giokrutoi
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yes I forgot that but I don't think that it's the write solution because that 10 centimeters are maximal extension for both but not for m2
That simple analysis is attractive, but incorrect. After m1 is released and before m2 is released, m1 is undergoing simple harmonic motion. It is easy to see that the maximal compression is 10 cm shorter than relaxed and that the maximal extension is 10 cm longer than relaxed. This motion can optionally be maintained for many cycles before m2 is finally released.giokrutoi said:maximal compression may be 10 centimeters and if that's true force should be 10 centimeter multiplied by k and acceleration of second mass should be this magnitude divided by m2
and yes I mean right when I write write
I understood what you have said and may guess was very silly but how can I solve this problem i wrote conservation of momentum up in commentary's and some of them said it was wrongjbriggs444 said:That simple analysis is attractive, but incorrect. After m1 is released and before m2 is released, m1 is undergoing simple harmonic motion. It is easy to see that the maximal compression is 10 cm shorter than relaxed and that the maximal extension is 10 cm longer than relaxed. This motion can optionally be maintained for many cycles before m2 is finally released.
When m2 is released, the spring is at its relaxed length. If m2 were still held stationary, the spring would eventually extend 10 cm longer than relaxed. But because m2 has been released, we are no longer assured that this will be the case.
One line of analysis that indicates that it cannot be the case is based on energy. Think initially about the state with mass m2 pinned in place. In its compressed state, the spring has a certain amount of potential energy. That amount of energy can be calculated based on the 10 cm number and the spring constant. In its extended state, the spring has that same amount of potential energy. In both cases the system has zero kinetic energy. All of the energy is in the spring.
The pin holding m2 in place is doing no work. It applies a force, but it is motionless. Following release the pin holding m2 in place still does no work. Accordingly, energy is conserved within the m1, m2, spring system both before and after the release of m2.
If m1 and m2 were both motionless then the spring would have to extend or compress to the full 10 cm in order for energy to be conserved. But as long as either are in motion, the spring cannot ever extend that far without violating energy conservation. But momentum is conserved following release of m2, so it can never be the case that both m1 and m2 are motionless following the release of m2.
giokrutoi said:yes I forgot that but I don't think that it's the write solution because that 10 centimeters are maximal extension for both but not for m2
I was going to point this out, but ehild has done so previously.ehild said:Do you mean "right" when you write "write"?
ok I made mistake sorrySammyS said:I was going to point this out, but ehild has done so previously.
"Right" = Correct ≠ "Write"
Right ?
but what can you say about soluteSammyS said:I was going to point this out, but ehild has done so previously.
"Right" = Correct ≠ "Write"
Right ?
Too many helpers at one time is not good.giokrutoi said:but what can you say about solute
but whom should I trust they are saying opposite thingsSammyS said:Too many helpers at one time is not good.
ehild and briggs are excellent.
We are saying identical things.giokrutoi said:but whom should I trust they are saying opposite things
but you say that it is impossible 10cm to be maximal extentionjbriggs444 said:We are saying identical things.
I say that it is not possible for 10 cm to be the maximal extension following release of m2. I do not see ehild making any contrary claim.giokrutoi said:but you say that it is impossible 10cm to be maximal extention
That says nothing about 10 cm.giokrutoi said:this
ehild said:Yes, but you need to calculate the compression in meters, and that should be multiplied by k=20 N/m.
No. We are not saying opposing things.giokrutoi said:see you are saying opposing things
I think that your argument is more convincingjbriggs444 said:I say that it is not possible for 10 cm to be the maximal extension following release of m2. I do not see ehild making any contrary claim.
Edit: In any case, one should judge the truth of the matter by the strength of the arguments offered, not based on trust. If you can follow the arguments and see that the results follow, all is well. .
giokrutoi said:maximal compression may be 10 centimeters and if that's true force should be 10 centimeter multiplied by k and acceleration of second mass should be this magnitude divided by m2
and yes I mean right when I write write
ehild said:Yes, but you need to calculate the compression in meters, and that should be multiplied by k=20 N/m.
Sorry, I made a mistake, the maximum distortion is not 0.1 m when both blocks move. You have to determine it first.giokrutoi said:maximal compression may be 10 centimeters and if that's true force should be 10 centimeter multiplied by k and acceleration of second mass should be this magnitude divided by m2
Well, the 20 N/m is new to me. May I remind you of post # 2? You are now at over 70 posts and still drag in new things (yang ??) that indicate to me that post #6 still applies.giokrutoi said:I have stated that before
giokrutoi said:i was thinking about this problem and i came to conclusion that post 33 makes sense if v2 is maximal
EDIT: If that's wrong than period of second object maybe 2 pi m2/k2 1/2 were k2 is different from k which is given because according to yang's theory when spring's length is decreased (it is decreased because I write origin of spring in the center of mass) then k must go up so if I call Z as length of spring when it is relaxed then if I subtract length from m1 to center of mass I will get length of spring from center of mass to m2 and with help of proportion I will calculate k2 which will be higher that original k
can this help me?
in file which i have attached to post 33 there is v2 and I state that it is maximumehild said:What is v2? what do you mean that it is maximal?
If you take the spring as two strings, connected at the centre of mass, you can determine the spring constant of both, and also the vibration frequency. Go ahead.
No. Check the parentheses and dimensions. I do not understand the sentence "if k constant from Z is k then for D length it is k(m1+m2)"giokrutoi said:in file which i have attached to post 33 there is v2 and I state that it is maximum
but i guess that conclusion( in post 33) is wrong because i didn't take in consideration that all the energy can't be in m2
now period of second mass is 2 pi square root from m2 / k2 k2 is spring constant derived from here
if length of spring is Z then center of mass must be on that spring but it must be closer to the bigger mass so if i call distance from m2 to center of mass D than I have to find D
D is derived from here m1(Z-D)=m2D D=Z/m1+m2 so if k constant from Z is k then for D length it is k(m1+m2)
so period is 2 p square root from m2/k(m1+m2)
is that right
I can not read your attachment. Type in your work.giokrutoi said:sorry i made mistakes there
here in attached file I wrote correct
if spring has length Z and i call D length from m2 to center of mass then m1(Z-D)=m2Dehild said:I can not read your attachment. Type in your work.
from center of mass to m2ehild said:The spring constant of which piece is k1?
The period is correct.
i calculated and it's sameehild said:OK, but would not it be more logical to call it k2? And what is the spring constant of the other piece and the period of mass m1?
Yes.giokrutoi said:EDIT :Now acceleration is omega squared times maximal strechment so omega squared is m1m2/(m1+m2)k
all I have to do is to calculate maximal strechment is that right?
Possibly, it's hard to be sure without seeing your working and answer. Keeping all the given data symbolic, (m1 etc.) what expression do you get for the max acceleration of m2?giokrutoi said:hey I think I figured out everything
look
we can calculate maximal speed of m1 at the release point from conservation of energy all the potential energy is converted in kinetic of m1
then this v is maximal for m1 thing is that m1's coordinate dependence on time look's so
y=XmaxSINUS OMEGA t were we know omega
t is time Xmax is maximal compression
now if we take derivative from that equation we will get velocity dependence on time
v=VmaxCOSINUS omega t
vmax is maximal velocity of m1 in reference frame of center of mass so we have to subtract velocity of center of mass from v maximal which we defined by conservation of energy
vmax also equals XMAX times omega so we know vmax and omega and we can find Xmax
now acceleration of first mass is omwga squared vmax we know both omega and vmax so we can find acceleration a1
then m1a1=m2a2 a2=m1a1/m2
is that conclusion right
no I have spring constant 20n/m.i forgot to mention it in early posts I said that k is givenharuspex said:not the spring constant, right?
That Vmax is valid in the ground frame of reference. After m2 is released, the whole system translates with the velocity of the center of mass, so both objects move with that velocity + the velocity of their vibration.giokrutoi said:hey I think I figured out everything
look
we can calculate maximal speed of m1 at the release point from conservation of energy all the potential energy is converted in kinetic of m1
then this v is maximal for m1 thing is that m1's coordinate dependence on time look's so
y=XmaxSINUS OMEGA t were we know omega
ehild said:That Vmax is valid in the ground frame of reference. After m2 is released, the whole system translates with the velocity of the center of mass, so both objects move with that velocity + the velocity of their vibration.
You turned to the center of mass frame of reference, where the blocks oscillate , but the maximum speed of oscillation is different from Vmax you got previously. You have to subtract the velocity of the center of mass.
If you got it, you can use that the maximum acceleration is maximum speed multiplied by omega. that you know already.
Just to check, the max acceleration I got for m2 is ##\frac{kx_1}{\sqrt{m_2(m_1+m_2)}}##giokrutoi said:yes that's exactly what I was saying
thanks a lot. For waisting your time on. Helping me
It depends what x1 means. It should be the initial compression, 0.1 m.haruspex said:Just to check, the max acceleration I got for m2 is ##\frac{kx_1}{\sqrt{m_2(m_1+m_2)}}##
ehild said:It depends what x1 means. It should be the initial compression, 0.1 m.
Yes, that looks to be what I did too. No need to get into the SHM details.ehild said:I outline the energy method suggested by jbriggs and me :
ΔL = 0.1 m is the initial compression of the spring.
V1 is the maximum speed of block1 after it was released, but block2 still fixed.
The total energy of the system is 1/2 m1V12=1/2 k (ΔL)2
##V_1 = \sqrt \frac {k}{m_1}\Delta L##
Speed of the CoM ##V_{CoM}= \frac {m_1V_1}{m_1+m_2}##
energy of translation ##E_{tr}=1/2 (m_1+m_2 ) \left( \frac {m_1V_1}{m_1+m_2} \right)^2##.
Let be S the maximum distortion of the spring after both blocks were released.
The spring energy is ##E_s =E-E_{tr}= 1/2 V_1^2 \frac {m_1m_2}{m_1+m_2}= 1/2 k S^2##
##S=V_1^2\sqrt {\frac {m_1m_2}{k(m_1+m_2)}}## and a2=KS/m2.