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Posts posted by DQW
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Note that China and India have respectively 4 times and 3 times the population of the US. On the other hand, they both have much greater fractions of their populations living below the poverty line.China will produce about 3.3 million college graduates this year, India 3.1 million (all of them English-speaking), the U.S. just 1.3 million. In engineering, China’s graduates will number over 600,000, India’s 350,000, America’s only about 70,000[/b']..."0 -
Wrong slash on "\math"
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One of my favorites was Martin Gardner's Science Fiction Puzzles.
There's some really neat puzzles at rec-puzzles.org
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Where's the error in this
[math]\sqrt{x} = x^{1/2} = x^{2/4} = \sqrt[4]{x^2}[/math]
Substitute in -1:
[math]\sqrt{-1} = \sqrt[4]{(-1)^2} = \sqrt[4]{1} = 1[/math]
There is no imaginary constant' date=' they were tricking us all along!!![/quote']That's exactly the same as saying [imath] 2 = \sqrt{4} = -2 [/imath], so 2 =-2. Only, it throws in more steps in between to "cover up" the obvious logical misstep.
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I believe it was either Hardy or Bertrand Russell, but I could be remembering wrong.Yes I have seen that one before where the mistake made is the divide by 0. It is a good one though.I can't remember which mathematician did this but I'm sure someone will enlighten us.
He proved that if 1=2 you could prove anyone was the pope.
i.e. Fact 1: John and the pope are 2. Fact 2: 1=2 therefore we can deduce that John and the pope are 1.
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If you can find chemical equations for the combustion (burning in oxygen) of diamond/graphite/fullerene that specify the enthalpy change, then you have something. Since the in-plane C-C bonds in graphite (and fullerene) are a little stronger, I'd expect them to have slightly larger anthalpies.
Edit : found a link; scroll down on page - http://wine1.sb.fsu.edu/chm1045/notes/Energy/HessLaw/Energy04.htm
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http://www.unr.edu/sb204/geology/mas.html
(most reactive)
Lithium
Potassium
Calcium
Sodium
Magnesium
Aluminum
Manganese
Zinc
Chromium
Iron
Lead
Copper
Mercury
Silver
Platinum
Gold
(Least Reactive)
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Consider Na (not a transition) metal. Each Na atom has 1 electron in the outermost shell. For Na to react' date=' it needs to have this extra electron ripped out. And after this electron gets pulled out, Na attains a very stable, Noble Gas configuration.????not very clear.....
any one?
[b']The high stability of the end-product and the relative ease of getting there is what makes Na very reactive.[/b]
Now consider Fe (a transition metal), which has the configuration [Ar] 3d6 4s2. The best you can do with Fe is pull out 2 electrons to make it [Ar] 3d5 4s1 (both half-filled subshells) or 3 electrons, to make it [Ar] 3d5 (one half-filled subshell). So, you see that for Fe to react, you must (i) pull out more electrons, (ii) and still not reach the "most" statble configuration (only a local minimum). Removing all the 3d and 4s electrons takes too much energy, so Fe can really never attain a Noble Gas configuration.
The not-so-great stability of the end-product and the relative difficulty of getting there is what makes Fe not so reactive.
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why do you obtain energy when bonds are formed??
Voila !
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If you are allowed to use the derivative of the logarithm (which is no more fundamental than that of the exponent), you have correctly found the answer, dy/dx = y = e^xI was given[math]y = e^x[/math]
So I did this!
[math]\ln y = x \ln e[/math]
[math]dx/dy = 1/y[/math]
[math]dy/dx = y[/math]
Am I making some illegal moves?
If you have to prove this from "more fundamental" results, I suggeswt you use the series expansion for e^x and differentiate term by term.
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...except that you haven't stated what the question asks for. You have merely provided an expression and asked for an answer.
Yes, it's obvious that you are required to simplify the provided expression, but unless you state this explicitly, the question does not exist.
Henceforth, please state the question in its entirety.
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Wait a minute : chemical equations are completely different from mathematical equations !!!
To all posters : please, PLEASE, post you problems/questions EXACTLY as they are given to you. What can you possibly gain by rewording it ?
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There are formulae used to calculate various hardness values based on expirimental data. For instance the Vickers hardness depends on the apex angle of the indenter, the applied load and the size of the indentation. You can probably find this online somewhere.
On the other hand, if the question wants you to derive (empirically) a relation between say, bond length and bond energy, that would be more interesting.
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Perhaps the bond energy ? The C - C single bond has an energy of 348 kJ/mol. Also, the bond energy varies roughly inversely with the bond length, which for the C - C bond is 154 pm.The strength of these bonds is a function of the degree to which the orbitals of neighboring atoms overlap, but I'm not sure how to quantify that into a number.http://www.science.uwaterloo.ca/~cchieh/cact/c120/bondel.html
The in-plane bond length in graphite is about 142 pm and hence these sp2 bonds are stronger that the bonds in diamond. But the interplanar spacing is about 335 pm, and the van der waals energy holding the layers together is small (roughly about 10 kJ/mol).Graphite is also formed by covalent bonding of carbon atoms using hybrid orbitals, but they are bonded together with pi bonds in addition to sigma bonds. These bonds allow electrons to travel between atoms with greater ease than in diamond, resulting in graphite's electric conductivity. In fact, the pi and sigma bonding in graphite makes graphite's bonds stronger than diamond's. The reason graphite is flaky and used as lead in pencils is because of the weak van der Waals forces between the sheets of graphite.Also, to say that "These [pi] bonds allow electrons to travel between atoms with greater ease" is like putting the cart before the horse. It is the delocalized 4th electron (of each C-atom) that gives rise to the distributed (meaning, the positions of the pi bonds are not fixed, just like in benzene) pi bonds in graphite.
Correct. The C-atoms in fullerenes are also sp2 hybrid, but being non-planar, the bond angles are smaller than 120 deg.Hope I've helped. I'll look for some more information on fullerene, but I think it possesses both pi and sigma bonds just as graphite does.0 -
OK' date=' here's the question:
Neutrons were discovered in 1932, more than 10 years after the existence of isotopes was confirmed. What property of electrons and protons led to their discovery?
I don't know the answer at all! Please help![/quote']1. Is the question (the last part) asking about the discovery of electrons and protons ?
2. What have you tried so far, to tackle this problem ?
3. What have you found out that may be relevant ?
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Oh, but if the units you are using are the least count (or resolution) of your fluxmeter, then you can only measure whole number units of flux.
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Not just possible, but a certainty !
Or by chance are you getting confused with the flux through a superconductor in the Abrikosov phase? That will always be an whole number multiple of h/2e.
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Sounds like the kind of strategery that the dude in your picture would come up with.
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Ah, I see.
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Don't know what I was thinking...ignore that.nope, think that the sum of the gp 1/2+1/4+1/8+... is 1.The wall I found myself running against was in understanding completeness (for QM). I got a feel for completeness (of an infinite set of orthogonal functions) in terms of being able to write any continuous function as a linear combination of the basis functions. Beyond that, one runs into Lebesgue integrals
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Alternatively, noticing that the Langrangian is not explicitly time-dependent, you can directly write H=T+V.
PS : This is a purely classical problem - nothing quantum about it (in fact, I don't see any physical chem in it either).
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Sorry for the "extended digression"...this will be the last of it (and it's only for the sake of completeness).
I recall arriving at the energy-time uncertainty by thinking about correlation amplitudes (courtesy Sakurai).
For a continuous spectrum you can write :
[math]C(t) = \langle \alpha,0|\alpha,t \rangle = \int dE |g(E)|^2 \rho(E) exp \left( \frac{-iEt}{\hbar} \right) [/math]
Now for a real, physical problem let [imath]|g(E)|^2 \rho(E)|[/imath] be peaked at some E = U. Then writing
[math]C(t) = exp \left( \frac{-iUt}{\hbar} \right) \int dE |g(E)|^2 \rho(E) exp \left( \frac{-i(E-U)t}{\hbar} \right) [/math]
For large t, the integrand oscillates rapidly unless |E-U| is small compared to [imath]\hbar /t [/imath]. So to not see significant deviations from C(t) = 1, you need [imath]t |E-U| \equiv t~\Delta E < \hbar [/imath].
And this is not true only in the case of a continuous spectrum.
Okay, now back to the naked singularity....
It has been shown repeatedly, I believe, (and Hawking has had to eat his words on this) that observable singularities can exist (from the collapse of a scalar field, for instance). So I don't see the validity of the question.
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That's not fair, Swansont. The energy-time uncertainty does not come out of QM the same way as the x,p relation. Yes, energy (frequency) and time are canonical conjugate variables (fourier transforms of each other), and this provides an argument for the existence of an energy-time uncertainty relation. You can't do the same thing that you do with position-momentum, because time is not an observable in NRQM. The way I arrive at the HUP relation for x,p is by plugging in for <[x,p]> and <{x,p}> in the Schwarz Inequality and juggling with the math (of hermitian and anti-hermitian operators), but there exist no canonical commutation relations for E,t so I can't do the same with them.
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The book's answer is correct. So are your steps up to everything that you've shown. (points are correct; slope is correct)
Perhaps you made a mistake substituting (x1,y1) in the final equation. Which point did you use - M or N ? I suggest you recheck this last bit of working, or show what you did.
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Metric Tensor?
in Linear Algebra and Group Theory
Posted
Cheers !
I don't believe there is a way to delete a post entirely.