Gibbs Free Energy Derivation

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  • Опубликовано: 27 дек 2024

Комментарии • 40

  • @Vorpike
    @Vorpike 9 лет назад +23

    if you're looking for the uni level derivation (G naught and such), this isn't it, turn back now

  • @AKLECTURES
    @AKLECTURES  12 лет назад +4

    Hey! The change in enthalpy is zero for all elements in their standard states (1 bar pressure).

  • @AKLECTURES
    @AKLECTURES  11 лет назад

    I am happy that the video helped. What kind of help did you have in mind?

  • @ugursoydan8187
    @ugursoydan8187 4 года назад +1

    how can we find the proof of delta(G)=delta(G)0-RTlnQ equation?

  • @AKLECTURES
    @AKLECTURES  11 лет назад +1

    Glad it helped! You're welcome :)

  • @AKLECTURES
    @AKLECTURES  11 лет назад

    Thank you! Happy to know it helped

  • @keerthanaputhuvaya8893
    @keerthanaputhuvaya8893 10 лет назад +3

    i did not get the part where you said that -T(delta)S is gibbs energy....7th step....HOW ?

  • @OutTryingIt
    @OutTryingIt 11 лет назад +1

    Hi thanks for the great video.May I ask a question on the first part of the lecture?
    You said the number of moles are constant.But in a reaction like A+B=C won't the number of moles change. And if that were the case, now that P and T is constant, and n can change as shown the the equation, won't V also be able to change?
    But even if that were the case,delta H would still be equal to the heat exchanged Q since the pressure of the system is held constant?But im not sure about why n is constant.

  • @sedgieroobets
    @sedgieroobets 4 года назад +1

    I like this derivation as you show the importance of entropy in the wider universe in determining which reactions are allowed and which are not.

  • @vijayalakshmisrinivasan6028
    @vijayalakshmisrinivasan6028 Год назад +1

    Thanks ❤❤

  • @rohitranjan4416
    @rohitranjan4416 4 года назад +2

    well at 1.55 , DELTA H FORWARD = - DELTA H REVERSE , IT IS STATED UNDER LAVOISIER AND LAPLACE LAW NOT THE HESS LAW . OTHERWISE EVERYTHING IS GUD AND FINE , INFORMATIVE VIDEO BUT IT WAS UNDER LAVOISIER AND LAPLACE LAW NOT HESS LAW .

  • @fathimaanwar9029
    @fathimaanwar9029 3 года назад +1

    thankyou sir

  • @maxsmith7060
    @maxsmith7060 11 лет назад +2

    Thanks for this video, very helpful!
    Still, something remains unclear to me, maybe you would be so kind to answer it?
    The thermodynamic potential for G = U - TS + PV,
    with U the inner energy.
    With dU = T dS - PdV (no particle exchange assumed),
    this leads to dG = -SdT + VdP.
    You said that the derived equation, dG = dH - TdS, only holds for constant pressure and constant temperature (dP=dT=0). But then for the above eq. we have:
    dG = -SdT + VdP = 0 = dS_universe
    What is going on here?

    • @kenshabazz4288
      @kenshabazz4288 3 года назад

      ABSOLUTELY NOTHING...HIS EXPLANATION IS DRACONIAN AND IRRELEVANT..

  • @sahilagrawal1522
    @sahilagrawal1522 5 лет назад

    thanks very much.... i was not able to understand.. but now i am very good at this

  • @ashrafmuhammad255
    @ashrafmuhammad255 4 года назад

    What about open system, where mass id also exchanged ?

  • @davidselway651
    @davidselway651 9 лет назад

    Thank you for a very helpful video. At least to me , it makes clear how the Gibbs Free Energy relation is "derived" from a consideration of the second law in the form -- change in entropy of the universe is always non-negative. I do, however, have one problem with the derivation. In step 2 you use the ideal gas law to allow setting delta_V to zero. in a liquid (not gaseous) case isn't it true that the volume could also change in a chemical reaction?

  • @OutTryingIt
    @OutTryingIt 11 лет назад

    Also, I was also thinking if we were to state that yes the number of moles, remains constant, what if some of the n aren't gas molecules. that would also mean that the n in the formula PV=nRT isn't constant too.
    So these 2 are the main questions i have on why n must be a constant for this to happen.

  • @YasirAli-hj7vi
    @YasirAli-hj7vi 7 лет назад +1

    Great video

  • @Chloetray
    @Chloetray 8 лет назад

    great video thanks for your help!

  • @stanfordkoga-zs9nh
    @stanfordkoga-zs9nh 4 месяца назад

    Thank you

  • @adityaagarwal636
    @adityaagarwal636 4 месяца назад

    Thanks sir❤

  • @alexandriaviktor846
    @alexandriaviktor846 9 лет назад

    hai! can you explained about the equilibrium constant in Gibbs free energy..how the formula was formed

  • @daliaahmed5799
    @daliaahmed5799 11 лет назад +1

    Its amazing really very helpfull
    Can you please reply me cuz I am in a pharmacy school and learning physical chem and wants a lot of help please

  • @takikun1427
    @takikun1427 2 года назад

    Thankyou bro😭

  • @tanmay3717
    @tanmay3717 12 лет назад

    When is delta H sys zero?

  • @daliaahmed5799
    @daliaahmed5799 11 лет назад

    I am now learning Phs. Chem 239 and A lot of cocepts I cant get it from our intructor , now we have finished 1st and 2nd law of thermo dynamics

  • @arbutusunedo6866
    @arbutusunedo6866 5 лет назад

    It seems that there is a mistake here.. In gibbs free energy, only T and P is assumed to be constant, not V. I think the presenter confuses it with helmholtz free energy. In helmholtz free energy, T and V is taken constant, not P.

  • @saksham5346
    @saksham5346 Год назад +1

    Hi

  • @architsharma292
    @architsharma292 5 лет назад

    Cool vid

  • @shashanksingh6578
    @shashanksingh6578 5 лет назад

    Kaunsa desh ka hai be

  • @maxhblum2379
    @maxhblum2379 11 лет назад

    are you american? you dont sound like one

    • @mohammedusman8818
      @mohammedusman8818 6 лет назад

      who is an american??? or should i say...the american. 1st Obama now trump both of whom are americans. perhaps the only thing they have in common apart from the being a president

  • @sedgieroobets
    @sedgieroobets 4 года назад +2

    I like this derivation as you show the importance of entropy in the wider universe in determining which reactions are allowed and which are not.