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Dev Abhishikth Bandi
246403
INSTRUCTOR
Matthew West
ME 540
Noise Cancellation in Cars
Introduction
The noise and vibration of cars have become
increasingly important. The predominant sources of
interior noise in cars are engine and wheel vibrations,
which propagate as structure-borne sound through the
car body and finally radiate as airborne sound into the
cabin. In order to reduce the noise and make it tolerable
and negligible we use noise cancellation techniques
1.Vibration Control
 Passive Vibration Control
 Active Vibration Control
2. Noise Control
 Passive Noise Control or Active Noise Reduction
 Active Noise Control
Active vibration control
The sensor is a
piezoelectric
accelerometer that
senses the
excitation of the
passive engine
mount.
The controller
generates a
canceling signal
that is fed to a
power amplifier.
The amplifier
converts the
controller's low-
voltage signal to an
actuator current.
The force generated
by the actuator
cancels the primary
disturbance signal
resulting in near
zero chassis
vibration.
Cancellation of Waves
Active Noise Cancellation
Active Noise Cancellation
 Most road noise comes from the sound of tires
contacting the road, but the vehicles' engines also
play a significant role
 The frequency of road noise is around 1,000 Hz.
Researchers have documented road noise as low
as 700 Hz and as high as 1,300 Hz.
Sound Wave
Y(t) = A*Sin(2π*f*t+ϕ) (sine wave form)
 A - Amplitude or Magnitude(decibels)
 f – Natural Frequency
 t – Time
 φ – Phase angle
We consider 40db for all the sound waves for
easier assumption.
Road Noise at a average Frequency of 1000Hz
t=(0:0.00001:0.003);
y1=40*sin(2000*pi*t);
plot(t,y1);
0 0.5 1 1.5 2 2.5 3
x 10
-3
-50
-40
-30
-20
-10
0
10
20
30
40
50
Time(t)
dba
Cancellation Input at 1000Hz frequency
t=(0:0.00001:0.003);
y2=-40*sin(2000*pi*t);
plot(t,y2);
0 0.5 1 1.5 2 2.5 3
x 10
-3
-40
-30
-20
-10
0
10
20
30
40
Time(t)
dba
Resultant Output wave
y=(y1+y2);
plot(t,y);
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
Time(t)
dba
Active Noise Cancellation
 Most road noise comes from the sound of tires
contacting the road, but the vehicles' engines also
play a significant role
 The frequency of road noise is around 1,000 Hz.
Researchers have documented road noise as low
as 700 Hz and as high as 1,300 Hz.
 The voiced speech of a typical adult male will
have a fundamental frequency from 85 to 180 Hz,
and that of a typical adult female from 165 to 255
Hz.
Female voice at a average of 200Hz frequency
t=(0:0.00001:0.01);
y3=40*sin(400*pi*t);
plot(t,y3);
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
-50
-40
-30
-20
-10
0
10
20
30
40
50
Time(t)
dba
Resultant Output with cancellation wave
y=(y2+y3);
plot(t,y);
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
-80
-60
-40
-20
0
20
40
60
80
Time(t)
dba
Male voice at an average of 130Hz Frequency
t=(0:0.00001:0.01);
y3=40*sin(400*pi*t);
plot(t,y3);
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016 0.018 0.02
-50
-40
-30
-20
-10
0
10
20
30
40
50
Time(t)
dba
Resultant output with cancellation wave
y=(y2+y4);
plot(t,y);
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016 0.018 0.02
-80
-60
-40
-20
0
20
40
60
80
Time(t)
dba
Resultant Output with both voices
t=(0:0.00001:0.02);
y=(y2+y3+y4);
plot(t,y);
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016 0.018 0.02
-150
-100
-50
0
50
100
150
Conclusion
 Although describing the system like that is
relatively simple, the acoustics inside a car made
getting it right a challenge.
 Unlike headphones, the in-car system has to deal
with both direct noise and its echo when it
bounces off interior walls.
 The technology required for clear identification of
the appropriate sound waves with certain
frequencies requires a lot of skill and money.
References
 http://www.cvel.clemson.edu/auto/systems/active
_cabin_noise_suppression.html
 http://www.autonews.com/article/20131118/OEM0
6/311189964/suppliers-improvements-to-noise-
cancellation-may-help-voice
 https://en.wikipedia.org/wiki/Active_vibration_cont
rol
Questions?

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ME 540 project (1)

  • 1. Dev Abhishikth Bandi 246403 INSTRUCTOR Matthew West ME 540 Noise Cancellation in Cars
  • 2. Introduction The noise and vibration of cars have become increasingly important. The predominant sources of interior noise in cars are engine and wheel vibrations, which propagate as structure-borne sound through the car body and finally radiate as airborne sound into the cabin. In order to reduce the noise and make it tolerable and negligible we use noise cancellation techniques 1.Vibration Control  Passive Vibration Control  Active Vibration Control 2. Noise Control  Passive Noise Control or Active Noise Reduction  Active Noise Control
  • 3. Active vibration control The sensor is a piezoelectric accelerometer that senses the excitation of the passive engine mount. The controller generates a canceling signal that is fed to a power amplifier. The amplifier converts the controller's low- voltage signal to an actuator current. The force generated by the actuator cancels the primary disturbance signal resulting in near zero chassis vibration.
  • 6. Active Noise Cancellation  Most road noise comes from the sound of tires contacting the road, but the vehicles' engines also play a significant role  The frequency of road noise is around 1,000 Hz. Researchers have documented road noise as low as 700 Hz and as high as 1,300 Hz.
  • 7. Sound Wave Y(t) = A*Sin(2π*f*t+ϕ) (sine wave form)  A - Amplitude or Magnitude(decibels)  f – Natural Frequency  t – Time  φ – Phase angle We consider 40db for all the sound waves for easier assumption.
  • 8. Road Noise at a average Frequency of 1000Hz t=(0:0.00001:0.003); y1=40*sin(2000*pi*t); plot(t,y1); 0 0.5 1 1.5 2 2.5 3 x 10 -3 -50 -40 -30 -20 -10 0 10 20 30 40 50 Time(t) dba
  • 9. Cancellation Input at 1000Hz frequency t=(0:0.00001:0.003); y2=-40*sin(2000*pi*t); plot(t,y2); 0 0.5 1 1.5 2 2.5 3 x 10 -3 -40 -30 -20 -10 0 10 20 30 40 Time(t) dba
  • 10. Resultant Output wave y=(y1+y2); plot(t,y); 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 Time(t) dba
  • 11. Active Noise Cancellation  Most road noise comes from the sound of tires contacting the road, but the vehicles' engines also play a significant role  The frequency of road noise is around 1,000 Hz. Researchers have documented road noise as low as 700 Hz and as high as 1,300 Hz.  The voiced speech of a typical adult male will have a fundamental frequency from 85 to 180 Hz, and that of a typical adult female from 165 to 255 Hz.
  • 12. Female voice at a average of 200Hz frequency t=(0:0.00001:0.01); y3=40*sin(400*pi*t); plot(t,y3); 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 -50 -40 -30 -20 -10 0 10 20 30 40 50 Time(t) dba
  • 13. Resultant Output with cancellation wave y=(y2+y3); plot(t,y); 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 -80 -60 -40 -20 0 20 40 60 80 Time(t) dba
  • 14. Male voice at an average of 130Hz Frequency t=(0:0.00001:0.01); y3=40*sin(400*pi*t); plot(t,y3); 0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016 0.018 0.02 -50 -40 -30 -20 -10 0 10 20 30 40 50 Time(t) dba
  • 15. Resultant output with cancellation wave y=(y2+y4); plot(t,y); 0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016 0.018 0.02 -80 -60 -40 -20 0 20 40 60 80 Time(t) dba
  • 16. Resultant Output with both voices t=(0:0.00001:0.02); y=(y2+y3+y4); plot(t,y); 0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016 0.018 0.02 -150 -100 -50 0 50 100 150
  • 17. Conclusion  Although describing the system like that is relatively simple, the acoustics inside a car made getting it right a challenge.  Unlike headphones, the in-car system has to deal with both direct noise and its echo when it bounces off interior walls.  The technology required for clear identification of the appropriate sound waves with certain frequencies requires a lot of skill and money.