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Computer	
  experiment	
  of	
  
Science	
  and	
  Engineering
High-­‐pass	
  filter	
  and	
  Low-­‐pass	
  filter	
  
University	
  of	
  Aizu	
  
s1210199	
  Masanori	
  Seino
What	
  is	
  a	
  High-­‐pass	
  filter?
A	
  high-­‐pass	
  filter	
  (HPF)	
  is	
  an	
  electronic	
  
filter	
  that	
  passes	
  high-­‐frequency	
  
signals	
  but	
  attenuates	
  (reduces	
  the	
  
amplitude	
  of)	
  signals	
  with	
  frequencies	
  
lower	
  than	
  the	
  cutoff	
  frequency.
 
	
  
The	
  product	
  of	
  the	
  resistance	
  and	
  
capacitance	
  (R×C)	
  is	
  the	
  time	
  constant	
  
(τ);	
  it	
  is	
  incersely	
  proportional	
  to	
  the	
  
cutoff	
  frequency	
  fc,	
  that	
  is,	
  
	
  
Fc	
  =	
  1	
  /	
  2πτ	
  =	
  1	
  /	
  2πRC
The	
  simple	
  first-­‐order	
  electronic	
  high-­‐
pass	
  filter	
  show	
  below	
  figure.
What	
  is	
  a	
  Low-­‐pass	
  filter?
A	
  low-­‐pass	
  filter	
  is	
  a	
  filter	
  that	
  passes	
  
low-­‐frequency	
  signals	
  and	
  attenuates	
  
(reduces	
  the	
  amplitude	
  of)	
  signals	
  with	
  
frequencies	
  higher	
  that	
  the	
  cutoff	
  
frequency.
The	
  break	
  frequency,	
  also	
  called	
  the	
  
turnover	
  frequency	
  or	
  cutoff	
  frequency	
  
(in	
  hertz),	
  is	
  determined	
  by	
  the	
  time	
  
constant:	
  
fc	
  =	
  1	
  /	
  2πτ	
  =	
  1	
  /	
  2πRC	
  
	
  
	
  
One	
  simple	
  low-­‐pass	
  filter	
  circuit	
  consists	
  of	
  
a	
  resistor	
  in	
  series	
  with	
  a	
  load,	
  and	
  a	
  
capacitor	
  in	
  parallel	
  with	
  the	
  load.
Experiment
1.  I	
  ask	
  the	
  f0	
  of	
  the	
  combination	
  of	
  CR	
  
that	
  has	
  been	
  selected.	
  
2.  I	
  measure	
  the	
  transfer	
  characteristic.	
  
3.  To	
  draw	
  a	
  graph	
  to	
  compare	
  the	
  two.	
  
My	
  data	
  (High-­‐pass)
f V1	
  p-­‐p V2	
  p-­‐p db Out	
  of	
  
phase
0.71k 5.16 0.52 -­‐19.9 87°
3.58k 5.16 2.36 -­‐6.79 63°
7.16k 5.12 3.6 -­‐3.05 45°	
  
14.4k 5.12 4.52 -­‐1.08 25.4°
71.6k 5.16 5.08 -­‐0.13 5.63°
716k 5.16 5.12 -­‐0.06 1.24°
My	
  data	
  (Low-­‐pass)
f V1	
  p-­‐p V2	
  p-­‐p dB Out	
  of	
  
phase
0.71k 4.64 4.56 -­‐0.15 -­‐18°
3.58k 5.28 4.64 -­‐1.12 -­‐25.9°
7.16k 5.28 3.68 -­‐3.13 -­‐45°
14.4k 5.28 2.40 -­‐6.84 -­‐58.3°
71.6k 5.28 0.72 -­‐0.17 -­‐60°
716k 5.28 0.32 -­‐0.24 88°
Graph	
  (High-­‐pass	
  filter)
Graph	
  (Low-­‐pass	
  filter)
Result	
  of	
  experiments
When	
  I	
  wrote	
  a	
  graph	
  based	
  on	
  
the	
  my	
  experimental	
  data,	
  
graph,	
  as	
  defined	
  could	
  be.	
  
Conclusion
High-­‐pass	
  filter	
  
•High	
  Frequency	
  
No	
  attenuation,	
  asymptotic	
  to	
  the	
  phase	
  
difference	
  without	
  
•Low	
  Frequency	
  
Phase	
  difference	
  is	
  asymptotic	
  to	
  +90°	
  
Low-­‐pass	
  filter	
  
•High	
  Frequency	
  
No	
  attenuation,	
  asymptotic	
  to	
  the	
  
phase	
  difference	
  without.	
  
•Low	
  Frequency	
  
Phase	
  difference	
  is	
  asymptotic	
  to	
  -­‐90°	
  
	
  

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Assignment

  • 1. Computer  experiment  of   Science  and  Engineering High-­‐pass  filter  and  Low-­‐pass  filter   University  of  Aizu   s1210199  Masanori  Seino
  • 2. What  is  a  High-­‐pass  filter? A  high-­‐pass  filter  (HPF)  is  an  electronic   filter  that  passes  high-­‐frequency   signals  but  attenuates  (reduces  the   amplitude  of)  signals  with  frequencies   lower  than  the  cutoff  frequency.
  • 3.     The  product  of  the  resistance  and   capacitance  (R×C)  is  the  time  constant   (τ);  it  is  incersely  proportional  to  the   cutoff  frequency  fc,  that  is,     Fc  =  1  /  2πτ  =  1  /  2πRC
  • 4. The  simple  first-­‐order  electronic  high-­‐ pass  filter  show  below  figure.
  • 5. What  is  a  Low-­‐pass  filter? A  low-­‐pass  filter  is  a  filter  that  passes   low-­‐frequency  signals  and  attenuates   (reduces  the  amplitude  of)  signals  with   frequencies  higher  that  the  cutoff   frequency.
  • 6. The  break  frequency,  also  called  the   turnover  frequency  or  cutoff  frequency   (in  hertz),  is  determined  by  the  time   constant:   fc  =  1  /  2πτ  =  1  /  2πRC      
  • 7. One  simple  low-­‐pass  filter  circuit  consists  of   a  resistor  in  series  with  a  load,  and  a   capacitor  in  parallel  with  the  load.
  • 8. Experiment 1.  I  ask  the  f0  of  the  combination  of  CR   that  has  been  selected.   2.  I  measure  the  transfer  characteristic.   3.  To  draw  a  graph  to  compare  the  two.  
  • 9. My  data  (High-­‐pass) f V1  p-­‐p V2  p-­‐p db Out  of   phase 0.71k 5.16 0.52 -­‐19.9 87° 3.58k 5.16 2.36 -­‐6.79 63° 7.16k 5.12 3.6 -­‐3.05 45°   14.4k 5.12 4.52 -­‐1.08 25.4° 71.6k 5.16 5.08 -­‐0.13 5.63° 716k 5.16 5.12 -­‐0.06 1.24°
  • 10. My  data  (Low-­‐pass) f V1  p-­‐p V2  p-­‐p dB Out  of   phase 0.71k 4.64 4.56 -­‐0.15 -­‐18° 3.58k 5.28 4.64 -­‐1.12 -­‐25.9° 7.16k 5.28 3.68 -­‐3.13 -­‐45° 14.4k 5.28 2.40 -­‐6.84 -­‐58.3° 71.6k 5.28 0.72 -­‐0.17 -­‐60° 716k 5.28 0.32 -­‐0.24 88°
  • 13. Result  of  experiments When  I  wrote  a  graph  based  on   the  my  experimental  data,   graph,  as  defined  could  be.  
  • 14. Conclusion High-­‐pass  filter   •High  Frequency   No  attenuation,  asymptotic  to  the  phase   difference  without   •Low  Frequency   Phase  difference  is  asymptotic  to  +90°  
  • 15. Low-­‐pass  filter   •High  Frequency   No  attenuation,  asymptotic  to  the   phase  difference  without.   •Low  Frequency   Phase  difference  is  asymptotic  to  -­‐90°