Difference between revisions of "B-field calculation"

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[[Image:B_field_trajectory.jpg |300px]]
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[[Image:B_field_trajectory2.jpg |300px]]
  
  
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<math>1 MeV = 1.6\cdot 10^{-13} J = 1.6\cdot 10^{-13} \frac{m^2\cdot kg}{s^2}</math>
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<math>c = 2.998 \cdot 10^8 \frac{m}{s}</math>
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<math>\frac{MeV}{C} = 0.534 \cdot 10^{-21} \frac{m\cdot kg}{s}</math>
  
 
<math>p_e = 14 \frac{MeV}{c} = 7.47 \cdot 10^{-21} \frac{m\cdot kg}{s}</math>
 
<math>p_e = 14 \frac{MeV}{c} = 7.47 \cdot 10^{-21} \frac{m\cdot kg}{s}</math>
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<math>B = \frac{p_e}{q_e \cdot R}</math>
 
<math>B = \frac{p_e}{q_e \cdot R}</math>
  
<math>1T=\frac{kg}{C\cdot s}</math>, <math>q_e = 1.6\cdot 10^{-19} C</math>
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<math>1T=\frac{kg}{C\cdot s}</math>, <math>q_e = 1.6\cdot 10^{-19} C</math>, <math>1T=10^{-4}G</math>
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<math>B(T) = \frac{p_e (\frac{MeV}{c})\cdot 0.33\cdot 10^{-2}}{R(m)}</math>
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<math>B(T) = \frac{4.67\cdot 10^{-2}}{R(m)}</math>
 
<math>B(T) = \frac{4.67\cdot 10^{-2}}{R(m)}</math>
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<math>\kappa = \gamma</math>
 
<math>\kappa = \gamma</math>
  
<math>d = R (1 - cos(\kappa))</math>
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<math>R = \frac{a}{cos(\beta)} = \frac{a}{cos(90^0 - \kappa)} = \frac{a}{sin(\kappa)}</math>
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<math>d = R \cdot (1 - cos(\kappa)) = \frac{a \cdot (1 - cos(\kappa))}{sin(\kappa)}</math>
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<math>B(T) = \frac{p_e (\frac{MeV}{c})\cdot 0.33\cdot 10^{-2}\cdot sin(\kappa)}{a(m)}</math> - general expression for B-field.
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<math>B(T) = \frac{4.67\cdot 10^{-2}\cdot sin(\kappa)}{a(m)}</math>
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If <math>\kappa = 2^0</math> then <math>sin(\kappa) = 0.0348995</math> and our B-field becomes:
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<math>B(T) = \frac{0.163\cdot 10^{-2}}{a(m)}</math>
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<math>a \simeq 0.12 m</math> for the coils under consideration. Hence, B-field is:
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<math>B = 0.01358 T = 135.8 G</math>
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[http://wiki.iac.isu.edu/index.php/PhotoFission_with_Polarized_Photons_from_HRRL Go Back]

Latest revision as of 06:17, 5 February 2009

B field trajectory2.jpg


1MeV=1.61013J=1.61013m2kgs2

c=2.998108ms

MeVC=0.5341021mkgs

pe=14MeVc=7.471021mkgs


B=peqeR

1T=kgCs, qe=1.61019C, 1T=104G

B(T)=pe(MeVc)0.33102R(m)


B(T)=4.67102R(m)

1800=κ+900+β

1800=γ+900+β

κ=γ

R=acos(β)=acos(900κ)=asin(κ)

d=R(1cos(κ))=a(1cos(κ))sin(κ)

B(T)=pe(MeVc)0.33102sin(κ)a(m) - general expression for B-field.

B(T)=4.67102sin(κ)a(m)

If κ=20 then sin(κ)=0.0348995 and our B-field becomes:

B(T)=0.163102a(m)

a0.12m for the coils under consideration. Hence, B-field is:

B=0.01358T=135.8G

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