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971 

Federal Aviation Administration, DOT 

Pt. 36, App. H 

Position N represents the helicopter location 
on the measured approach flight path for 
which PNLTM is observed at measuring sta-
tion A, and N

r

is the corresponding position 

on the reference approach flight path. The 
measured and reference noise propagation 
paths are AN and AN

r

, respectively, both of 

which form the same angle, 

q

APP

, cor-

responding to PNLTM relative to their ap-
proach flight paths. 

(e) 

Correction of noise at source during level 

flyover.  (1) For level overflight, if any com-
bination of the following three factors, air-
speed deviations from reference, rotor speed 
deviations from reference, and temperature 
deviations from reference, results in a noise 
correlating parameter whose value deviates 
from the reference value of this parameter, 
then source noise adjustments must be de-
termined from the manufacturer’s data that 
is approved by the FAA. 

(2) Off-reference tip Mach number adjust-

ments must be based upon a sensitivity 
curve of PNLTM versus advancing blade tip 
Mach number, deduced from overflights per-
formed at different airspeeds surrounding 
the reference airspeed. If the test aircraft is 
unable to attain the reference value, then an 
extrapolation of the sensitivity curve is per-
mitted if data cover at least a range of 0.03 
Mach units. The advancing blade tip Mach 
number must be computed using true air-
speed, onboard outside air temperature, and 
rotor speed. A separate PNLTM versus ad-
vancing blade tip Mach number function 
must be derived for each of the three certifi-
cation microphone locations, 

i.e., centerline, 

sideline left, and sideline right. Sideline left 
and right are defined relative to the direc-
tion of flight for each run. PNLTM adjust-
ments are to be applied to each microphone 
datum using the appropriate PNLTM func-
tion. 

(f) 

PNLT corrections. If the measured ambi-

ent atmospheric conditions of temperature 
and relative humidity differ from those pre-
scribed as reference conditions under this ap-
pendix (77 degrees F and 70 percent, respec-
tively), corrections to the EPNL values must 
be calculated from the measured data under 
paragraph (a) of this section as follows: 

(1) 

Takeoff flight path. For the takeoff 

flight path shown in Figure H1, the spectrum 
of PNLTM observed at station A for the air-
craft at position L is decomposed into its in-
dividual SPL(

i) values. 

(i) Step 1. A set of corrected values are 

then computed as follows: 

SPL(

i)

r

= SPL(

i) + C[

a(i)  ¥  a(i)

o

]AL + 

C

a(i)

o

 

(AL ¥ AL

r

) + 20 log (AL/AL

r

where SPL(

i) and SPL(i)

r

are the measured 

and corrected sound pressure levels, respec-
tively, in the 

i-th one-third octave band. The 

first correction term adjusts for the effect of 
change in atmospheric sound absorption 
where 

a(i) and a(i)

o

are the sound attenuation 

coefficients for the test and reference atmos-
pheric conditions, respectively, for the 

i-th 

one-third octave band, and AL is the meas-
ured takeoff sound propagation path. The 
conversion factor constant, 

C, is 0.001 for 

English System of Units and is 0.01 for Inter-
national System of Units. The second correc-
tion term adjusts for the effects of atmos-
pheric attenuation due to the difference in 
the sound propagation path length where AL

r

 

is the Reference takeoff sound propagation 
path. The third correction term, known as 
the ‘‘inverse square’’ law, adjusts for the ef-
fect of the difference in the sound propaga-
tion path lengths. 

(ii) Step 2. The corrected values of the 

SPL(

i)

r

are then converted to reference con-

dition PNLT and a correction term cal-
culated as follows: 

D

1

= PNLT ¥ PNLTM 

which represents the correction to be added 
algebraically to the EPNL calculated from 
the measured data. 

(2) 

Level flyover flight path. (i) The proce-

dure described in paragraph (f)(1) of this sec-
tion for takeoff paths is also used for the 
level flyover paths, with the values of SPL(

i)

r

 

relating to the flyover sound propagation 
paths shown in Figure H2 as follows: 

SPL(

i)

r

= SPL(

i) + C[

a(i)  ¥  a(i)

o

]AM + 

C

a(i)

o

 

(AM ¥ AM

r

) + 20 log (AM/AM

r

where the lines AM and AM

r

are the meas-

ured and reference level flyover sound propa-
gation paths, respectively. 

(ii) The remainder of the procedure is the 

same for the flyover condition as that pre-
scribed in the paragraph (f)(1)(ii) of this sec-
tion regarding takeoff flight path. 

(3) 

Approach flight path. (i) The procedure 

described in paragraph (f)(1) of this section 
for takeoff paths is also used for the ap-
proach paths, with the values of SPL(

i)

r

re-

lating to the approach sound propagation 
paths shown in Figure H3 as follows: 

SPL(

i)

r

= SPL(

i) + C[

a(i)  ¥  a(i)

o

]AN + 

C

a(i)

o

 

(AN ¥ AN

r

) + 20 log (AN/AN

r

where the lines AN and AN

r

are the measured 

and reference approach sound propagation 
paths, respectively. 

(ii) The remainder of the procedure is the 

same for the approach condition as that pre-
scribed in the paragraph (f)(1)(ii) of this sec-
tion regarding takeoff flight path. 

(4) 

Sideline microphones. (i) The procedure 

prescribed in paragraph (f)(1) of this section 
for takeoff paths is also used for the propa-
gation to the sideline locations, with the val-
ues of SPL(

i)

r

relating as follows to the 

measured sideline sound propagation path 
shown in Figure H3 as follows: 

SPL(

i)

r

= SPL(

i) + C[

a(i)  ¥  a(i)

o

]SX + 

C

a(i)

o

 

(SX ¥ SX

r

) + 20 log (SX/SX

r

where S is the sideline measuring station 
and, based upon the flight condition, the hel-
icopter positions, X and X

r

, correspond to: 

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