text: Homework Help: Block hitting spring
  
  1. Jan 12, 2014
  
  Tanero
  
  1. The problem statement, all variables and given/known data
  
  A small block of mass m=1 kg and v0=6.32m/s hits a massless relaxed spring with spring constant k= 3 N/m, which starts to be compressed as the block continues to move horizontally. There is friction between the block and the horizontal surface, and it is not uniform. As a function of distance, the friction coefficient varies like μ(x)=αx, with α= 0.7 m^−1. For simplicity that static and dynamic friction coefficients are the same.
  
  What time t1 does it take for the block to travel between x=0 (relaxed spring) and x=x1 (block at first stop)? (in seconds)
  
  https://courses.edx.org/static/content-mit-801x~2013_SOND/html/final_p06.png [Broken]
  
  2. Relevant equations
  I chose x axis positive to the right. x0=0 at point of contact, x1=first momentarily stop
  Ffriction=-μmg=-αxmg
  Fspring=-kx
  
  Newton's Second Law
  ∑F=m*d2x/dt2
  
  3. The attempt at a solution
  
  -kx-αxmg=m*d2x/dt2
  -(k+αmg)x=m*d2x/dt2
  
  new konstant K=k+αmg
  -K/m=d2x/dt2
  
  This is SHO with general solution x(t)=Acos(ωt+θ)
  ω=√(K/m)=3.16
  
  To find A, and θ our initial conditions are:
  x0=x(t=0)=0
  v0=v(t=0)=6.32 m/s
  
  Thus, 0=x(t=0)=Acos(θ)
  This is true when θ=pi/2 or -3/2pi . Question: which angle should I use ???
  
  v0=v(t=0)=6.32/-ω=Asin(θ)
  
  A=√(x(t=o)^2+(v(t=0)/ω)^2)=√(0+(6.32/3.16)^2/)=2
  
  So, I know that my amplitude is 2, x1=2m.
  
  (Trying with 3/2pi. pi/2 can't feet because I am getting negative time.)
  
  2=x(t1)=2*cos(3.16t-3/2pi)
  
  1=cos(3.16t-3/2pi)
  This is true when (3.16t-3/2pi)=0
  t1=1.49 sec.
  
  Please, check my solution if it seemed to be right.
  And my t1 should be also half a period T=pi/ω=pi/3.16=0.99s. Isn't it? I am confused.
  
  Last edited by a moderator: May 6, 2017
  2. Jan 12, 2014
  
  voko
  
  This is not SHO because there is friction between the block and the surface.
  
  3. Jan 12, 2014
  
  Tanero
  
  So, what approach should I take instead?
  
  4. Jan 12, 2014
  
  voko
  
  Do you have any ideas?
  
  5. Jan 12, 2014
  
  Tanero
  
  I have found how far it travels using work - energy theorem. May be using equations of motion: x(t)=x0+v0t+1/2at^2, v(t)=v0+at. and for acceleration put acceleration from N2L -(k+αmg)/m*x=d2x/dt2. May be then I can find my t?
  
  6. Jan 12, 2014
  
  voko
  
  I have re-read the problem and your original solution, and I must say that I misunderstood what you were doing.
  
  While the system is not an SHO, it is not incorrect to treat it as an SHO until the block stops because the equation is the same.
  
  You have found the angular frequency $\omega$ of this system. How does that correspond to the period? What part of the period is spent by an SHO between max kinetic energy and max potential energy?
  
  7. Jan 12, 2014
  
  Tanero
  
  T=2pi/ω. Between those two conditions block on spring spends half period T/2=pi/ω ?
  
  8. Jan 12, 2014
  
  voko
  
  9. Jan 12, 2014
  
  Tanero
  
  T=pi/ω=pi/3.16=0.99 s.
  
  But I tried using equations of motion: v(t)=v0+at. for acceleration I put acceleration from N2L -(k+αmg)/m*x=d2x/dt2.
  
  0=v(t1)=vo-(k+αmg)/m*x*t
  x1=2
  t1=.316 s.
  
  Something wrong.
  
  10. Jan 12, 2014
  
  voko
  
  Your equation of motion is $$- {k + \alpha m g \over m} x = {d^2 x \over dt^2} .$$ This is a differential equation and its solution cannot be obtained by multiplying it by $t$. In fact, its solution is given by $x = A \cos (\omega t + \theta)$ as you wrote originally.
  
  11. Jan 12, 2014
  
  Tanero
  
  But this equation v(t)=v0+at is also differential v(t)=v0+d2x/dt2*t . I have acceleration in both equations. I substitute one into another. Wanna understand why this is not right thing to do?
  
  12. Jan 12, 2014
  
  voko
  
  $v(t) = v_0 + at$ is only correct when $a = \mathrm{const}$. Which is not the case here. In this case, we have $v(t) = -A \omega \sin (\omega t + \theta)$, and $a = -A \omega^2 \cos (\omega t + \theta) \ne \mathrm{const}$.
  
  13. Jan 12, 2014
  
  Tanero
  
  ahhh! sure, a is constant! that's why you can't. Thanks!
  
  14. Jan 12, 2014
  
  Geldof
  
  Could either of you please explain why half of the period should be used?
  
  15. Jan 12, 2014
  
  dummyano
  
  I found the max displacement for the mass via the energy work theorem, basically
  -> Potential Energy became Kinetic Energy at the end of the track
  -> in the collision no energy is lost as it is stated by the problem, so
  -> it is KE = Work F_spring + Work F_friction
  -> they both change with x so i took the integral from x0 to x1 for both the Work done
  that way I found max displacement.
  
  1) is that correct?
  2) is it possible to find the time without SHO equations?
  
  Last edited: Jan 12, 2014
  16. Jan 12, 2014
  
  Tanero
  
  @ dummyano
  1) Yes, the way you found x is correct.
  2) It seems you can't find t without SHO
  
  I am very much in doubt about finding t from T/2 . It doesn't agree with t found from solving SHO general solution equation. See above. I am stuck.
  
  17. Jan 12, 2014
  
  Tanero
  
  because it when object slides to the right it makes half a period.
  
  18. Jan 12, 2014
  
  Tanero
  
  I am very much in doubt about finding t from T/2 . It doesn't agree with t found from solving SHO general solution equation. See above.
  
  Can you please comment?
  
  19. Jan 12, 2014
  
  dummyano
  
  Thank you for answering.
  I will try SHO for t and post the result then
  
  20. Jan 12, 2014
  
  TSny
  
  What fraction of a period does it take for a mass in SHM to travel from the equilibrium position to the first time it comes to rest?
  
  Last edited: Jan 12, 2014
  21. Jan 12, 2014
  
  TSny
  
  pi/2 and -3pi/2 are effectively the same angle. (They differ by a full cycle.)
  
  Try to find another choice for θ.
  
  22. Jan 13, 2014
  
  voko
  
  Your doubts are right on. A simple harmonic oscillator goes like this:
  
  (0) max kinetic energy, velocity directed to the right;
  
  (1) max potential energy, no velocity;
  
  (2) max kinetic energy, velocity directed to the left;
  
  (3) max potential energy, no velocity;
  
  (4) max kinetic energy, velocity directed to the right; this completes the period.
  
  In this case, you are interested in the transition from (0) to (1). How much of the period is that?
  
  23. Jan 13, 2014
  
  Tanero
  
  wow! voko! you are opening my eyes on SHO! I never thought of period like this. So, it's T/4? right?
  
  24. Jan 13, 2014
  
  Tanero
  
  Well, I was trying to find other choices, but only these two angles make x(t=0)=0 .
  Moreover, problem is that when I put pi/2 to find my time I get negative time. That's why i chose 3/2pi to overcome it.
  
  Can you suggest the angle? I don't see. May be I can find angle from v0=v(t=0) part of solution. I know A, v0, w, then try to find angle through arcsin...
  
  25. Jan 13, 2014
  
  voko
  
  Yes, T/4 should be right. Sorry for not spotting the mistake earlier.
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