SlideShare a Scribd company logo
1 of 1
Physics example
A speleologist lets fall a stone into a hole and at the beginning it was firm. The sound speed in the
air is 343m/s and the speleologist hears the sound of the stone when it touches the hole's bottom
1,5s after he lets it fall.
How deep is the hole?

Known data:

Sound speed: vs=343m/s
Total time: t=1.5s                                                                                      ?
Speed at the beginning: v0=0m/s

Solution:
t=t1+t2 where t1=time the stone needs to reach the ground
t2=time the sound needs to go back to the speleologist  t2=1.5 s – t1.
The stone moves with uniformly accelerated rectilinear motion, following the law:
    1 2
s=    gt + v 0 t + s 0 where s0=0m, v0=0m/s and g=9,8m/s2  s = 4.9m / s 2 t12
    2
Sound propagates with uniform rectilinear motion following the law: s = v s t + s 0 where s0=0m,
vs=343m/s  s = 343m / st 2.
The distance covered by the sound and the stone are exactly the same, so 4.9m / s 2 t12 = 343m / st 2
 4.9m / s t1 − 343m / st 2 = 0 , but t2=1.5s – t1  4.9m/s2 (t1)2 – 343m/s (1.5s – t1)=0 
            2 2


4.9m/s2 (t1)2 + 343m/s t1–514.5m=0  Solving the second degree equation, we obtain two solutions,
one is <0 and it is not acceptable (we can’t go back on the time line!), the other one is t1=1.47s 
t2=1.5 s – 1.47s=0.03s (time needed to the sound to go from the bottom of the hole to the ear of the
speleologist) substituting this value into the sound propagation law, we obtain: s=343m/s ∙
0.03s=10.58m that is the deep of the hole.

More Related Content

Similar to Speleologist

Similar to Speleologist (20)

Reflection of Sound Part 1
Reflection of Sound Part 1Reflection of Sound Part 1
Reflection of Sound Part 1
 
Interference and Beats
Interference and BeatsInterference and Beats
Interference and Beats
 
SOUND WAVES.pdf
SOUND WAVES.pdfSOUND WAVES.pdf
SOUND WAVES.pdf
 
Anschp22
Anschp22Anschp22
Anschp22
 
Lo 7(2)
Lo 7(2)Lo 7(2)
Lo 7(2)
 
sound.pptx
sound.pptxsound.pptx
sound.pptx
 
What is-a-sound-wave
What is-a-sound-waveWhat is-a-sound-wave
What is-a-sound-wave
 
Learning object: wave speed relationships
Learning object: wave speed relationshipsLearning object: wave speed relationships
Learning object: wave speed relationships
 
Physics 101 Learning Object 2
Physics 101 Learning Object 2Physics 101 Learning Object 2
Physics 101 Learning Object 2
 
Sound solving
Sound solvingSound solving
Sound solving
 
Physics chapter 7
Physics chapter 7Physics chapter 7
Physics chapter 7
 
3.5 form 4 sound
3.5 form 4 sound3.5 form 4 sound
3.5 form 4 sound
 
Sound lecture part 1
Sound lecture part 1Sound lecture part 1
Sound lecture part 1
 
pardhu.docx
pardhu.docxpardhu.docx
pardhu.docx
 
Physics by Younes Sina
Physics by Younes SinaPhysics by Younes Sina
Physics by Younes Sina
 
Learning object 4 sound waves
Learning object 4 sound wavesLearning object 4 sound waves
Learning object 4 sound waves
 
Sound Energy
Sound EnergySound Energy
Sound Energy
 
Lecture22
Lecture22Lecture22
Lecture22
 
Lecture22
Lecture22Lecture22
Lecture22
 
Phys12
Phys12Phys12
Phys12
 

More from Enrica Maragliano

La gestione della classe nella scuola secondaria
La gestione della classe nella scuola secondariaLa gestione della classe nella scuola secondaria
La gestione della classe nella scuola secondariaEnrica Maragliano
 
Observation and feedback impact model by Rachel Lofthouse
Observation and feedback impact model by Rachel Lofthouse Observation and feedback impact model by Rachel Lofthouse
Observation and feedback impact model by Rachel Lofthouse Enrica Maragliano
 
Physical awareness presentation
Physical awareness presentationPhysical awareness presentation
Physical awareness presentationEnrica Maragliano
 
The Age Of Newton In History, Science
The  Age Of  Newton In  History,  ScienceThe  Age Of  Newton In  History,  Science
The Age Of Newton In History, ScienceEnrica Maragliano
 

More from Enrica Maragliano (7)

Presentazione Inducas 2017
Presentazione Inducas 2017Presentazione Inducas 2017
Presentazione Inducas 2017
 
La gestione della classe nella scuola secondaria
La gestione della classe nella scuola secondariaLa gestione della classe nella scuola secondaria
La gestione della classe nella scuola secondaria
 
Observation and feedback impact model by Rachel Lofthouse
Observation and feedback impact model by Rachel Lofthouse Observation and feedback impact model by Rachel Lofthouse
Observation and feedback impact model by Rachel Lofthouse
 
Presentazione 20 aprile
Presentazione 20 aprilePresentazione 20 aprile
Presentazione 20 aprile
 
Presentazione pnsd
Presentazione pnsdPresentazione pnsd
Presentazione pnsd
 
Physical awareness presentation
Physical awareness presentationPhysical awareness presentation
Physical awareness presentation
 
The Age Of Newton In History, Science
The  Age Of  Newton In  History,  ScienceThe  Age Of  Newton In  History,  Science
The Age Of Newton In History, Science
 

Speleologist

  • 1. Physics example A speleologist lets fall a stone into a hole and at the beginning it was firm. The sound speed in the air is 343m/s and the speleologist hears the sound of the stone when it touches the hole's bottom 1,5s after he lets it fall. How deep is the hole? Known data: Sound speed: vs=343m/s Total time: t=1.5s ? Speed at the beginning: v0=0m/s Solution: t=t1+t2 where t1=time the stone needs to reach the ground t2=time the sound needs to go back to the speleologist  t2=1.5 s – t1. The stone moves with uniformly accelerated rectilinear motion, following the law: 1 2 s= gt + v 0 t + s 0 where s0=0m, v0=0m/s and g=9,8m/s2  s = 4.9m / s 2 t12 2 Sound propagates with uniform rectilinear motion following the law: s = v s t + s 0 where s0=0m, vs=343m/s  s = 343m / st 2. The distance covered by the sound and the stone are exactly the same, so 4.9m / s 2 t12 = 343m / st 2  4.9m / s t1 − 343m / st 2 = 0 , but t2=1.5s – t1  4.9m/s2 (t1)2 – 343m/s (1.5s – t1)=0  2 2 4.9m/s2 (t1)2 + 343m/s t1–514.5m=0  Solving the second degree equation, we obtain two solutions, one is <0 and it is not acceptable (we can’t go back on the time line!), the other one is t1=1.47s  t2=1.5 s – 1.47s=0.03s (time needed to the sound to go from the bottom of the hole to the ear of the speleologist) substituting this value into the sound propagation law, we obtain: s=343m/s ∙ 0.03s=10.58m that is the deep of the hole.