String waves on a cable car and free falling.

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SUMMARY

The discussion centers on the physics of string waves in a cable car during an earthquake, specifically how the amplitude of the wave must meet a certain condition for the cable car to experience free fall. The derived formula for the amplitude Y is Y ≥ (gλ²u)/(4π²T), where g is the acceleration due to gravity, λ is the wavelength, u is the linear mass density, and T is the tension in the cable. Participants explored the relationship between wave acceleration and gravitational acceleration, utilizing equations for wave speed and angular frequency.

PREREQUISITES
  • Understanding of wave mechanics, specifically transverse waves
  • Familiarity with the concepts of tension and linear mass density in strings
  • Knowledge of basic calculus, particularly partial derivatives
  • Ability to manipulate trigonometric functions and their maximum values
NEXT STEPS
  • Study the derivation of wave speed in strings, focusing on Tension and Linear Mass Density
  • Learn about the implications of wave amplitude in oscillatory motion
  • Explore the relationship between angular frequency and wave properties
  • Investigate the effects of gravitational forces on oscillating systems
USEFUL FOR

Students and educators in physics, particularly those studying wave mechanics and dynamics, as well as engineers working with cable systems and oscillatory motion.

Gravitino22
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Homework Statement



You're riding a cable car from Bogota up to Monser-
rate. During your ride there is a small earthquake that
sends vertical, transverse waves propagating along the
cable. The cable's tension is T, its linear mass den-
sity is u, and the wavelength of the wave is \lambda. If the
amplitude of the wave is large enough, the motion of
the cable car will momentarily leave you in free fall.
Show that in order for this to happen the amplitude
must be given by

Y => \frac{g\lambda^{2}u}{4\pi^{2}T}

Homework Equations


position along a wave: y=Ysin(kx-wt)

string waves speed: v = \sqrt{\frac{T}{u}}



The Attempt at a Solution



My train of thought is that for free fall to happen the acceleration of the wave must be greater than the acceleration of gravity.

I tried taking the second partial derivate with respect to time of the waves position equation to obtain its acceleration which gave me:

a_{y}=-w^{2}Ysin(kx-wt) that should be => then g

but i don't know where the tension would or the linear mass density would come in.


Any help pointing me in the right direction would be appriciated! thanks :)
 
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Gravitino22 said:
a_{y}=-w^{2}Ysin(kx-wt) that should be => then g

but i don't know where the tension would or the linear mass density would come in.

try to compute k and w.
 
w = 2\pif where f is the angular frequency and k =\frac{2\pi}{\lambda}

that would give you sin(2\pi(\frac{x}{\lambda} - ft)) by factoring a 2pii inside... still not seeing how the sine term is somehow related to the tension and linear mass density =/
 
the frequency depends on the wave speed and the wavelength
 
ok i made the following substitutions:

f=\frac{v}{\lambda} and made v=\frac{x}{t} (iam unsure about this one)


so far i have this

g<=-\frac{4\pi^{2}x^{2}Y}{\lambda^{2}t^{2}}sin(2\pi) the sin term is 1.
 
wait wait! i have it just substitute back for v^{2} and which equals T/u and viola!


tho there's a small problem...the negative sign...


Thanks a lot tho man!
 
nm! i don't have it now...iam stupid sine of 2pii is not 1 lol that sine term still bothering me...somehow i know i have to make the stuff inside the sine equal to pii/2.
 
Gravitino22 said:
nm! i don't have it now...iam stupid sine of 2pii is not 1 lol that sine term still bothering me...somehow i know i have to make the stuff inside the sine equal to pii/2.

you already gave an equation for v.

For the amplitude you can just take the maximum value of sin() which is 1
 
hmm yea that's what i was thinking...Thanks a lot :)
 

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