Proton Collision: Velocity & Direction Calc.

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A proton traveling at 3*10^7 m/s collides elastically with a stationary oxygen nucleus, rebounding at a 90-degree angle. The discussion emphasizes using conservation of momentum and kinetic energy to solve for the velocity and direction of the oxygen nucleus post-collision. The equations derived involve the masses of the proton and oxygen atom, allowing for calculations of the new velocities. The final velocity of the oxygen nucleus can be expressed in terms of the proton's initial velocity and mass ratio. This analytical approach provides a clear method for determining the outcomes of the collision.
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A proton traveling at 3*10^7 m/s collides with the nucleus of a stationary oxygen atom and rebounds in a direction at 90 degree to its original path, calculate the velocity and the direction of the oxygen nucleus assuming the that the collision was perfectly elastic and ignoring relativistic effects .
Mass of proton =1.6*10^-27kg and mass of oxygen atom =2.56*10^-26kg . Thnks to you in advance.
 
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Hi there!
Welcome to the forum...
Surely, you've heard of the conservation of momentum & kinetic energy; Have you tried applying those principles here? It makes for very, easily solving in this case...
Daniel
 


can u pls try it out and explain how
 


Of course,
Look, first we need to solve any such problem analytically, by taking the mass of the proton as m1 and its speed as v1, the oxygen nucleus at m2 and v2 as its velocity after the collison.
Let's assume they were both on the x axes.
Therefore:
\Large p_x = p'_x \Longrightarrow m_1v_1 = m_2v_{2,x}
There's also conservation on the y axes:
Note that since the new velocity of the proton is now at 90 degrees to the original path, it's now traveling on the y axis.
\Large p_y = p'_y \Longrightarrow 0 = m_1v'_1+m_2v_{2,y}
Finally the conservation of kinetic energy:
<br /> \Large<br /> m_1{v_1}^2 = m_1{v&#039;_1}^2+m_2({v_{2,x}}^2+{v_{2,y}}^2).<br />
From the first equation you can extract v_2x, from the second, v_2y, and then find v'_1..
And that's it!
 


Check your answers, to see that you should get
\large<br /> v_2 = \frac{\alpha v_1\sqrt{2}}{\sqrt{1+2\alpha}}, \alpha=\frac{m_1}{m_2};<br />
The direction with the horizontal is given by:
<br /> \tan{\theta} = \frac{v_{2, y}}{v_{2, x}}<br />
Which is easily discovered from the former...
Give it a go!
Daniel
 
thnks a lot that was really helping.
 
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