Final temperature of diamond using Cv

In summary, at low temperatures, the coefficient of viscosity of solids is given by: Cv = D(\frac{T}{\Theta})3 where: D = 1.94*10^3 for diamond at 1860K; if 100J of heat is transferred to 1mole of diamond, initially at 10K, the final temperature will be given by: Cv = D(\frac{T}{\Theta})3
  • #1
Ryomega
67
0

Homework Statement



At low temperatures, Cv of solids is given by:

Cv = D([itex]\frac{T}{\Theta}[/itex])3

where:

D = 1.94*10^3
[itex]\Theta[/itex] = Debye Temperature, for diamond 1860K

If 100J of heat is transferred to 1mole of diamond, initially at 10K. Calculate the final temperature.

Homework Equations



Cv = D([itex]\frac{T}{\Theta}[/itex])3
Q = mCv(Tf-Ti)


The Attempt at a Solution



This is a straight forward question as the equation becomes:

Q = mCv(Tf-Ti)

Tf = [itex]\frac{Q}{mC}[/itex]+Ti


So the real problem I'm having is the fact that Cv is a function of T and T is changing as heat is being put in.
So how do I go about this question?

Thanks in advance
 
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  • #2
Oh and I'm guessing mass is just 1 molar mass of carbon
 
  • #3
dQ = CvdT

Plug in your expression for Cv and integrate from 10 to T:

Q = 1000J = ∫CvdT' from [10, T]

then solve for T.
 
  • #4
Oh... that would do it... *Face Palm*

Can't BELIEVE I didn't see that.:rolleyes:

Thanks!
 
  • #5
Actually how do you propose to do that?

Cv is the only variable changing with Temperature so:

Cv = D[itex]\int[/itex][itex]\frac{T^3}{θ^3}[/itex]

Cv = [itex]\frac{D}{θ^3}[/itex][itex]\int[/itex]T3 (from 10 to Tf)

Cv = [itex]\frac{D}{4θ^3}[/itex] (T4f-104)

Q =mCv (Tf-10)

Q =[itex]\frac{mD}{4θ^3}[/itex] (T4f-104)

Let A = [itex]\frac{mD}{4θ^3}[/itex]

Q =A (Tf-10) (T4f-104)

At this point it becomes pretty much impractical to solve. Am I doing something wrong?
 
  • #6
Q is the heat you added to the system, 1000J. It's just simple algebra from there.
 
  • #7
If we expand it (Q = 100J btw)

[itex]\frac{T^5}{10}[/itex] -T4-103T-104=[itex]\frac{10}{A}[/itex]

I suppose you're going to tell me I have to do long division? No easier way?
 
  • #8
Ryomega said:
Actually how do you propose to do that?

Cv is the only variable changing with Temperature so:

Cv = D[itex]\int[/itex][itex]\frac{T^3}{θ^3}[/itex]

Cv = [itex]\frac{D}{θ^3}[/itex][itex]\int[/itex]T3 (from 10 to Tf)

Cv = [itex]\frac{D}{4θ^3}[/itex] (T4f-104)

Q =mCv (Tf-10)

Q =[itex]\frac{mD}{4θ^3}[/itex] (T4f-104)

Let A = [itex]\frac{mD}{4θ^3}[/itex]

Q =A (Tf-10) (T4f-104)

At this point it becomes pretty much impractical to solve. Am I doing something wrong?

No, your integration is wrong here.

Q = ∫CvdT = A(T4 -104)

Q/A + 104 = T4

T = (Q/A + 104)1/4
 
  • #9
Wow... I should go back to school. Thanks a lot.
 

Related to Final temperature of diamond using Cv

What is the specific heat capacity (Cv) of diamond?

The specific heat capacity of diamond is approximately 0.519 joules per gram per degree Celsius (J/g°C).

How is the final temperature of diamond calculated using Cv?

The final temperature of diamond can be calculated using the formula Tf = Ti + Q/mCv, where Tf is the final temperature, Ti is the initial temperature, Q is the amount of heat transferred, m is the mass of the diamond, and Cv is the specific heat capacity.

What factors affect the final temperature of diamond when using Cv?

The final temperature of diamond can be affected by the initial temperature, the amount of heat transferred, and the mass and specific heat capacity of the diamond.

Is the final temperature of diamond using Cv affected by the pressure or environment?

No, the final temperature of diamond using Cv is not affected by pressure or environment, as long as the diamond remains in a closed system and does not undergo any phase changes.

How accurate is the final temperature of diamond using Cv in real-life scenarios?

The final temperature calculated using Cv is an approximation and may vary from real-life scenarios due to factors such as heat loss to the surroundings and the presence of impurities in the diamond. However, it can still provide a good estimate of the final temperature in most cases.

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