k 3 8 , s l b ,Sample 9 Toronto B r i c k c i n d e r b l o c k 8" x 8"
x
16'" weight p e rb l o c k
35e7
lboNote: Samples 2 and
3
were r e p o r t e d by t h e i n t e r e s t e d agency t o have f a i l e d t o meet a compressive s t r e n g t h t e s t , Samples4,
6 ,7,
8 and9
p a s s e d t h e compressive s t r e n g t h t e s t , Sample5
has n o t been t e s t e d ,TABLE I1
REVERBERATION
CHAMBEH
DATA
Frequency (c ,p , s o ) Absorbing System 1 2 5 250 500 1000 2000 4000 c o r r e c t e d f o r e f f e c t of s m a l l sample a r e a ) a ) l a i d f l a t on f l o o r b ) b l o c k s spaced