mechanics of materials
youngs modulus \[E= stress / strain \] \[E= \frac{\sigma } {\Delta L/L}\]
if we change stress by \( d\sigma\) , do we get \[E= \frac{d \sigma } {d L/L}\] ?
this bothers me becuse, on re-arranging \[\frac{dL}{d \sigma}= L/E\]
the solution to that is exponential, length changes exponentially when stress is increased
i was expecting it would be something similar to a spring,(linear) F=kx
it is a spring. i don't see how you got it was exponential.\[F=\color{#c00}{\frac{YA}L} x\]
youngs modulus is defined as stress by strain... lets consider unit cross section forget the A... strain is \[\Delta L / L\]
and we have stress proprtional to "strain" from youngs modulus unlike a spring, where force proportional to change in lenght
is it not the same case here?
as in, from the yongs mod formula, if i had specimens of two different lenghths L1 and L2, I would need DIFFERENT stresses to elongate BOTH by 1 metre
yes of course. but the real thing is if you double the respective stresses, then the change in length would be double. all springs are different in nature.
doubling stress would double "strain" i.e change in length divided by original length, the actual change in length would not double, it will be something else.... ?
the original length is constant anyway... if a double \(cx\), you also double \(x\).
\(L = 10cm\) \(\Delta L = 1cm\implies \dfrac{\Delta L}{L} = 0.1\) \(\Delta L = 2cm\implies \dfrac{\Delta L}{L} = 0.2\)
yes what if you are inceasing the stress in steps? \[\Delta L = ?\implies \dfrac{\Delta L}{1.1} \]
* 11.1
the reason why we look at "strain", that is, the percentage change in dimension, is because young's modulus is the property of a MATERIAL. we've observed that the PERCENTAGE change brought about by a given stress for all instances of a material is the same (for small stresses only, of course) no matter what the initial dimensions are
well doubling the stress would not double the strain in all cases.. we can conclude this looking at the graph |dw:1451471603734:dw|
yea, i'm consider inside elastic limit
*considering
\[\frac{dL}{d \sigma}= L/E\] This does give us an exponential relationship between \(L\) and \(\sigma\)
i think its boiling down to is L a constant or a variable??
That eqn is telling us that the length of rod grows exponentially as the stress is increased
a constant for a given rod!
just as you would wonder, "is cross-sectional area constant or variable?"
so we talking for cases in which elastic limit is not reached..?
physics aside, I'm just interpreting the differential eqn..
what if i changed stress in small steps, the new L would be the old L + the elongation
oh, you're talking about it like that. nice.
@imqwerty i only considering parts where that graph is a straight line
yes... if the steps are infinitely small....
now i fell there is something wrong with that... because of all the spring mass problems i've solved xD
*feel
\[E= \frac{d \sigma } {d L/L}\] this is something i made up, thinking what would happpen if i change stress in steps.. i do not know if it is correct
that follows directly from stress = E*strain right ?
yep
this is directly contrasting with the case of a spring, in a spring, the actual length of the spring does not matter, only its elongation with respect to equilibrium. however the yonugs modulus shows that its actulal length matters... if we were going to treat 'L' as a constant, then why define youngs mod as ratio of "stress to strain" rather than simply "stress to elongation" just like a spring?
i answered that before you even asked haha the reason why we look at "strain", that is, the percentage change in dimension, is because young's modulus is the property of a MATERIAL. we've observed that the PERCENTAGE change brought about by a given stress for all instances of a material is the same (for small stresses only, of course) no matter what the initial dimensions are
and why do you think that in case of a spring the actual length doesn't matter?! it does! it's just that in the equation of a spring, you do not get to see the dependence on length.
F=kx ?
Yes.\[k = \frac{YA}{L}\]
thats the formula for ^spring constant ? i.e specifically taken in the context of springs?
yes, of course
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