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(v/c)^2 (<br />

1<br />

Proton and Electron Velocity<br />

electrons<br />

“Einstein”<br />

protons<br />

0<br />

0 100 200 300 400 500<br />

Kinetic Energy [MeV]<br />

β2 =(v/c) 2 as function of kinetic<br />

energy T for protons and<br />

electrons. l t<br />

Relativistic (Einstein) relation:<br />

2<br />

T = m 0 0c<br />

(<br />

1<br />

2<br />

1−<br />

v<br />

2<br />

−1<br />

) = m0c<br />

( γ −1<br />

)<br />

2<br />

0 γ<br />

c<br />

Classic (Newton) relation:<br />

2<br />

2<br />

v<br />

2 1 v<br />

T = m0<br />

= m0c<br />

( ) 2<br />

2 2 c<br />

→ Protons (rest energy 938.3 MeV): follow “Newton” mechanics up to some tens of MeV<br />

(Δ (Δv/v / < 1% for f W < 15 MeV) M V) then th slowly l l become b relativistic l ti i ti (“Ei (“Einstein”). t i ”) FFrom th the GGeV V<br />

range velocity is nearly constant (v~0.95c at 2 GeV) → linacs can cope with the<br />

increasing particle velocity, synchrotrons are more efficient for v nearly constant.<br />

→ Electrons (rest energy 511 keV, keV 1/1836 of protons): relativistic from the keV range<br />

(v~0.1c at 2.5 keV) then increasing velocity up to the MeV range (v~0.95c at 1.1 MeV)<br />

→ v~c after few meters of acceleration in a linac (typical gradient 10 MeV/m).<br />

3

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