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Electrical Analogy For Thermal Conduction - Practice Questions & MCQ

Edited By admin | Updated on Sep 18, 2023 18:34 AM | #JEE Main

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  • 11 Questions around this concept.

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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 :

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Concepts Covered - 1

Electrical Analogy for Thermal Conduction

 

                                                                       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
 electric current.

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
related with the temperature
difference as$H=\frac{\theta_1-\theta_2}{R}$

where R, is the thermal resistance of
the conductor

4. From the above point the electrical resistance is defined as

$$
R=\frac{\rho l}{A}=\frac{l}{\sigma A}
$$

$\rho=$ Resistivity
where, $\sigma=$ Electrical conductivity

$$
\frac{d q}{d t}=I=\frac{V_1-V_2}{R}=\frac{\sigma A}{l}\left(V_1-V_2\right)
$$
 

4.Similarly from the above point the thermal resistance may be

defined as $R=\frac{l}{K A}$
where $\mathrm{K}=$ Thermal conductivity

$$
\frac{d Q}{d t}=H=\frac{\theta_1-\theta_2}{R}=\frac{K A}{l}\left(\theta_1-\theta_2\right)
$$
 

 

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Electrical Analogy for Thermal Conduction

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