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X_TRISO_RES.py
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#!/usr/bin/env python
#! -*- coding:utf-8 -*-
''' Add the TRISO model and the BP model of MCNP '''
import math
def CentralLocation(r, origin_theta, theta):
x = r * math.cos((origin_theta + theta) * math.pi / 180)
y = r * math.sin((origin_theta + theta) * math.pi / 180)
return x, y
# judge the plates to be positive or negative
def PlatePositive(target_x, target_y, A, B, negative_D):
if A*target_x + B*target_y + negative_D > 0:
return 1
else:
return -1
# write the material card
def MaterialCard(filename):
with open(filename, "w") as f:
f.write("m1 1001 1.0\n");
f.write("m2 8016 1.0\n");
# main function
# diag_radius and the axis_radius are the inner circle
# clad_diag_radius and the clad_axis_radius are the outter circle
def Main(plate_cnt,
R, r,
low, high,
diag_radius, axis_raidus,
clad_diag_radius, clad_axis_radius,
surface_cnt, cell_cnt, original_surface_cnt,
material_type):
# judge the material type first
if material_type == 1: # HCF
universe = 1
particle_universe = 998 # TRISO universe
elif material_type == 2: # posion rod
universe = 4
particle_universe = 996 # BP universe
elif material_type == 3: # graphite rod
material_number = 3
material_density = -2.266
universe = 3
with open("surface.txt", "a") as f_surface, open("cell.txt", "a") as f_cell:
d_theta = 360 / plate_cnt
d_h = (high-low) / plate_cnt
for i in range(plate_cnt):
X1, Y1 = CentralLocation(R, 45, i*d_theta)
X2, Y2 = CentralLocation(R, 135, i*d_theta)
X3, Y3 = CentralLocation(R, 225, i*d_theta)
X4, Y4 = CentralLocation(R, 315, i*d_theta)
x1, y1 = CentralLocation(r, 0, i*d_theta)
x2, y2 = CentralLocation(r, 90, i*d_theta)
x3, y3 = CentralLocation(r, 180, i*d_theta)
x4, y4 = CentralLocation(r, 270, i*d_theta)
print("===================================")
print("X1=%f, Y1=%f" % (X1, Y1))
print("X2=%f, Y2=%f" % (X2, Y2))
print("X3=%f, Y3=%f" % (X3, Y3))
print("X4=%f, Y4=%f" % (X4, Y4))
print("x1=%f, y1=%f" % (x1, y1))
print("x2=%f, y2=%f" % (x2, y2))
print("x3=%f, y3=%f" % (x3, y3))
print("x4=%f, y4=%f" % (x4, y4))
print("===================================")
# get the plate function
theta = i*d_theta
if 0 < theta < 90:
k1 = math.tan((90 + (theta % 90)) * math.pi/180)
A1 = -k1
D1 = -x1 * k1 + y1
k2 = -1 / k1
A2 = -k2
D2 = -x2 * k2 + y2
k3 = k1
A3 = -k3
D3 = -x3 * k3 + y3
k4 = k2
A4 = -k4
D4 = -x4 * k4 + y4
B1 = B2 = B3 = B4 = 1.0
elif 90 < theta < 180:
k4 = math.tan((90 + (theta % 90)) * math.pi/180)
A4 = -k4
D4 = -x4 * k4 + y4
k2 = k4
A2 = -k2
D2 = -x2 * k2 + y2
k3 = -1 / k4
A3 = -k3
D3 = -x3 * k3 + y3
k1 = k3
A1 = -k1
D1 = -x1 * k1 + y1
B1 = B2 = B3 = B4 = 1.0
elif 180 < theta < 270:
k3 = math.tan((90 + (theta % 90)) * math.pi/180)
A3 = -k3
D3 = -x3 * k3 + y3
k1 = k3
A1 = -k1
D1 = -x1 * k1 + y1
k2 = -1 / k3
A2 = -k2
D2 = -x2 * k2 + y2
k4 = k2
A4 = -k4
D4 = -x4 * k4 + y4
B1 = B2 = B3 = B4 = 1.0
elif 270 < theta < 360:
k2 = math.tan((90 + (theta % 90)) * math.pi/180)
A2 = -k2
D2 = -x2 * k2 + y2
k4 = k2
A4 = -k4
D4 = -x4 * k4 + y4
k3 = -1 / k2
A3 = -k3
D3 = -x3 * k3 + y3
k1 = k3
A1 = -k1
D1 = -x1 * k1 + y1
B1 = B2 = B3 = B4 = 1.0
elif theta % 90 == 0:
A1 = 1.0
B1 = 0.0
D1 = R / math.sqrt(2)
A2 = 0.0
B2 = 1.0
D2 = R / math.sqrt(2)
A3 = 1.0
B3 = 0.0
D3 = -R / math.sqrt(2)
A4 = 0.0
B4 = 1.0
D4 = -R / math.sqrt(2)
# if we choose the HCF type, then we write down the surface card,
# the posion rod and the control rod we do not need to write the surface card, only write the cell card is enough.
if material_type == 1:
###############################################################
# SURFACE CARD #
###############################################################
# plate surface
f_surface.write("%d P %f %f %f %f\n" % (surface_cnt, A1, B1, 0.0, D1)) # original_surface_cnt + 0
surface_cnt += 1
f_surface.write("%d P %f %f %f %f\n" % (surface_cnt, A2, B2, 0.0, D2)) # original_surface_cnt + 1
surface_cnt += 1
f_surface.write("%d P %f %f %f %f\n" % (surface_cnt, A3, B3, 0.0, D3)) # original_surface_cnt + 2
surface_cnt += 1
f_surface.write("%d P %f %f %f %f\n" % (surface_cnt, A4, B4, 0.0, D4)) # original_surface_cnt + 3
surface_cnt += 1
f_surface.write("%d PZ %f\n" % (surface_cnt, low + i*d_h)) # original_surface_cnt + 4
surface_cnt += 1
f_surface.write("%d PZ %f\n" %(surface_cnt, low + (i+1)*d_h)) # original_surface_cnt + 5
surface_cnt += 1
# large cylinder which is INSIDE.
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X1, Y1, diag_radius)) # original_surface_cnt + 6
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X2, Y2, diag_radius)) # original_surface_cnt + 7
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X3, Y3, diag_radius)) # original_surface_cnt + 8
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X4, Y4, diag_radius)) # original_surface_cnt + 9
surface_cnt += 1
# litte cylinder which is INSIDE.
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x1, y1, axis_raidus)) # original_surface_cnt + 10
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x2, y2, axis_raidus)) # original_surface_cnt + 11
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x3, y3, axis_raidus)) # original_surface_cnt + 12
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x4, y4, axis_raidus)) # original_surface_cnt + 13
surface_cnt += 1
# large cylinder which is OUTSIDE.
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X1, Y1, clad_diag_radius)) # original_surface_cnt + 14
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X2, Y2, clad_diag_radius)) # original_surface_cnt + 15
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X3, Y3, clad_diag_radius)) # original_surface_cnt + 16
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, X4, Y4, clad_diag_radius)) # original_surface_cnt + 17
surface_cnt += 1
# little cylinder which is OUTSIDE.
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x1, y1, clad_axis_radius)) # original_surface_cnt + 18
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x2, y2, clad_axis_radius)) # original_surface_cnt + 19
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x3, y3, clad_axis_radius)) # original_surface_cnt + 20
surface_cnt += 1
f_surface.write("%d C/Z %f %f %f\n" % (surface_cnt, x4, y4, clad_axis_radius)) # original_surface_cnt + 21
surface_cnt += 1
###############################################################
# CELL CARD #
###############################################################
# judge the type is there any filled particles.
if material_type == 1 or material_type == 2:
string = "%d 0 %d %d %d %d %d -%d & \n" % (cell_cnt,
PlatePositive(0, 0, A1, 1.0, -D1)*(original_surface_cnt+0),
PlatePositive(0, 0, A2, 1.0, -D2)*(original_surface_cnt+1),
PlatePositive(0, 0, A3, 1.0, -D3)*(original_surface_cnt+2),
PlatePositive(0, 0, A4, 1.0, -D4)*(original_surface_cnt+3),
original_surface_cnt+4,
original_surface_cnt+5)
string = string + " (%d %d -%d) (%d %d -%d) & \n (%d %d -%d) (%d %d -%d) & \n" % (
original_surface_cnt+6, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+7, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+8, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+9, original_surface_cnt+4, original_surface_cnt+5)
string = string + " :(-%d %d -%d):(-%d %d -%d): & \n (-%d %d -%d):(-%d %d -%d) u=%d fill=%d imp:n=1\n" % (
original_surface_cnt+10, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+11, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+12, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+13, original_surface_cnt+4, original_surface_cnt+5,
universe,
particle_universe)
# the graphite rod, which not contains the particles.
else:
string = "%d %d %.3f %d %d %d %d %d -%d & \n" % (cell_cnt,
material_number, material_density,
PlatePositive(0, 0, A1, 1.0, -D1)*(original_surface_cnt+0),
PlatePositive(0, 0, A2, 1.0, -D2)*(original_surface_cnt+1),
PlatePositive(0, 0, A3, 1.0, -D3)*(original_surface_cnt+2),
PlatePositive(0, 0, A4, 1.0, -D4)*(original_surface_cnt+3),
original_surface_cnt+4,
original_surface_cnt+5)
string = string + " (%d %d -%d) (%d %d -%d) & \n (%d %d -%d) (%d %d -%d) & \n" % (
original_surface_cnt+6, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+7, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+8, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+9, original_surface_cnt+4, original_surface_cnt+5)
string = string + " :(-%d %d -%d):(-%d %d -%d): & \n (-%d %d -%d):(-%d %d -%d) u=%d imp:n=1\n" % (
original_surface_cnt+10, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+11, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+12, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+13, original_surface_cnt+4, original_surface_cnt+5,
universe)
cell_cnt += 1
''' the HCF cladding model '''
string = string + "%d 3 -2.266 (%d %d %d %d %d -%d & \n" % (cell_cnt,
PlatePositive(0, 0, A1, 1.0, -D1)*(original_surface_cnt+0),
PlatePositive(0, 0, A2, 1.0, -D2)*(original_surface_cnt+1),
PlatePositive(0, 0, A3, 1.0, -D3)*(original_surface_cnt+2),
PlatePositive(0, 0, A4, 1.0, -D4)*(original_surface_cnt+3),
original_surface_cnt+4,
original_surface_cnt+5)
string = string + " (%d %d -%d) (%d %d -%d) & \n (%d %d -%d) (%d %d -%d) & \n" % (
original_surface_cnt+14, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+15, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+16, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+17, original_surface_cnt+4, original_surface_cnt+5)
string = string + " :(-%d %d -%d):(-%d %d -%d): & \n (-%d %d -%d):(-%d %d -%d)) #%d u=%d imp:n=1\n" % (
original_surface_cnt+18, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+19, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+20, original_surface_cnt+4, original_surface_cnt+5,
original_surface_cnt+21, original_surface_cnt+4, original_surface_cnt+5,
cell_cnt-1,
universe)
cell_cnt += 1
string = string + "%d 2 -1.94 -99002 99005 -99007 99004 -99006 99003 & \n %d -%d #%d #%d u=%d imp:n=1\n" % (cell_cnt,
original_surface_cnt+4, original_surface_cnt+5,
cell_cnt-1, cell_cnt-2,
universe)
cell_cnt += 1
# the graphite rod the the posion rod also used to get the original_surface_cnt,
# but we should trace back the first time original_surface_cnt (use record_original_surface_cnt)
# and use the record_origianl_surface_cnt to be the parameter to be used in the next function.
if i == 0:
record_original_surface_cnt = original_surface_cnt
else:
pass
# this command must be under from the record_origianl_surface_cnt.
original_surface_cnt += 22
f_cell.write(string)
return surface_cnt, cell_cnt, original_surface_cnt, record_original_surface_cnt
if __name__ == '__main__':
# TYPE
HCF = 1
posion_rod = 2
graphite_rod = 3
plate_cnt = 8
surface_cnt, cell_cnt, original_surface_cnt = 1, 1, 1
d_height = 80
for i in range(5):
surface_cnt, cell_cnt, original_surface_cnt, record_original_surface_cnt = Main(plate_cnt,
1.2001*math.sqrt(2), 1.2001,
0.05+i*d_height, 0.05+(i+1)*d_height,
0.835, 0.365,
0.755, 0.445,
surface_cnt, cell_cnt, original_surface_cnt,
HCF)
surface_cnt, cell_cnt, original_surface_cnt, record_original_surface_cnt = Main(plate_cnt,
1.2001*math.sqrt(2), 1.2001,
0.05+i*d_height, 0.05+(i+1)*d_height,
0.835, 0.365,
0.755, 0.445,
surface_cnt, cell_cnt, record_original_surface_cnt,
posion_rod)
surface_cnt, cell_cnt, original_surface_cnt, record_original_surface_cnt = Main(plate_cnt,
1.2001*math.sqrt(2), 1.2001,
0.05+i*d_height, 0.05+(i+1)*d_height,
0.835, 0.365,
0.755, 0.445,
surface_cnt, cell_cnt, record_original_surface_cnt,
graphite_rod)
print("Done...\n")