How Much Ice Melts When Shot with a Lead Bullet?

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SUMMARY

The discussion focuses on calculating the amount of ice that melts when a lead bullet, weighing 3.00g and traveling at 240 m/s, impacts ice at 30 °C. The correct approach involves using the formula 1/2 m v² + m_b c_b |Δ| T = L_f Δm to determine the energy transfer and subsequent melting of ice. The user incorrectly attempted to calculate the bullet's final temperature after embedding in the ice, resulting in an erroneous melting calculation. The consensus is that the initial method is flawed due to misapplication of thermal energy principles.

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I am trying to find the amount of ice that melts when a lead bullet traveling at 240 m/s at 30 °C. This textbook claims I should use the formula
\dfrac{1}{2} m v^2 + m_{bullet} c_{bullet} \left|\Delta \right| T = L_f \Delta m

What I don't understand is why I shouldn't first calculate how hot the bullet gets after embedding into the ice using
\dfrac{1}{2} m v^2 = mc \left( T_f-30^{\circ}C \right)

Then calculate the amount of ice that melts using:
L \Delta m = -m_{bullet} c_{bullet} \left( T_f - T_i \right)
Where Tf is 0°C and Ti is the Tf after the embedding in the ice.

The data is that the mass of the bullet is 3.00g, so (1/2)mv^2 = mc(Tf-Ti) gives a Tf of 481 deg Celsius, which would cause a change in mass (melting of the ice into water) of .56 g but this is incorrect. Can anyone explain why this method is wrong?
 
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Changing the variable names to be consistent, you have:
\dfrac{1}{2} m_b v^2 = m_bc_b \left( T_h-T_{30}\right)
L \Delta m = -m_b c_b \left( T_f - T_h \right)
Subtracting one from the other gives
\dfrac{1}{2} m_b v^2 - L \Delta m = m_bc_b \left( T_f-T_{30}\right)
Rearranging
\dfrac{1}{2} m_b v^2 - m_bc_b \left( T_f-T_{30}\right) = L \Delta m
For the bullet, \Delta T = T_f-T_{30} < 0, so - m_bc_b \left( T_f-T_{30}\right) = - m_bc_b \Delta T = +m_bc_b |\Delta T|
That gives the equation in the book, so you ought to get the same result either way. If you did not then you must have made a numerical error.
 

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