Difference between revisions of "Chapter 25 Problem 28"
From 105/106 Lecture Notes by OBM
(Created page with "==Problem== The filament of a light bulb has a resistance of 12 <math>\Omega</math> at 20°C and 140 <math>\Omega</math> when hot. (a) Calculate the temperature of the filam...") |
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<math>R=\rho\frac{l}{A}=\rho_0\frac{4l}{\pi d^2}=\rho_0\left[1+\alpha(T-T_0)\right]\frac{4l_0\left[1+\alpha_T(T-T_0)\right]}{\pi \left(d_0 \left[1+\alpha_T(T-T_0)\right]\right)^2}</math> | <math>R=\rho\frac{l}{A}=\rho_0\frac{4l}{\pi d^2}=\rho_0\left[1+\alpha(T-T_0)\right]\frac{4l_0\left[1+\alpha_T(T-T_0)\right]}{\pi \left(d_0 \left[1+\alpha_T(T-T_0)\right]\right)^2}</math> | ||
+ | <math>=\rho_0\frac{4l_0\left[1+\alpha(T-T_0)\right]}{\pi d_0^2 \left[1+\alpha_T(T-T_0)\right]}</math> | ||
+ | <math>=R_0\frac{\left[1+\alpha(T-T_0)\right]}{\left[1+\alpha_T(T-T_0)\right]}</math> | ||
− | + | <math>\rightarrow R\left[1+\alpha_T(T-T_0)\right]= R_0\left[1+\alpha(T-T_0)\right]</math> | |
− | <math>\ | + | |
+ | <math>T=T_0+\frac{(R-R_0)}{(R_0\alpha-R\alpha_T)}=20^\circ\textrm{C}+\frac{(140-12)\Omega}{(12 \Omega)(0.0045^\circ\textrm{C}^-1)-(140 \Omega )(5.5\times}</math> |
Revision as of 03:12, 25 March 2019
Problem
The filament of a light bulb has a resistance of 12 at 20°C and 140 when hot.
(a) Calculate the temperature of the filament when it is hot, and take into account the change in length and area of the filament due to thermal expansion (assume tungsten for which the thermal expansion coefficient is C° ).
(b) In this temperature range, what is the percentage change in resistance due to thermal expansion, and what is the percentage change in resistance due solely to the change in
use
Solution
(a)
Lower temperature resistance:
(remember we use diameter instead of radius for standard compliance)
at higher temperature ( being the temperature coefficient and being the therma expansion coefficient)