Calculating Final Temperature of Lead Bullet

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Homework Help Overview

The problem involves calculating the final temperature of a lead bullet after it is stopped in a block of wood, with all its kinetic energy converted into heat. The bullet's initial temperature is given, along with its mass and specific heat capacity. The discussion revolves around the effects of phase transitions and energy calculations related to heating and melting the bullet.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the importance of considering phase transitions and latent heat when calculating temperature changes. There are attempts to clarify the role of mass in energy calculations, and questions arise about the implications of reaching the melting point of lead.

Discussion Status

Participants are actively engaging with the problem, exploring different interpretations of the energy calculations and the effects of melting. Some guidance has been offered regarding unit consistency and the relationship between energy input and temperature changes, particularly at phase transitions.

Contextual Notes

There is an ongoing discussion about the assumptions related to the heat capacity of solid versus molten lead, and whether the energy provided is sufficient to fully melt the bullet. The original poster's calculations and the subsequent responses highlight the complexity of the energy distribution during the heating and melting processes.

leslie123
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Homework Statement


A 5 g lead bullet moving at 343 m/s is stopped in a block of wood. All of the kinetic energy goes into heat energy added to the bullet. The initial temperature of the bullet is 24 degrees C. What is the final temperature of the bullet in degrees C? (cPb = 0.128 kJ/kg . K, LfPb = 24.7 kJ/kg, MPPb = 600 K)

Homework Equations


K = 1/2*m*v^2
Q = mc\DeltaT
Answer = 327C

The Attempt at a Solution


1/2mv^{2}=mc\DeltaT
1/2v^{2} = c\DeltaT

Using this equation \DeltaT = 460C

I realize that the mass must come into it with the other provided information but can not work out how.
 
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When approaching such a problem, one of the most important things to remember is phase transitions. When you heat a substance past its melting point, whatever energy you add to it, goes into melting another portion of the mass (The concept of latent heat is useful in solving such problems, note that it was given to you.)

Another useful thing to remember is to never mix your units, having some data in degrees Celsius, and the rest in kelvins is confusing, move everything to kelvins and see what you can say about what's happening.
 


You said the mass must come into it. But why? In your step 3 you showed that "m" cancels out.
 


Ok, once I started working in the same units (Thanks!) I realized that with a temperature change of 460K, the bullet has easily reached its melting point.

As the bullet starts at 297K it must use 303K worth of heat to reach its melting point.
Using Q=mc\DeltaT plugging in Q = (5*10^-3)(0.128*10^3)(303) we have 194J to heat the bullet up to melting point.

Using Q = mL plugging in Q = (5*10-3)(24.7*10^3) the system needs 124J to fully melt the bullet.

Using Q=mc\DeltaT plugging in Q = (5*10^-3)(0.128*10^3)(460) we have 294J total energy going into the system.

As the bullet will use all of the energy up (194J to heat it up and 100J to melt it) before it is fully melted is this the reason that it stays at 600K (327C)? If the bullet had enough energy to melt it would it continue to heat up?
 


leslie123 said:
Ok, once I started working in the same units (Thanks!) I realized that with a temperature change of 460K, the bullet has easily reached its melting point.

As the bullet starts at 297K it must use 303K worth of heat to reach its melting point.
Using Q=mc\DeltaT plugging in Q = (5*10^-3)(0.128*10^3)(303) we have 194J to heat the bullet up to melting point.

Using Q = mL plugging in Q = (5*10-3)(24.7*10^3) the system needs 124J to fully melt the bullet.

Using Q=mc\DeltaT plugging in Q = (5*10^-3)(0.128*10^3)(460) we have 294J total energy going into the system.

As the bullet will use all of the energy up (194J to heat it up and 100J to melt it) before it is fully melted is this the reason that it stays at 600K (327C)? If the bullet had enough energy to melt it would it continue to heat up?

The question is whether there is enough energy to melt the entire bullet, or not. If there's only enough energy to melt some of the lead, then the system will end up at the melting point of lead, since it can't go over that temperature until all of the lead has melted.

Once the entire bullet has melted, whatever energy you put into it goes into warming it up. I think the assumption you're expected to work under here is that the heat capacity of the molten lead is the same as that of the solid lead, which may not be too realistic, but it's what we've got. :)

Looking it up on the internet I found that the molar specific heat capacity of liquid lead is c=28.6 \frac{J}{mol \cdot K}. Comparing that with the value for solid lead, which is 26.6 \frac{J}{mol \cdot K} justifies our assumption.
 


Awesome, thanks!
 

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