INTRODUCTION TO NUCLEAR ENGINEERING Homework 2.1

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INTRODUCTION TO NUCLEAR ENGINEERING Homework. Problem: An accelerator increases the total energy of electrons uniformly to 0 GeV over a 3000 m path. That means that at 30 m, 300 m, and 3000 m, the kinetic energy is 0 8, 0 9, and 0 0 ev, respectively. At each of these distances, compute the velocity, relative to light (v/c), and the mass in atomic mass units. Solution: The kinetic energy T is equal to the difference between the total energy (m )and the particle's (i.e., the electron's) rest energy as given by Eq. (.0), T mc - m e. Next, Eq. (.) can be rewritten to determine the velocity v relative to the speed of light c by solving for v/c. Evaluation at 30 m: ET30 0 8 : 0 6 MeV, Total energy of electron at 30 meters c :.9979458 0 8 m/s, Speed of light ET30 c m30 : amu, Mass of electron at 30 m 93.49403 m30 0.074 me : 5.485799 0 4 amu, Rest mass of an electron (Table.5) me v_c30 : dimensionless, Ratio of v/c at 30 meters m30 v_c30 9.999869439 0 Evaluation at 300 m: 0 9 ET300 : 0 6 MeV, Total energy of electron at 300 meters

c :.9979458 0 8 m/s, Speed of light ET300 c m300 : amu, Mass of electron at 300 m 93.49403 m300.0735 me : 5.485799 0 4 amu, Rest mass of an electron (Table.5) me v_c300 : dimensionless, Ratio of v/c at 300 meters m300 v_c300 9.9999986944 0 Evaluation at 3000 m: 0 0 ET3000 : 0 6 MeV, Total energy of electron at 3000 meters c :.9979458 0 8 m/s, Speed of light m3000 : ET3000 c 93.49403 amu, Mass of electron at 3000 m m3000 0.7354 me : 5.485799 0 4 amu, Rest mass of an electron (Table.5) me v_c3000 : dimensionless, Ratio of v/c at 30 m3000 meters

v_c3000 9.9999999869 0 This concludes the problem solution for Homework Problem.! [HW.xmcd]

INTRODUCTION TO NUCLEAR ENGINEERING Homework. Problem: Consider a fast moving particle whose relativistic mass m is 00ε percent greater than its rest mass m o, i.e., m m o (+ε). (a) Show that the particle's speed v, relative to that of light is v/c(-/(+ε )) 0.5 (b) For v/c<<, show that this exact result reduces to v/c is approximately (ε) 0.5 Solution: The solution using Eq. (.) is as follows when we let vvcc v/c: ( ) m mo + ε From the problem definition m.o m Relativistic mass with respect to the rest v mass from Eq. (.) m mo vvc mo ( + ε) mo ( vvc ) vvcc ( ε + ε ) + ε ε + ε ( + ε) ε + ε + ( + ε) ( + ε) ( + ε) vvcc ( + ε)

Now if v/c is very small, then utilizing the result above and the Taylor Series expansion, Eq. (.) becomes: vvcc + ε ( ) ( + ε) ( + ε) ( + ε) ( + ε) ( + ε ) ( + ε) Note that +ε is approximately equal to when v/c is very small! ε vvcc ε This concludes the problem solution for Homework Problem.! [HW.xmcd]

INTRODUCTION TO NUCLEAR ENGINEERING Homework.3 Problem: In fission reactors, one deals with neutrons having kinetic energies as high as 0 MeV. How much error is incurred in computing the speed of 0 MeV neutrons by using the classical expression rather than the relativistic expression for kinetic energy? Solution: We must determine v, the velocity of the neutrons by both classical and relativistic expressions. The solution using Eq. (.0) for the relativistic expression for kinetic energy is as follows: mn :.008664933 amu, Rest mass of neutron T : 0 MeV, Kinetic energy of neutrons Classical Mechanics T m n vclassical T vclassical : (MeV/amu) /, Speed of neutrons in classical mn mechanics approach vclassical 4.459 Relativistic Mechanics T mrel mn mn vrel T mn ( ) + vrel c : 93.49 (MeV/amu) /, Energy-to-mass conversion factor for the speed of light

vrel ( Tmn + T ) c : T + mn (MeV/amu) /, Speed of neutrons in relativistic mechanics approach vrel 4.477 verror vclassical : vrel 00 %error in using classical mechanics approach to calculate neutron velocity verror 0.7965 % This concludes the problem solution for Homework Problem.3! [HW 3.xmcd]

INTRODUCTION TO NUCLEAR ENGINEERING Homework.4 Problem: What speed (m/s) and kinetic energy (MeV) would a neutron have if its relativistic mass were 0% greater than its rest mass? Solution: We will use some of the results from Problem.3 to calculate the relativistic speed and the kinetic energy of the neutron along with Eq. (.0). mn :.008664933 amu, Rest mass of neutron mrel :.0 mn amu, Relativistic mass of neutron c : 93.49 (MeV/amu) /, Energy-to-mass conversion factor for the speed of light Relativistic Mechanics T : mrel mn MeV, Kinetic energy of neutron T 93.956 T mrel mn mn vrel T mn ( ) + vrel vrel ( Tmn + T ) c : T + mn (MeV/amu) /, Speed of neutrons in relativistic mechanics approach (see results from Problem.3) vrel.747

( ).998 0 8 Vrel : vrel m/s, Speed of neutron 93.49 Vrel.490 0 8 It is interesting to note the conversion factor to get from (MeV/amu) / to meters/second. Remember that the equivalent conversion for the square of the speed of light,, is 93.49 MeV/amu. Obviously, then to get the units for c, the square root of 93.49 MeV/amu must be taken and remember that c.998*0 8 meters/second! Always perform a units check to ensure your conversions are executed properly. This concludes the problem solution for Homework Problem.4! [HW 4.xmcd]

INTRODUCTION TO NUCLEAR ENGINEERING Homework.5 Problem: In a Relativistic Heavy Ion Collider, nuclei of gold are accelerated to speeds of 99.95% the speed of light. These nuclei are almost spherical when at rest; however, as they move past the experimenters they appear considerably flattened in the direction of motion because of relativistic effects. Calculate the apparent diameter of such a gold nucleus in its direction of motion relative to that perpendicular to the motion. Solution: Fist we will write down what we know from the problem definition such as v/c and the diameter of a gold nucleus. We will then look at the change in length due to relativistic effects as it may apply to the diameter of the gold nucleus. c :.998 0 8 m/s, Speed of light fac : 0.9995 dimensionless, Ratio of speed of gold nuclei to the speed of light v : fac c m/s, speed of gold nuclei AAu : 96.96655 amu, Atomic weight of gold Ro :.5 0 3 cm, Spherical radius constant (see Eq. (.7)) RAu 3 : Ro AAu cm, Calculated radius of gold nucleus per Eq. (.7) of text Do : RAu cm, Nucleus diameter as it appears when "stationary" Dexp : Do fa cm, Length (or diameter) as it appears to experimenters watching the gold nuclei fly by Dexp 4.599 0 4 This concludes the problem solution for Homework Problem.5! [HW 5.xmcd]