我想让我的代码循环,这样每次执行计算时,它基本上都会对我的变量delta_omega进行累加。即,对于每一次计算,它都会取delta_omega数组中以前的值,将它们相加,然后使用该值再次执行计算,以此类推。我真的不知道该如何进行,因为我也想绘制这些结果。
import numpy as np
import matplotlib.pyplot as plt
delta_omega = np.linspace(-900*10**6, -100*10**6, m) #Hz - range of frequencies
i = 0
while i<len(delta_omega):
delta = delta_omega[i] - (k*v_cap) + (mu_eff*B)/hbar
p_ee = (s0*L/2) / (1 + s0 + (2*delta/L)**2) #population of the excited state
R = L * p_ee # scattering rate
F = hbar*k*(R) #scattering force on atoms
a = F/m_Rb #acceleration assumed constant
vf_slower = (v_cap**2 - (2*a*z0))**0.5 #velocity at the end of the slower
t_d = 1/a * (v_cap - vf_slower) #time taken during slower
# -------- After slower --------
da = 0.1 #(m) distance from end of slower to the middle of the MOT
vf_MOT = (vf_slower**2 - (2*a*da))**0.5 #(m/s) - velocity of the particles at MOT center
t_a = da/vf_MOT #(s) time taken after slower
r0 = 0.01 #MOT capture radius
vr_max = r0/(t_b+t_d+t_a) #maximum transveral velocity
vz_max = (v_cap**2 + 2*a_max*z0)**0.5 #m/s - maximum axial velocity
# -------- Flux of atoms captured --------
P = 10**(4.312-(4040/T)) #vapour pressure for liquid phase (use 4.857 for solid phase)
A = 5*10**-4 #area of the oven aperture
n = P/(k_b*T) #atomic number density
f_oven = ((n*A)/4) * (2/(np.pi)**0.5) * ((2*k_b*T)/m_Rb)**0.5
f = f_oven * (1 - np.exp(-vr_max**2/vp**2))*(1 - np.exp(-vz_max**2/vp**2))
i+=1
plt.plot(delta_omega, f)
一个简单的累积和将定义循环外的变量并添加
i = 0
x = 0
while i < 10:
x = x + 5 #do your work on the cumulative value here
i += 1
print("cumulative sum: {}".format(x))
因此,定义一个包含累积和的变量,每个循环都添加