How Do Protons and Alpha Particles Behave After an Elastic Collision?

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Collisions between protons and alpha particles are typically elastic, allowing for the application of conservation laws. In this discussion, a proton traveling at 274 km/s collides with a stationary alpha particle, prompting the need to calculate the post-collision velocities. The conservation of momentum and kinetic energy equations are established to solve for the unknown velocities after the collision. The masses of the proton and alpha particle are provided, enabling calculations of momentum and kinetic energy. The discussion emphasizes the importance of using both conservation equations to isolate and solve for the unknowns in the elastic collision scenario.
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Collisions between atomic and subatomic particles are usually perfectly elastic. In one such collision, a proton traveling to the right at 274 km/s collides elastically with a stationary alpha particle (a helium nucleus, having mass 6.65×10−27 kg . I am trying to figure out the velocity of after collision for helium nucleus

Ma=?
Mb=6.65 x10-27kg
Vai= 274000m/s


i started off using the cons. of momentum so i got

Ma(274000m/s)+6.65^-27 kg(0 m/s) = MaVaf + Mb+Vbf

i know I am missing a step here to continue working the problem i just can't figure out where
 
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MaVaf + Mb+Vbf
should be MaVaf + MbVbf, but I presume that is a typo.

Well - one has two unknowns Vaf and Vbf, so one needs two equations.

One is conservation of momentum and the other is conservation of energy.

Now, is one assuming a head on collision without any lateral deflection?

See - http://hyperphysics.phy-astr.gsu.edu/hbase/colsta.html

But look at Rutherford scattering -

http://hyperphysics.phy-astr.gsu.edu/hbase/nuclear/rutsca2.html#c4
http://hyperphysics.phy-astr.gsu.edu/hbase/nuclear/ruthlink.html
 
yes its a head on collision no lateral deflection. so how would you use the conservation of energy to solve for the unknown of the two equations?
 
Kinetic energy before = kinetic energy after, similar to conservation of momentum.

274 km/s = 0.000913c, so non-relativistic mechanics is reasonable.
 
yes so would you then set up 1/2MaVai^2 +1/2MbVbi^2=1/2MaVaf^2+ 1/2MbVbf^2 to get the unknown Mass or velocity?
 
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Yes. One knows the mass of a proton and helium atom (nucleus = alpha particle). Assume the helium atom is stationary, which it should be, otherwise calculate its velocity assuming room temperature.
 
thats where I am stuck on i have both equations set up but i don't see what i have that can be substituted in for each other. i know its somewhere simple

I have 1/2Ma(274000m/s)^2+ 0 = 1/2MaVaf^2 + 1/2 6.65^-27kg Vbf^2

thats for the conservation of KE

you already see what i have for the cons. of momentum up there i just can't see what unknown i have to isolate first to then solve for it
 
Start with what one knows.

Besides the mass of the He nucleus (6.65 E-27 kg), one knows the mass of a proton, which is 1.67 E-27 kg. The proton is moving at 2.74 E5 m/s.

One can compute the momentum (mv) and kinetic energy (1/2mv2) of the proton. The values are 0 for the He nucleus.

Momentum eq: mpvpi= mpvpf + mavaf, where mp is the mass of the proton and ma is the mass of the alpha particle, and i,f subscripts denote initial and final quantities.

Now one could divide the momentum equation by mp and obtain an equation of one unknown velocity in terms of the other, then substitute that into the energy equation.

Energy eq: mpvpi2= mpvpf2 + mavaf2 (the 1/2 factored out)

Similarly, one could divide by mp.

The quantities on the left-hand sides of the momentum and energy equations are known.
 
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