Created
February 8, 2010 05:11
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My uncompleted calculations for a Thermal Systems lab.
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import csv | |
from libtsl import subset,htparams,sphere | |
from numpy import array, exp | |
from matplotlib.pyplot import * | |
from keas.unit.unit import UnitConverter | |
#Reads in data points | |
datareader=csv.reader(open('friday_aluminum_sphere.csv')) | |
time=[] | |
temp=[] | |
datareader.next() | |
for row in datareader: | |
temp=temp+[float(row[2])] | |
time=time+[15*len(temp)-1] | |
#pulls off front crap | |
istart=temp.index(max(temp)) | |
tempsub=temp[istart:-1] | |
timesub=time[istart:-1] | |
#Subsets data points | |
n=10 | |
timesub=array(subset(timesub,n)) | |
tempsub=array(subset(tempsub,n)) | |
#finds theoretical equation action | |
#units in 'murican | |
#unit converter object | |
c=UnitConverter() | |
#sphere dimensions | |
sphdims=sphere(1.95) | |
sphere=htparams(g=386.22, #thx wiki | |
l=sphdims.d, | |
xsect=sphdims.xsect, | |
sarea=sphdims.sarea, | |
vol=sphdims.vol, | |
Tinf=float(c.convert('tempF('+str(temp[0])+')','tempR')), | |
kvisc=(1.54e-8)*1550.0031, #thx Crowe, et al | |
rho=0.0975436884, #lb/in^3 | |
k=0.0016584693, #thx engineeringtoolbox.com | |
cp=0.229, #thx cengel/boles | |
emmis=0.26) | |
Tzero=float(c.convert('tempF('+str(tempsub[0])+')', 'tempR')) | |
Tfinal=float(c.convert('tempF('+str(tempsub[-1])+')','tempR')) | |
print 'T0=', Tzero | |
print 'Tf=', Tfinal | |
print 'Tinf=', sphere.Tinf | |
print 'Axs=', sphere.xsect | |
print 'Sa=', sphere.sarea | |
print 'V=', sphere.vol | |
Tfilm=sphere.Tfilm(Tzero,Tfinal) | |
print 'film temperature=', Tfilm | |
sphere.thermexp=1.0/Tfilm #approximation for ideal gasses, thx wiki | |
print 'thermal expansion=', sphere.thermexp | |
h=sphere.hc(Tzero,Tfinal) + sphere.hr(Tzero) | |
print 'h=', h | |
beta=(h*sphere.sarea)/(sphere.rho*sphere.vol*sphere.cp) | |
print '1/Tau=', beta | |
theory=(tempsub[0]-temp[0])*exp(-beta*(timesub-timesub[0])) + temp[0] | |
print theory | |
#plot some shizz | |
#plot(timesub,tempsub, 'ko') | |
plot(timesub,theory, 'k-') | |
#axis([0, time[-1],80, 400] ) | |
#show() |
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from math import pi | |
#data manipulations | |
def subset(set,n): | |
sub=[] | |
for i in range(len(set)): | |
if i%n==0: | |
sub=sub+[set[i]] | |
return sub | |
class sphere: | |
def __init__(self,d): | |
self.d=d | |
self.r=d/2.0 | |
self.xsect=pi*self.r**2.0 | |
self.sarea=4.0*self.xsect | |
self.vol=(4.0/3.0)*pi*self.r**3.0 | |
#heat transfer params | |
class htparams: | |
def __init__(self,**args): | |
self.g=args.get('g',9.81) | |
self.l=args.get('l',1.0) | |
self.xsect=args.get('xsect',1.0) | |
self.sarea=args.get('sarea',1.0) | |
self.vol=args.get('vol',1.0) | |
self.Tinf=args.get('Tinf',273.15) | |
self.kvisc=args.get('kvisc',False) | |
self.rho=args.get('rho',False) | |
self.dvisc=args.get('dvisc',False) | |
if(not self.kvisc and self.rho and self.dvisc): | |
self.kvisc=self.dvisc/self.rho | |
if(not self.dvisc and self.rho and self.kvisc): | |
self.dvisc=self.kvisc*self.rho | |
self.k=args.get('k',False) | |
self.cp=args.get('cp',False) | |
self.alpha=args.get('alpha',False) | |
if (not self.alpha and self.rho and self.cp and self.k): | |
self.alpha=self.k/(self.rho*self.cp) | |
self.h=args.get('h',False) | |
self.emiss=args.get('emiss',1.0) | |
self.thermexp=args.get('thermexp',1.0) | |
# def biot(self) | |
# return h*l/k | |
def rayleigh(self,Tf): | |
print 'Ra=', self.grashof(Tf)*self.prandtl(Tf) | |
return self.grashof(Tf)*self.prandtl(Tf) | |
def grashof(self,T): | |
print 'Gr=', self.g * self.thermexp * (T-self.Tinf)*(self.l**3.0)/(self.kvisc**2) | |
return (self.g*self.thermexp*(T-self.Tinf)*self.l**3.0)/(self.kvisc**2) | |
def prandtl(self,T): | |
print 'Pr=', self.kvisc/self.alpha | |
return self.kvisc/self.alpha | |
def reynolds(self): | |
return self.v*self.l/self.kvisc | |
def Tfilm(self,Tzero,Tfinal): | |
return 0.25*(Tzero+Tfinal)+0.5*self.Tinf | |
#specific to metal sphere | |
def hc(self,Tzero,Tfinal): | |
#Incropera and Dewitt's empirical equation for hc | |
#May depend on Englilish units. | |
Tf=self.Tfilm(Tzero,Tfinal) | |
return (self.k/self.l)*((0.589*self.rayleigh(Tf)**0.25)/(1+(0.469/self.prandtl(Tf))**(9.0/16.0))**(4.0/9.0)+2) | |
def hr(self,Tsurf): | |
#Don't forget to use absolute temps! | |
stefboltz=5.6704e-5/1055.0559/1550.0031/1.8 #thx units as well | |
#thx http://en.wikipedia.org/wiki/Stefan%E2%80%93Boltzmann_constant | |
return self.emiss*stefboltz*(Tsurf**4.0-self.Tinf**4.0)/(Tsurf-self.Tinf) |
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