Deriving general specific heat capacity formula

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The forum discussion centers on deriving the specific heat capacity formula, specifically the equation c = \frac{\Delta Q}{m \Delta T}. Participants debate the physical significance of \Delta Q and its relationship to heat transfer, with emphasis on the concept that heat is not a state function. The conversation highlights the importance of understanding heat as a summation of differential elements dQ and the implications of using derivatives of internal energy or entropy in defining specific heats. The conclusion drawn is that while \Delta Q can be considered meaningful in certain contexts, it must be approached with caution due to its differential nature.

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Dose anybody please know of a better way to derive the formula without having ##c = \frac{\Delta Q}{m \Delta T}## then taking the limit of both sides at ##\Delta T## approaches zero? I thought ##\Delta Q## like ##\Delta W## was not physically meaningful since by definition ##Q## is the heat transfer.

Many thanks!
 
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ChiralSuperfields said:
I thought ##\Delta Q## like ##\Delta W## was not physically meaningful since by definition ##Q## is the heat transfer.
Do you think that ##Q## is physically meaningful?
 
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kuruman said:
Do you think that ##Q## is physically meaningful?
Thank you for your reply @kuruman!

Yes I do, since it is the quantity of heat transferred.

Many thanks!
 
ChiralSuperfields said:
Thank you for your reply @kuruman!

Yes I do, since it is the quantity of heat transferred.

Many thanks!
Well, ##Q##, which is physically meaningful, is not transferred instantaneously all at once but in increments ##\Delta Q##. Why is ##Q## meaningful but not an element ##\Delta Q## that is part of it? BTW, the same reasoning applies to ##\Delta W.##
 
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kuruman said:
Well, ##Q##, which is physically meaningful, is not transferred instantaneously all at once but in increments ##\Delta Q##. Why is ##Q## meaningful but not an element ##\Delta Q## that is part of it? BTW, the same reasoning applies to ##\Delta W.##
Thank you for your reply @kuruman!

So could we think of the heat transferred as the summation of the differential heat elements ##dQ## which I think leads to ##Q = \int dQ##.

However, back to the algebra way of thinking, is the reason why the heat element ##\Delta Q## is not meaningful because it is causes a differential change in the state of the system that can be considered negligible?

Many thanks!
 
ChiralSuperfields said:
Thank you for your reply @kuruman!

So could we think of the heat transferred as the summation of the differential heat elements ##dQ## which I think leads to ##Q = \int dQ##.

However, back to the algebra way of thinking, is the reason why the heat element ##\Delta Q## is not meaningful because it is causes a differential change in the state of the system that can be considered negligible?

Many thanks!
Why do you insist ##\Delta Q## is not meaningful? In post #3 you agreed that it is.
 
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kuruman said:
Why do you insist ##\Delta Q## is not meaningful? In post #3 you agreed that it is.
Thank you for your reply @kuruman!

Yeah I guess it is meaningful if we think of it has a differential heat element not as ##Q_f - Q_i## which cannot be true since heat is state variable.

Many thanks!
 
The specific heats are defined in terms of derivatives of intenal energy or entropy not of heat. And as definitions, they cannot be proven.
The heat is not a function of state so using the derivative of heat in respect to temperature it may be a little hand waving.
 
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nasu said:
The specific heats are defined in terms of derivatives of intenal energy or entropy not of heat. And as definitions, they cannot be proven.
The heat is not a function of state so using the derivative of heat in respect to temperature it may be a little hand waving.
Thank you for your reply @nasu!

That is very interesting what you mention. Sorry I did quite get the bit I put it italic above. I don't understand the bit about hand waving. Is it still correct what the textbook did?

Many thanks!
 

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