Heat transfer... variable area. ?

physics

1 Answer
Mar 19, 2018

drawn
For the sake of computation let us consider that the the center of the left circular surface as origin # (0,0) # and line perpendicular on it through its center point as #x#-axis. We also consider a very thin disk of radius #r(x)# and thickness #dx# at an arbitrary distance #x# from the origin along X- axis.

Here radius of the thermal resistor decreases with respect to its length at the rate of #=(3R-6R)/(3L)=-R/L#.
Expressing radius of circular cross section as function of #x# as

#r(x)=(6 R-R/Lx)#

And area of cross section as function of #x#

#A(x)=pi(6R-R/Lx)^2# .......(1)

Now let #Q# be the rate of heat transfer in one dimension along the axis considered in the steady state .

So the rate of heat transfer through a slice of infinitesimal thickness #dx# at a distance #x# from origin will be-

#Q=-(A(x)kd theta)/(dx)#
where #d theta# represents decrease in temperature across the slice #dx# considered. Here #k# represents the thermal conductivity of the material of the truncated cone.

So

#Q(dx)/(A(x))=-kd theta#

Using (1) we get

#color(magenta)(Q/pi(dx)/(6R-R/Lx)^2=-kd theta)# ......(2)

To find temperature at a particular value of #x# we need to integrate both sides with respect to respective variables. Before that we make following substitution.

Let #z=6R-R/Lx#

#dz=-R/L dx#

With this substitution (2) becomes

#-(QL)/(Rpi)(dz)/z^2=-kd theta#

#=>(QL)/(Rpi)(dz)/z^2=kd theta# .......(3)

The revised required limits for integration are
For #x=0,z=6R#
for #x=2L,z=4R#
and when #x=3L,z=3R#

Integrating (3) for first set of limits we get

#(QL)/(Rpi)int_(6R)^(4R)(dz)/z^2=kint_100^Td theta#
#=>(-QL)/(Rpi)[1/z]_(6R)^(4R)=k[theta]_100^T#
#=>(-QL)/(Rpi)[1/(4R)-1/(6R)]=k(T-100)#
#=>color(blue)((-QL)/(Rpi)[1/(12R)]=k(T-100))# ........(4)

Similarly for second set of limits we have

#(QL)/(Rpi)int_(4R)^(3R)(dz)/z^2=kint_T^10 d theta#
#=>(-QL)/(Rpi)[1/z]_(4R)^(3R)=k[theta]_T ^10#
#=>(-QL)/(Rpi)[1/(3R)-1/(4R)]=k(10-T)#
#=>color(green)((-QL)/(Rpi)[1/(12R)]=k(10-T))# .......(5)

Observing that LHSs of (4) and (5) are equal. So equating RHSs which must also be equal we get

#k(T-100)=k(10-T)#

#T-100=10-T#

#=>color(red)(T=55^@C)#