Deriving general specific heat capacity formula

In summary: 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?
  • #1
ChiralSuperfields
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Homework Statement
Please see below
Relevant Equations
Please see below
For this,
1681169914989.png

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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  • #2
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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  • #3
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!
 
  • #4
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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  • #5
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!
 
  • #6
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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  • #7
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!
 
  • #8
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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  • #9
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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