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import sympy as sm
import numpy as np
import matplotlib.pyplot as plt
sm.init_printing()
print("PROBLEM 1:")
print("part a:")
s, z, t = sm.symbols("s z t")
J, B, RHO, RADIUS, L, RESIST, T = sm.symbols(
"J, B, rho, r, L, R, T", Real=True, Positive=True
)
K_T, K_B = sm.symbols("K_T, K_b")
# loop gain
Loop_Gain = K_T * 1 / (J * s + B)
# transfer function from motor current command to linear displacement (ignoring feedback)
X_over_I = Loop_Gain * RHO / s * RADIUS
sm.pprint(X_over_I)
X_over_I = X_over_I.expand().simplify()
sm.pprint(X_over_I)
print("part b:")
# recall ZOH_eq
# G(z) = (1-z**-1) Z{L**-1{G(s)/s}}
print("Finding inverse laplace of G/s")
G_s = X_over_I
sm.pprint(G_s / s)
g_t = sm.inverse_laplace_transform(G_s / s, s, t)
sm.pprint(g_t.expand())
# make z substitution subs
G_z = (
K_T * T * RADIUS * RHO / B * (z / (z - 1) ** 2)
- J * K_T * RADIUS * RHO / B**2
+ J * K_T * RADIUS * RHO / B**2 * (z / (z - sm.exp(-B / J * T)))
)
sm.pprint(G_z.simplify())
# part c was on the board
print("part c")
F = sm.Matrix([[0, RHO], [0, -B / J]])
G = sm.Matrix([0, K_T / J])
# part d
print("part d")
A = sm.exp(F * T)
B = sm.integrate(A, (T, 0, T))
sm.pprint(F)
sm.pprint(G)
sm.pprint(A)
sm.pprint(B)

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print("Experiment 6.1\n")
measured_activity = 5.2e-6 # curies
elapsed_time = 193.92 # s
sigma_u1 = 35331 # counts
background_time = 193.94 # s
sigma_b = 558 # counts
R = sigma_u1 / elapsed_time - sigma_b / background_time
print(f"R: {R:.3e} counts / s")
print(f"R: {R/3.7e10*1e6:.3e} microcurie")
eps_ip = 0.101 # from figure 6.2
f = 0.6617
d = 100 # mm
r = 38 / 2 # mm
G = r**2 / 4 / d**2
A = R / eps_ip / G / f
print(f"G: {G:.3e}")
print(f"A: {A:.3e} decays / s")
print(f"A: {A/3.7e10*1e6:.3e} microcurie")
A = 4.5 * 3.7e10 / 1e6
eps_ip_est = R / A / G / f
print(f"eps_ips: {eps_ip_est:.3e}")
sigma_u1 = [10122, 11763, 14464, 17476, 22073, 28268, 38084]
sigma_b = 130
d = [100, 90, 80, 70, 60, 50, 40]
t = 60 # s
import numpy as np
n = len(sigma_u1)
R = np.empty(n)
G = np.empty(n)
eps_ip = np.empty(n)
for i, value in enumerate(sigma_u1):
print(i, value)
R[i] = (value - sigma_b) / t
G[i] = r**2 / 4 / d[i] ** 2
eps_ip[i] = R[i] / A / G[i] / f
print("R")
print(R.transpose())
print("G")
print(G.transpose())
print("eps_ip")
print(eps_ip.transpose())
import matplotlib.pyplot as plt
plt.plot(d, eps_ip, ".b")
plt.xlabel("Distance [mm]")
plt.ylabel("$\epsilon_{ip}$")
plt.grid("both")
plt.savefig("exercise6_4.png")
plt.show()