Time for a steel die to reach temperature

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Discussion Overview

The discussion revolves around the thermal dynamics of a steel die during an experiment involving the heating and quenching of a boron steel specimen. Participants explore the time it takes for the die to reach a certain temperature due to heat conduction from the heated specimen, focusing on calculations and assumptions related to thermal properties and heat transfer.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Exploratory

Main Points Raised

  • One participant outlines an experimental setup involving heating a steel specimen to 950°C and transferring it to a die at room temperature, seeking to estimate the time for the die to reach 60-80°C.
  • Another participant proposes a formula to estimate the temperature rise of the die based on the specific heat and volumes of the specimen and die, suggesting a minimal temperature increase of less than one degree.
  • A subsequent reply questions the accuracy of the initial calculation, proposing an alternative formula for temperature estimation that leads to a revised temperature for the next experiment.
  • Participants discuss the significance of specific heat differences between the specimen and die, with one suggesting that the difference may not be crucial for the calculations.
  • There is a request for clarification on the origin of the proposed equations, indicating that some participants find the solutions unexpectedly simple compared to their own research.
  • A later reply explains the conservation of heat energy principle as the basis for the temperature calculation, emphasizing the importance of mass and specific heat in the context of the experiment.

Areas of Agreement / Disagreement

Participants express varying degrees of confidence in the calculations and assumptions made, with some uncertainty about the significance of specific heat differences and the accuracy of the proposed formulas. No consensus is reached on the best approach or the validity of the calculations.

Contextual Notes

Limitations include assumptions about specific heat being equal and the neglect of other factors such as heat loss to the environment or the effects of stamping on temperature changes.

Thoomy
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Hello. I will be doing some experiments with boron steel. The idea is to heat a steel specimen (200x20x1,5 mm dimensions) to 950°C and then quickly transfer it from the oven to the die at room temperature. When the specimen reaches the steel die it will supposedly be at around 800°C. At this temperature, the upper and lower die close and come into contact with the specimen which rapidly cools and quenches in 15 seconds. Since the tool is not cooled, I am now trying to calculate an approximate time when the dies will be at certain temperature (lets say around 60- 80°C) beacuse of the heat conduction from the specimen. The upper and lower die combined are approximately 200x200x150mm in size. Since I will be doing this experiment repeatedly I need at least some kind of orientation how long the experiments will last. Thank you for any help or advice.
 
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Assuming that the die material has the same thermal capacity (specific heat) as the specimen can be roughly estimated temperature rise in one experiment:
$$\Delta t= 1+\frac{v}{V}\cdot (t_e-t_r)=1+\frac{200\cdot 20 \cdot 1,5}{200\cdot 200\cdot 150}\cdot (800-20) $$
ie less than one degree if I understand well.
This estimate does not account for the heating associated with stamping. :)
 
Well the die material has a bit higher specific heat, but I think the difference is not cruical for the approximate calculation. Correct me if I'm wrong, the result of this equation means, that becuse of cooling down the specimen from 800°C, the die roughly heats up by only 1.78°C in 1 experiment?
 
Thoomy said:
roughly heats up by only 1.78°C in 1 experiment?
Forgive me for haste. The formula had to be:
$$t=\frac{t_r\cdot V + t_e\cdot v}{V+v}$$
and as V>>v:
$$t=t_r+ \frac{t_e\cdot v}{V}=20+0,8=20,8$$
so in the next experiment tr=20,8...
That means $$\Delta t = t - t_r = \frac{t_e\cdot v}{V}=0,8 $$
:)
 
Did not think the difference would be so small :) May I just ask where did you get this equation, since I was searching in a lot of different sources and have never seen so simple solution elsewhere? But thank you for the reply!
 
Thoomy said:
I was searching in a lot of different sources and have never seen so simple solution elsewhere
You have, I sure. You just did not recognize it. The conservation heat energy (balance):
$$c\cdot m\cdot t _m+ c\cdot M\cdot t_M = c\cdot (m+M)\cdot t$$
when two bodies are made of the same material or have equal spesific heats (c). Than assuming the densities are close too we can change the masses by volumes. That is because here it is important the ratio as it is a proportion (the resulting equation for temperature of both bodies t - right side )).
 

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