A constant electric current flows along a uniform wire with cross-sectional radius ‘R’ and heat conductivity coefficient ‘K’. A unit volume of the wire generates a thermal power ‘W’. Find the temperature distribution across the wire provided the steady-state temperature at the wire surface is equal to T.
temp= T-WR^2/2K(ln[r/R])
ReplyDeleter=radius vector from center
yup same
ReplyDeleteand wrong too.
ReplyDeletebhaiya, any hints then.
ReplyDeleteis it T-W(R^2-r^2)/4K.
ReplyDeletea soln to this, please!
ReplyDeletesambhav,
ReplyDeletemaine dH/dt ko W likha hai and RHS is 2piK(@-T)....
But, what I think shourya has done is write dH/dt as (W/R^2)x^2 and then have done the integral. I couldn't understand the reason that why he has divided the power as function of distance, wont it be the same???
In this problem, H is not a constant, but a function of 'r'. So, you should consider an element of negligible thickness i.e. a thin shell of radius 'r'.
ReplyDeleteAssume the temperature difference across this shell to be dT, and the 'H' to be constant i.e. H(r).
You can write H(r) in terms of dT and dr easily.
But H(r) is quite simple itself, isn't it?? ;)
H(r) he to samajh nhi aaya :P
ReplyDeletei thought that if we consider a thin shell rad(r),
ReplyDeletethen h(r) would depend on the current flowing inside this shell. so h(r) is not constt.
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ReplyDeletethe shell of thickness 'dr' radiates negligible power. 'H' thru the shell is the total power radiated by the spherical volume enclosed by the shell.
ReplyDeletegettin the same as Shourya..
ReplyDeleteT(r) = T-W(R^2-r^2)/4K
plz confirm bhaiya..
thats right.
ReplyDeletebhaiya, please confirm the reason for varying power. Is it that heat is also being generated inside the wire but, as steady state is there so, it must transfer all the heat forward on the surface.
ReplyDelete@Amit: Heat is being generated inside the wire ONLY.. Read the question again yaar..
ReplyDelete