Momentum of flashlight in intergalactic space

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The discussion revolves around calculating the momentum of a flashlight in intergalactic space, focusing on two parts of a physics problem. For part (a), the user applies conservation of linear momentum and Einstein's mass-energy equivalence to derive the change in momentum as Δp = ΔE/c. In part (b), the user initially calculates a high velocity of 44.7 m/s using conservation of mechanical energy but later revises this to v = 3.33 μm by applying conservation of linear momentum, recognizing that the momentum from photons is ΔE/c. The user seeks validation for the revised solution, expressing concerns about the expected low momentum of photons. The conversation highlights the complexities of applying fundamental physics principles to scenarios involving light and momentum.
opticaltempest
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Hello,

I am looking for some help on the following problem:

http://img387.imageshack.us/img387/5481/problemuk7.jpg

I have some questions on part (b)

Here is my solution for (a):

Conservation of linear momentum:

\Delta p = p_f - p_i = m_f v_f - m_i v_i

Solving for mass:

E = mc^2 \Rightarrow m = \frac{E}{{c^2 }}

Substituting mass into conservation of linear momentum:

<br /> \Delta p = \frac{{E_f }}{{c^2 }} \cdot v_f - \frac{{E_i }}{{c^2 }} \cdot v_i <br />

Replace final velocity and initial velocity with c since both velocities are the speed of the photons which are constant speed of light:

\Delta p = \frac{{E_f }}{{c^2 }} \cdot c - \frac{{E_i }}{{c^2 }} \cdot c<br />

Simplify:

\Delta p = \frac{{E_f }}{c} - \frac{{E_i }}{c}

\Delta p = \frac{{\Delta E}}{c}
I think I may have a solution for part (b):

Using the conservation of mechanical energy:

\Delta E_{internal} = \Delta K

1500 = \frac{1}{2}mv^2

1500 = \frac{1}{2}\left( {1.5} \right)v^2

v = \sqrt {\frac{{1500}}{{\left( {0.5} \right)\left( {1.5} \right)}}}

v = 44.7 \mbox{ m/s}

Does that look like a valid solution for part (b)?
 
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Part (b) seems incorrect. Does anyone have any suggestions? The velocity seems high because I would imagine photons possesses little momentum.Here is my new answer for (b):

Using the conservation of linear momentum and the fact that the momentum of the release of photons is equal to <br /> \frac{{\Delta E}}{c}, we have

\frac{{\Delta E}}{c} = mv

\frac{{1500}}{c} = 1.5v

v = \frac{{1500}}{{1.5c}}

v = 3.33 \mbox{\mu m}
 
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