Question- Newton's Law of Cooling

AI Thread Summary
The discussion centers on solving a problem using Newton's Law of Cooling, specifically determining the time it takes for a hot body to lose 90% of its maximum heat. The initial attempt involved calculating temperature differences and using a simplified version of the cooling law, which led to an incorrect time estimate. It was clarified that the approximation used is only valid for small temperature changes, which does not apply in this scenario due to the significant temperature difference throughout the cooling process. The correct approach involves integration to account for the changing rate of heat loss as the temperature difference decreases. Ultimately, the accurate solution is found to be t = ln(10)/k, emphasizing the importance of understanding the conditions under which approximations can be applied.
sankalpmittal
Messages
785
Reaction score
27

Homework Statement



A hot body placed in the surrounding of temperature θo obeys Newton's law of cooling dθ/dt = -k(θ-θo), where k is any constant. Its temperature is θ1 at t=0. t is time. The specific heat capacity of body is "s" and its mass is "m". Find the time starting from t=0 in which it will lose 90% of the maximum heat.

Homework Equations




http://www.ugrad.math.ubc.ca/coursedoc/math100/notes/diffeqs/cool.html


The Attempt at a Solution



I solved it via integration and got the correct answer as well. As far as I know, it can be solved without integration:

The maximum heat body can lose has to be ms(θ1o). If only 90 percent of this maximum heat is lost, we have, Heat lost = 9ms(θ1o)/10. As ms is constant we have, Temperature difference = 9(θ1o)/10

Initial temperature of body at time t=0 : θ1
Final temperature of body when it cools as per condition : θ1 - 9(θ1o)/10 = (θ1 + 9θo)/10

Average temperature of body = (Initial temperature + Finial temperature)/2 = (11θ1 + 9θo)/20

In magnitude only, we can write law as, Δθ/Δt= k(θ-θo)

Now change in temperature Δθ = Final temperature of body when it cools as per condition - Initial temperature of body at time t=0 = 9(θ1o)/10

Now Δt = t-0=t
θ-θo = Average temperature of body - θo = 11(θ1o)/20

Now putting all these values in Δθ/Δt= k(θ-θo), we get

9/t = 11k/2 => t = 18/11k

But the answer is t= ln(10)/k = 2.303/k.

Where did I go wrong ?

Please help !

Thanks in advance... :smile:
 
Physics news on Phys.org
sankalpmittal said:

Homework Statement



A hot body placed in the surrounding of temperature θo obeys Newton's law of cooling dθ/dt = -k(θ-θo), where k is any constant. Its temperature is θ1 at t=0. t is time. The specific heat capacity of body is "s" and its mass is "m". Find the time starting from t=0 in which it will lose 90% of the maximum heat.

Homework Equations

http://www.ugrad.math.ubc.ca/coursedoc/math100/notes/diffeqs/cool.html

The Attempt at a Solution



I solved it via integration and got the correct answer as well. As far as I know, it can be solved without integration:

The maximum heat body can lose has to be ms(θ1o). If only 90 percent of this maximum heat is lost, we have, Heat lost = 9ms(θ1o)/10. As ms is constant we have, Temperature difference = 9(θ1o)/10

Initial temperature of body at time t=0 : θ1
Final temperature of body when it cools as per condition : θ1 - 9(θ1o)/10 = (θ1 + 9θo)/10

Average temperature of body = (Initial temperature + Finial temperature)/2 = (11θ1 + 9θo)/20

In magnitude only, we can write law as, Δθ/Δt= k(θ-θo)

Now change in temperature Δθ = Final temperature of body when it cools as per condition - Initial temperature of body at time t=0 = 9(θ1o)/10

Now Δt = t-0=t
θ-θo = Average temperature of body - θo = 11(θ1o)/20

Now putting all these values in Δθ/Δt= k(θ-θo), we get

9/t = 11k/2 => t = 18/11k

But the answer is t= ln(10)/k = 2.303/k.

Where did I go wrong ?

Please help !

Thanks in advance... :smile:

Your problem is that the equation Δθ/Δt= k(θ-θo) is only valid when Δθ and Δt are very small, but they're not small here. You're basically treating the problem as though the heat flow is constant over the total duration of the problem, but you know that's not true: as the temperature difference between the body and the environment decreases, the rate of heat flow also decreases. That's why you need to solve the problem by integration.
 
Mute said:
Your problem is that the equation Δθ/Δt= k(θ-θo) is only valid when Δθ and Δt are very small, but they're not small here. You're basically treating the problem as though the heat flow is constant over the total duration of the problem, but you know that's not true: as the temperature difference between the body and the environment decreases, the rate of heat flow also decreases. That's why you need to solve the problem by integration.

But my textbook and reference books say that Newton's law of cooling in only valid when temperature difference between body and surrounding is not very large that is small. So why cannot I use the method in "Attempt at solution" here ?

In other words the books say that Newton's law of cooling itself is true for only small temperature difference. Question says that the body obeys Newton;'s law of cooling. So temperature difference between body and surrounding is also small. Am I correct ?
 
sankalpmittal said:
But my textbook and reference books say that Newton's law of cooling in only valid when temperature difference between body and surrounding is not very large that is small. So why cannot I use the method in "Attempt at solution" here ?

In other words the books say that Newton's law of cooling itself is true for only small temperature difference. Question says that the body obeys Newton;'s law of cooling. So temperature difference between body and surrounding is also small. Am I correct ?

Small compared to what? You need to be clear on what "small" and "large" are in reference to when using approximation techniques.

In this case, using your "attempt at solution" method requires that Δθ = θ(t + Δt) -θ(t) is small in the sense that Δθ = θ(t + Δt) -θ(t) ≈ θ'(t)Δt is a valid approximation, which requires that Δt is small compared to the timescale 1/k in the problem. Your method finds that the time between the initial and final condition is ~ 1.64/k, which is of course not small compared to the typical 1/k timescale. Hence, the conditions under which you used your approximation are violated, as indicated by your solution.

Note that these conditions of "smallness" are different from the conditions under which even the differential form of Newton's law, θ'(t) = k(θ-θo), holds. There, the "small" temperature difference is likely referring to the difference between the body and the environment. Probably, the "smallness" is determined by requiring that the heat-transfer coefficient between the two bodies is approximately constant (temperature independent). This temperature-scale could be much larger than the Δθ = θ(t + Δt) -θ(t), and so has no bearing on whether you can approximate Δθ = θ(t + Δt) -θ(t) ≈ θ'(t)Δt (except to say that the whole law is invalid if the heat-transfer coefficient is not constant).
 
  • Like
Likes 1 person
Mute said:
Small compared to what? You need to be clear on what "small" and "large" are in reference to when using approximation techniques.

In this case, using your "attempt at solution" method requires that Δθ = θ(t + Δt) -θ(t) is small in the sense that Δθ = θ(t + Δt) -θ(t) ≈ θ'(t)Δt is a valid approximation, which requires that Δt is small compared to the timescale 1/k in the problem... Snip

Great Explanation Mute ! I get the concept now ! Thanks a lot ! :)
:smile:
 
Thread 'Collision of a bullet on a rod-string system: query'
In this question, I have a question. I am NOT trying to solve it, but it is just a conceptual question. Consider the point on the rod, which connects the string and the rod. My question: just before and after the collision, is ANGULAR momentum CONSERVED about this point? Lets call the point which connects the string and rod as P. Why am I asking this? : it is clear from the scenario that the point of concern, which connects the string and the rod, moves in a circular path due to the string...
Thread 'A cylinder connected to a hanged mass'
Let's declare that for the cylinder, mass = M = 10 kg Radius = R = 4 m For the wall and the floor, Friction coeff = ##\mu## = 0.5 For the hanging mass, mass = m = 11 kg First, we divide the force according to their respective plane (x and y thing, correct me if I'm wrong) and according to which, cylinder or the hanging mass, they're working on. Force on the hanging mass $$mg - T = ma$$ Force(Cylinder) on y $$N_f + f_w - Mg = 0$$ Force(Cylinder) on x $$T + f_f - N_w = Ma$$ There's also...
Back
Top