- #36
erobz
Gold Member
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- 1,689
So as a simple physics model applying conservation of energy treating the gas trapped between piston and bb as incompressible and without significant mass:
$$ \frac{1}{2}kx_o^2 = \frac{1}{2}M_{p} v^2 + \frac{1}{2} \frac{1}{3}M_s v^2 + \frac{1}{2}M_{bb} \left( \frac{D_p}{D_{bb}}\right)^4 v^2 $$
Is this in the ballpark upper bound for the velocity of piston as the BB leaves the barrel?
Giving for the BB and upper bound of:
$$ v_{bb} = \left( \frac{D_{p}}{D_b} \right)^4 v \approx 1500~\text{m/s} $$
If its even half that in actuality, I've done some other ballpark calculations that say the back pressure from accelerating the air ahead of the bb out of the barrel could be significant.
$$ \frac{1}{2}kx_o^2 = \frac{1}{2}M_{p} v^2 + \frac{1}{2} \frac{1}{3}M_s v^2 + \frac{1}{2}M_{bb} \left( \frac{D_p}{D_{bb}}\right)^4 v^2 $$
Is this in the ballpark upper bound for the velocity of piston as the BB leaves the barrel?
Giving for the BB and upper bound of:
$$ v_{bb} = \left( \frac{D_{p}}{D_b} \right)^4 v \approx 1500~\text{m/s} $$
If its even half that in actuality, I've done some other ballpark calculations that say the back pressure from accelerating the air ahead of the bb out of the barrel could be significant.
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