def impv_bs(spot, strike, r, d, expiry, price, optiontype):
low = 0.000001
high = 0.3
if (optiontype != "EURO_CALL" and optiontype != "EURO_PUT"):
return "NAN1"
if (optiontype == "EURO_CALL"):
ce = bs_call(spot, strike, r, d, high, expiry)
else:
ce = bs_put(spot, strike, r, d, high, expiry)
while (ce < price):
high *= 2.0
if (high > 1e10):
return "NAN2"
if (optiontype == "EURO_CALL"):
ce = bs_call(spot, strike, r, d, high, expiry)
else:
ce = bs_put(spot, strike, r, d, high, expiry)
if (optiontype == "EURO_CALL"):
return brent(low, high, price, bs_call, None, None, spot, strike, r, d,
expiry, 0, 0)
else:
return brent(low, high, price, bs_put, None, None, spot, strike, r, d,
expiry, 0, 0)
def impv_bi(spot, strike, r, d, expiry, steps, price, optiontype):
low = 0.001
high = 0.3
if (optiontype != "AMER_CALL" and optiontype != "AMER_PUT"):
return "optiontype error"
if (optiontype == "AMER_CALL"):
ce = bi_amer_call(spot, strike, r, d, high, expiry, steps)
else:
ce = bi_amer_put(spot, strike, r, d, high, expiry, steps)
while (ce < price):
high *= 2.0
if (high > 1e10):
return "can't find a high vol"
if (optiontype == "AMER_CALL"):
ce = bi_amer_call(spot, strike, r, d, high, expiry, steps)
else:
ce = bi_amer_put(spot, strike, r, d, high, expiry, steps)
if (optiontype == "AMER_CALL"):
return brent(low, high, price, None, bi_amer_call, None, spot, strike,
r, d, expiry, 0, steps)
else:
return brent(low, high, price, None, bi_amer_put, None, spot, strike,
r, d, expiry, 0, steps)
def eigenvals3(d, c, N):
def f(x): # f(x) = |[A] - x[I]|
p = sturmSeq(d, c, x)
return p[len(p) - 1]
lam = zeros((N), type=Float64)
r = lamRange(d, c, N) # Bracket eigenvalues
for i in range(N): # Solve by Brent's method
lam[i] = brent(f, r[i], r[i + 1])
return lam
def eigenvals3(d,c,N):
def f(x): # f(x) = |[A] - x[I]|
p = sturmSeq(d,c,x)
return p[len(p)-1]
lam = zeros((N),type=Float64)
r = lamRange(d,c,N) # Bracket eigenvalues
for i in range(N): # Solve by Brent's method
lam[i] = brent(f,r[i],r[i+1])
return lam
#!/usr/bin/python
## example4_5
from math import cos
from brent import *
def f(x):
return x * abs(cos(x)) - 1.0
print "root =", brent(f, 0.0, 4.0)
raw_input("Press return to exit")
#!/usr/bin/python
## example4_5
from math import cos
from brent import *
def f(x): return x*abs(cos(x)) - 1.0
print "root =",brent(f,0.0,4.0)
raw_input("Press return to exit")
#!/usr/bin/python
## example8_1
from numarray import zeros,Float64,array
from run_kut4 import *
from brent import *
from printSoln import *
def initCond(u): # Init. values of [y, y’]; use ’u’ if unknown
return array([0.0, u])
def r(u): # Boundary condition residual--see Eq. (8.3)
X,Y = integrate(F,xStart,initCond(u),xStop,h)
y = Y[len(Y) - 1]
r = y[0] - 1.0
return r
def F(x,y): # First-order differential equations
F = zeros((2),type=Float64)
F[0] = y[1]
F[1] = -3.0*y[0]*y[1]
return F
xStart = 0.0 # Start of integration
xStop = 2.0 # End of integration
u1 = 1.0 # 1st trial value of unknown init. cond.
u2 = 2.0 # 2nd trial value of unknown init. cond.
h = 0.1 # Step size
freq = 2 # Printout frequency
u = brent(r,u1,u2) # Compute the correct initial condition
X,Y = integrate(F,xStart,initCond(u),xStop,h)
printSoln(X,Y,freq)
raw_input(’’\nPress return to exit’’)
def initCond(u): # Init. values of [y,y']; use 'u' if unknown
return array([0.0, u])
def r(u): # Boundary condition residual--see Eq. (8.3)
X, Y = integrate(F, xStart, initCond(u), xStop, h)
y = Y[len(Y) - 1]
r = y[0] - 1.0
return r
def F(x, y): # First-order differential equations
F = zeros((2), type=Float64)
F[0] = y[1]
F[1] = -3.0 * y[0] * y[1]
return F
xStart = 0.0 # Start of integration
xStop = 2.0 # End of integration
u1 = 1.0 # 1st trial value of unknown init. cond.
u2 = 2.0 # 2nd trial value of unknown init. cond.
h = 0.1 # Step size
freq = 2 # Printout frequency
u = brent(r, u1, u2) # Compute the correct initial condition
X, Y = integrate(F, xStart, initCond(u), xStop, h)
printSoln(X, Y, freq)
raw_input("\nPress return to exit")
return x * x * x - 2 * x - 10
def g(x):
return (x * 2 + 10) / x / x
# ------------------------------------------------------------
# buscar raices
a, b = rootSearch(f, -10, 10, 0.5, printText=1)
# bisection
print "\nMetodo Bisection"
print bisection(f, a, b, switch=1)
# brent
print "\nMetodo Brent"
print brent(f, a, b, printText=0)
# secant
print "\nMetodo Secant"
print secant(f, a, b, printText=0)
# newton
print "\nMetodo de Newton"
print newton(f, d1f, a, printText=0)
# newton raphson
print "\nMetodo de Newton-Raphson"
print newtonRaphson(f, d1f, a, b, printText=0)
# posicion falsa
print "\nMetodo Posicion Falsa o Falsa Regla"
print falseRule(f, a, b, printText=0)
# punto fijo
print "\nMetodo Punto Fijo"
print fixedPoint(g, a, printText=0)
from bisection import *
from regula_falsi import *
from ridder import *
from brent import *
def f(x):
return x**3 - 10 * x**2 + 5.0
x1 = 0.0
x2 = 1.0
x, err = bisection(f, x1, x2, TOL=1e-10, verbose=True)
print("Final root = %18.10f" % x)
print("True err = %18.10e" % abs(f(x)))
x, err = regula_falsi(f, x1, x2, TOL=1e-10, verbose=True)
print("Final root = %18.10f" % x)
print("True err = %18.10e" % abs(f(x)))
x, err = ridder(f, x1, x2, TOL=1e-10, verbose=True)
print("Final root = %18.10f" % x)
print("True err = %18.10e" % abs(f(x)))
x, err = brent(f, x1, x2, TOL=1e-10, verbose=True)
print("Final root = %18.10f" % x)
print("True err = %18.10e" % abs(f(x)))
