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11 Questions around this concept.
The temperature $\theta$ at the junction of two insulting sheets, having thermal resistances $R_1$ and $R_2$ as well as top and bottom temperatures $\theta_1$ and $\theta_2$ (as shown in figure) is given by :
Two metallic blocks $\mathrm{M}_1$ and $\mathrm{M}_2$ of same area of cross-section are connected to each other(as shown in figure).If the thermal conductivity of $\mathrm{M}_2$ is K then the thermal conductivity of $\mathrm{M}_1$ will be : [Assume steady state heat conduction]
As per the given figure, two plates $A$ and $B$ of thermal conductivity $
\mathrm{K} \text { and } 2 \mathrm{~K}
$ are joined together to form a compound plate. The thickness of the plates is $
4.0 \mathrm{~cm} \text { and } 2.5 \mathrm{~cm}
$ respectively and the area of the cross-section is $120 \mathrm{~cm}^2$ for each plate. The equivalent thermal conductivity of the compound plate is $\left(1+\frac{5}{\alpha}\right) \mathrm{K}$, then the value of $\alpha$ will be_____________.
If $\mathrm{K}_1$ and $\mathrm{K}_2$ are the thermal conductivities, $\mathrm{L}_1$ and $\mathrm{L}_2$ are the lengths and $\mathrm{A}_1$ and $\mathrm{A}_2$ are the cross sectional areas of steel and copper rods respectively such that $\frac{\mathrm{K}_2}{\mathrm{~K}_1}=9, \frac{\mathrm{~A}_1}{\mathrm{~A}_2}=2, \frac{\mathrm{~L}_1}{\mathrm{~L}_2}=2$. Then, for the arrangement as shown in the figure, the value of temperature T of the steel - copper junction in the steady state will be :
A rod CD of thermal resistance $10.0 \mathrm{KW}^{-1}$ is joined at the middle of an identical rod AB as shown in the figure. The ends $A, B$ and $D$ are maintained at $200^{\circ} \mathrm{C}, 100^{\circ} \mathrm{C}$ and $125^{\circ} \mathrm{C}$ respectively. The heat current in $C D$ is $P$ watt. The value of $P$ is $\qquad$
Heat is transmitted through a glass window of area 1$m^2$ and thickness 0.2cm. If the temperature difference between the two sides is $40^{\circ} \mathrm{C}$ then the calculation of heat current through the glass is [K for glass 0.2cal/m $^{\circ} \mathrm{C}$ s]
Two rod of same length and different material are arrange as shown . At steady state the temperature of middle point is - K1 =300 unit, K2 =200 unit
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Two rod of same material and cross- section are arranged as shown in figure . The temperature at mid point B at steady state is
Two materials having coefficients of thermal conductivity ' $3 K^{\prime}$ and ' $K^{\prime}$ and thickness ' $d$ ' and ' $3 d^{\prime}$, respectively are joined to form a slab as shown in the figure. The temperatures of the outer surfaces are ' $\theta_2^{\prime}$ and ' $\theta_1^{\prime}$ respectively , $\left.\theta_2>\theta_1\right)$.The temperature at the interface is :
Electrical Analogy for Thermal Conduction
Electrical Conduction |
Thermal conduction |
1. Natural flow of electric charge is from higher potential to lower potential |
1. Heat flows from higher temperature to lower temperature |
2. The rate of flow of charge is defined as i.e., $I=\frac{d q}{d t}$ |
2. The rate of flow of heat may is called as heat current. i.e., $H=\frac{d Q}{d t}$ |
3. Ohm's law gives the relation between the electric current and the potential difference $I=\frac{V_1-V_2}{R}$ where, R is the electrical resistance of the conductor |
3. Similarly, the heat current may be where R, is the thermal resistance of |
4. From the above point the electrical resistance is defined as $$ $\rho=$ Resistivity $$ |
4.Similarly from the above point the thermal resistance may be defined as $R=\frac{l}{K A}$ $$ |
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