AlphaLearner
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Differentiating or integrating in presence of a constant (multiplied or divided) by function will not give zero.
I can write down an infinite number of different quantities. Like mpxhg or mpxhg^2 or mpxhg^3 etc. Just because I can write it down doesn't mean that it is physically interesting. In order for it to be interesting I would need to show that it has some useful relationship to other quantities, or some special properties that make it otherwise useful. I certainly wouldn't expect any textbooks to spend any time discussing why mpxhg is not useful.Mr real said:I was talking about the formula x.dF that if we integrate this for a constant force then the integral would be zero. I was not talking about F.dx.
I was agreeing with your point that if we consider x.dF then it wouldn't work for a constant force and that goes a step ahead in proving why it can't be considered ( But I need more explanation for the case when the force is variable). Thanks for making it a little more clearer.sophiecentaur said:I really have no idea what point you are trying to make. Random maths doesn't necessarily have any relation to Science. There are a million maths arguments that will tell you that 0=0 or 1=2 but they have no meaning.
Yes, dF is clearly saying that force is not constant. But did you see that 'x' alone? Says that displacement is constant. Work done is clearly zero if that 'x' does not vary in any way with respect to time.Mr real said:I was agreeing with your point that if we consider x.dF then it wouldn't work for a constant force and that goes a step ahead in proving why it can't be considered ( But I need more explanation for the case when the force is variable). Thanks for making it a little more clearer.
But x.dF doesn't say that x is constant just like F.dx doesn't say that F is constant, it only says that F is constant for a small displacement dx.AlphaLearner said:Yes, dF is clearly saying that force is not constant. But did you see that 'x' alone? Says that displacement is constant. Work done is clearly zero if that 'x' does not vary in any way with respect to time.
Correct. But it does say that F is not constant*, and often F is constant.Mr real said:But x.dF doesn't say that x is constant
If we are considering F.dx it means that F was constant during the displacement dx, it can vary during the whole process. Similarly x.dF means x was constant for force dF andAlphaLearner said:Just 'F' denote that the force was same and unchanged at all moments throughout the process.
You said that x.dF means that x is constant which it doesn't have have to be that's what I explained to you. Then you said what dx means which i am already pretty clear with. Please read the questions carefully before answering them.AlphaLearner said:Mr real, you are facing problem understanding mathematical expressions leading you to misconceptions in physics. I suggest you to have a look at this book "Calculus made easy" giving a clear idea of what 'dx' means and think about how it is applied in physics. You will find solution for this answer too.
But no one ever asked you regarding the meaning of dF or dx. Your comments are off-topic so please stop posting replies that are not relevant to the discussion.AlphaLearner said:Since there is no 'd' in front of 'x' it clearly states, 'x' is constant. Similarly no 'd' in front of 'F' says 'F' is constant.
This is not correct. For instance, for a spring F=-kx. So F is not constant, but the integral of F.dx is well defined.AlphaLearner said:Since there is no 'd' in front of 'x' it clearly states, 'x' is constant. Similarly no 'd' in front of 'F' says 'F' is constant.
But... F=-kx is an 'equation' expressing how force vary with change in displacement proportionally. F.dx is just an expression and when this small part F.dx is made to join with other remaining parts (integrating), even remaining parts should also be having same 'F' but different 'x'. Its like grouping up different members 'x' under same team 'F'.Dale said:This is not correct. For instance, for a spring F=-kx. So F is not constant, but the integral of F.dx is well defined.
It's a definite integral between equal limits. That gives zero.AlphaLearner said:Differentiating or integrating in presence of a constant (multiplied or divided) by function will not give zero.
Prove me then differential or integral of a function like f(x) = 2x will give a zero.sophiecentaur said:It's a definite integral between equal limits. That gives zero.
(I didn't know how to approach you so I'm replying to this post to get your attention). Please can you reply to post #48.sophiecentaur said:It's a definite integral between equal limits. That gives zero.
I have no idea what #49 is about.Mr real said:(I didn't know how to approach you so I'm replying to this post to get your attention). Please can you reply to post #49.
Well, that sounds like a reasonable heuristic, but mathematically neither F nor dx has any restrictions related to time. So I am not sure that it is exactly on point.Mr real said:Please correct me if I'm wrong. Here goes: F.dx is meaningful as it is possible to get dx displacement by applying force for an infinitesimal time but it would require infinite time to produce a displacement x from dF force, which is not possible.
Sorry I meant post #48.sophiecentaur said:I have no idea what #49 is about.
$$\int_1^1 2x \, dx = 0$$AlphaLearner said:Prove me then differential or integral of a function like f(x) = 2x will give a zero.