Suppose I have an oscillating system, that oscillates under a standard restoring force given by :
F = − k x ,
where x is the displacement and k is the constant of proportionality with k > 0 .
Now suppose it is being damped by a viscous force given by the standard equation of
− b x ˙ = F d r a g .
Suppose that the particle under the forces have mass
m
, and at
t
=
0
we have
x
=
x
0
.
Then what is the
limiting
value of
b
for which the particle will not cross the origin even once?
Details and Assumptions
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Exactly , Because when b falls below 2, we get sinusoidal damped solutions (considering the real class of solutions) which necessarily cross the origin. It is interesting how it oscillates infinite times if b slightly less than 2 and just once when more or equal. Such a harsh discontinuity
Can you tell how you solved it I am stuck
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You don't solve . You guess the solution.If you cannot access the videos reply here.
https://www.youtube.com/watch?v=f8HJ6g1S6OA
https://www.youtube.com/watch?v=XCdPk1pIT1Y
https://www.youtube.com/watch?v=NU5nkbOa1zk
https://www.youtube.com/watch?v=17D4U_r6Gwk
https://www.youtube.com/watch?v=LmFGrx-MSzU
If you want to learn more about Waves and Optics enroll in PHYS201x on EdX.
what do you mean by ODE ? Does This equation has Many Other Solution also ? If So then what is Best Solution for This . ?
I just Use The Standard Solution of this Damping which is given in NCERT, x ( t ) = A 0 e m − b t sin ( ω d t + ϕ ) ω d = ( m k ) − ( 2 m b ) 2
Now For Never crossing X-axis It's Sinusoidal Time Phase Should be constant , Which is only Possible when It's damping frequency should be zero . (or Time period is Infinite) i.e ω d = 0 ⇒ b = 4 m k
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ODE is ordinary differential equation,
yes, inface ur eqn holds when b is less than 2, when equal, another equation holds whose graph i have plotted. when more than 2, still another set of equations hold,, all solutions are however expressible as
C1e^(tr1)+C2e^(tr2) ,
ur way holds when r1 and r2 are imaginary and C1 = C2 (the good form) , then use e^(ix)=cos(x)+isin(x),
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F = m x ′ ′ = − k x − b x ′
Solving this second order linear ODE, we get x ( t ) = c 1 e − 2 m t ( b 2 − 4 m k + b ) + c 2 e 2 m t ( b 2 − 4 m k − b )
For the limiting case of not crossing origin, b 2 − 4 m k = 0 or b = 2