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THE EFFECT OF SOUND ON
THE GROWTH OF PLANTS
By- Taufiq Ahamed
INTRODUCTION
• Very little research has been conducted on the specific effect of the growth of
plants subjected to sounds of varying inten sity and frequency. Any environmental
factor that places a biological system under stress can affect its performance
and/or behaviour. The effect of sound on physiology and behaviour of animals and
man has been studied by various researchers . However, only a limited amount of
detailed information is available on the effect of sound on plant systems.
• An article entitled “The Effect of Noise on Plant Growth” , stimulated an interest in
further research in this field. The author, A.E. Lord, performed random noise
experiments
• on coleus plants in which one group was subjected to random noise and a second
group was used as a control. Lord came to the conclusion that botanists had not
carried out sufficient experiments to show causes behind the effects that he
observed, and he put forward the idea that the rate of water transpired out of the
leaves is affected by the sound. Transpiration, in turn, affects growth. Typical leaf
structures and the topic of transpiration can be found in textbooks on botany.
APPARATUS AND PROCEDURE
• The plants were housed in environmental chambers,
162 cm high, 153 cm wide, 84 cm deep with 2 cm
thick walls [Figure 1]. The environmental chambers
were made by Percival Co. of Boone, Iowa, U.S.A.
They controlled the temperature and lightning, and
provided a constant flow of air by means of in built
fans and vents. The operating specifications of the
chambers were: Photoperiod: DA Y/NIGHT;
Thermoperiod: 0 to 150 degrees F / 15 to 65
degrees C; and Fluorescent lighting: 6 tubes, cool
white, 40 W
DISCUSSION AND OBSERVATIONS
• At the outset of these experiments, it was reasoned that there might be a
relationship between the wavelength of the sound generated and a
characteristic dimension of the leaf.
• Figure represents the outline of a bean leaf, and there is a small particle
of air moving back and forth on the surface of the leaf with velocities of
positive and negative “u”. This wave movement occurs as a result of the
diaphragm of the speaker moving back and forth, setting up a travelling
compression and rarefaction wave. The compression results in a positive
pressure [above atmospheric] and the rarefac tion in a negative pressure
[below atmospheric]. This is propagated across the surface of the leaf and
is commonly represented as a sinusoidal air pressure variation. The parti
cle velocity is proportional to the sound pressure [13], and a positive
pressure results in a positive particle velocity, the magnitude of the
velocity being proportional to the pressure at any point as it moves across
the leaf. The same process results from a negative pressure, only with the
particle veloc ity in the opposite direction. This creates a scrubbing or
brushing action on the surface of the leaf, which wipes away any stagnant
film of moisture and allows the plant to breathe [transpire] more freely.
CONCLUSIONS AND
RECOMMENDATIONS
• From the results of the experiments as shown in Figures 3 and 4, it is
clear that, in time, i.e. after 28 days of testing, the optimum growth of
both the beans and the impatiens plants occurred when the wavelength
of the sound coincided with the plant leaf dimension. This conclusion
cannot be drawn for the growth periods of up to about 16 days. Below
this the results are mixed and inconclusive. It should be noted that, for
the beans, the growth with the random noise was less than the growth
with any of the pure tones. There was not this marked difference
between the growth in the impatiens plants when subjected to random
and pure tones
• In the latter days of the testing, growth with the random noise was less
with the bean plants [Figure 3] than with the impatiens plants , This is
something that warrants further testing, especially with a larger number
of plants, perhaps a larger species variety, and a longer testing period.
ACKNOWLEDGEMENTS & EPILOGUE
• The author would like to express his appreciation to Professors D. Fahselt
and A. Maun of the Department of Plant Sciences and the Sound and
Vibration Laboratory of The University of Western Ontario for the use of
equipment in this experiment. He is also grateful to Wai Keung Li of the
Faculty of Social Sciences for his careful statistical analysis of data. Further,
the author acknowledges the capa ble assistance of Mary Daniel in the
preparation and typing of this manuscript.
• This work was conducted in 1979 by Margaret E. Collins while she was a
student in Mechanical Engineering at the Faculty of Engineering Science of
The University of Western Ontario. I was her supervisor and we were assisted
by the Department of Plant Sciences at the University [see
Acknowledgements], The work was recorded in her thesis as part
requirement for ES 400 - Project, Thesis and Seminar. Ms. Collins is now
deceased and this paper is written to her memory. John E.K. Foreman,
Professor Emeritus, May, 2001
The Effect of Sound on Plant Growth

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The Effect of Sound on Plant Growth

  • 1. THE EFFECT OF SOUND ON THE GROWTH OF PLANTS By- Taufiq Ahamed
  • 2. INTRODUCTION • Very little research has been conducted on the specific effect of the growth of plants subjected to sounds of varying inten sity and frequency. Any environmental factor that places a biological system under stress can affect its performance and/or behaviour. The effect of sound on physiology and behaviour of animals and man has been studied by various researchers . However, only a limited amount of detailed information is available on the effect of sound on plant systems. • An article entitled “The Effect of Noise on Plant Growth” , stimulated an interest in further research in this field. The author, A.E. Lord, performed random noise experiments • on coleus plants in which one group was subjected to random noise and a second group was used as a control. Lord came to the conclusion that botanists had not carried out sufficient experiments to show causes behind the effects that he observed, and he put forward the idea that the rate of water transpired out of the leaves is affected by the sound. Transpiration, in turn, affects growth. Typical leaf structures and the topic of transpiration can be found in textbooks on botany.
  • 3. APPARATUS AND PROCEDURE • The plants were housed in environmental chambers, 162 cm high, 153 cm wide, 84 cm deep with 2 cm thick walls [Figure 1]. The environmental chambers were made by Percival Co. of Boone, Iowa, U.S.A. They controlled the temperature and lightning, and provided a constant flow of air by means of in built fans and vents. The operating specifications of the chambers were: Photoperiod: DA Y/NIGHT; Thermoperiod: 0 to 150 degrees F / 15 to 65 degrees C; and Fluorescent lighting: 6 tubes, cool white, 40 W
  • 4. DISCUSSION AND OBSERVATIONS • At the outset of these experiments, it was reasoned that there might be a relationship between the wavelength of the sound generated and a characteristic dimension of the leaf. • Figure represents the outline of a bean leaf, and there is a small particle of air moving back and forth on the surface of the leaf with velocities of positive and negative “u”. This wave movement occurs as a result of the diaphragm of the speaker moving back and forth, setting up a travelling compression and rarefaction wave. The compression results in a positive pressure [above atmospheric] and the rarefac tion in a negative pressure [below atmospheric]. This is propagated across the surface of the leaf and is commonly represented as a sinusoidal air pressure variation. The parti cle velocity is proportional to the sound pressure [13], and a positive pressure results in a positive particle velocity, the magnitude of the velocity being proportional to the pressure at any point as it moves across the leaf. The same process results from a negative pressure, only with the particle veloc ity in the opposite direction. This creates a scrubbing or brushing action on the surface of the leaf, which wipes away any stagnant film of moisture and allows the plant to breathe [transpire] more freely.
  • 5. CONCLUSIONS AND RECOMMENDATIONS • From the results of the experiments as shown in Figures 3 and 4, it is clear that, in time, i.e. after 28 days of testing, the optimum growth of both the beans and the impatiens plants occurred when the wavelength of the sound coincided with the plant leaf dimension. This conclusion cannot be drawn for the growth periods of up to about 16 days. Below this the results are mixed and inconclusive. It should be noted that, for the beans, the growth with the random noise was less than the growth with any of the pure tones. There was not this marked difference between the growth in the impatiens plants when subjected to random and pure tones • In the latter days of the testing, growth with the random noise was less with the bean plants [Figure 3] than with the impatiens plants , This is something that warrants further testing, especially with a larger number of plants, perhaps a larger species variety, and a longer testing period.
  • 6. ACKNOWLEDGEMENTS & EPILOGUE • The author would like to express his appreciation to Professors D. Fahselt and A. Maun of the Department of Plant Sciences and the Sound and Vibration Laboratory of The University of Western Ontario for the use of equipment in this experiment. He is also grateful to Wai Keung Li of the Faculty of Social Sciences for his careful statistical analysis of data. Further, the author acknowledges the capa ble assistance of Mary Daniel in the preparation and typing of this manuscript. • This work was conducted in 1979 by Margaret E. Collins while she was a student in Mechanical Engineering at the Faculty of Engineering Science of The University of Western Ontario. I was her supervisor and we were assisted by the Department of Plant Sciences at the University [see Acknowledgements], The work was recorded in her thesis as part requirement for ES 400 - Project, Thesis and Seminar. Ms. Collins is now deceased and this paper is written to her memory. John E.K. Foreman, Professor Emeritus, May, 2001