Act like a helpful tutor and exlain me :
Give step-by-step solution with explanation and final answer:
A
2
-
mm
-
thick insulating coating
(
k
=
0
.
1
3
W
/
m
-
K
)
covers a
2
-
mm diameter electrical wire. The thermal contact resistance between them is R
=
6
x
1
0
.
4
m
^
2
-
K
/
W
.
The ambient air is at
2
5
°
C and has a convective heat transfer coefficient of
7
W
/
m
^
2
K
.
If the temperature of the insulation cannot exceed
5
5
°
C
,
what is the maximum electric power that can be dissipated per unit length, in W
/
m
?
Find the corresponding surface temperature of the wire, in
°
C
.
Question:
Act like a helpful tutor and exlain me :
Give step-by-step solution with explanation and final answer:
A
2
-
mm
-
thick insulating coating
(
k
=
0
.
1
3
W
/
m
-
K
)
covers a
2
-
mm diameter electrical wire. The thermal contact resistance between them is R
=
6
x
1
0
.
4
m
^
2
-
K
/
W
.
The ambient air is at
2
5
°
C and has a convective heat transfer coefficient of
7
W
/
m
^
2
K
.
If the temperature of the insulation cannot exceed
5
5
°
C
,
what is the maximum electric power that can be dissipated per unit length, in W
/
m
?
Find the corresponding surface temperature of the wire, in
°
C
.
This is AI generated Response.
Asked by: manish kumar
Created at: 2025-09-24 00:40:41
Final Answer:
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# Step-by-Step Solution
Let's break down the problem:
- **Wire diameter**: \( d_{\text{wire}} = 2\,\text{mm} = 0.002\,\text{m} \)
- **Insulation thickness**: \( t_{\text{ins}} = 2\,\text{mm} = 0.002\,\text{m} \)
- **Thermal conductivity of insulation**: \( k_{\text{ins}} = 0.13\,\text{W/m-K} \)
- **Thermal contact resistance**: \( R_c = 6 \times 10^{-4}\,\text{m}^2\text{-K/W} \)
- **Ambient temperature**: \( T_\infty = 25^\circ\text{C} \)
- **Convective heat transfer coefficient**: \( h = 7\,\text{W/m}^2\text{-K} \)
- **Max insulation surface temp**: \( T_{\text{ins}} \leq 55^\circ\text{C} \)
- **Find**:
1. **Maximum power dissipated per meter** (\( \dot{Q}_{\text{max}} \), W/m)
2. **Corresponding wire surface temperature** (\( T_{\text{wire}} \), in \( ^\circ\text{C} \))
---
## 1. **Thermal Resistances**
### a. **Geometry**
- **Wire radius**: \( r_1 = d_{\text{wire}}/2 = 0.001\,\text{m} \)
- **Outer insulation radius**: \( r_2 = r_1 + t_{\text{ins}} = 0.001 + 0.002 = 0.003\,\text{m} \)
### b. **Thermal Resistance Network**
Heat escapes from the wire core through:
1. **Contact resistance** (\( R_c \)) at the interface (per unit length)
2. **Cylindrical insulation** (\( R_{\text{ins}} \))
3. **Convection** (\( R_{\text{conv}} \)) to air
#### i. **Thermal Contact Resistance** (per length)
\[
R_{c,\,\text{per}\,m} = \frac{R_c}{2\pi r_1}
\]
#### ii. **Insulation (Cylinder) Resistance** (per length)
\[
R_{\text{ins}} = \frac{\ln(r_2/r_1)}{2\pi k_{\text{ins}} L}
\]
For \( L = 1\,\text{m} \).
#### iii. **Convection Resistance** (per length)
\[
R_{\text{conv}} = \frac{1}{2\pi r_2 h L}
\]
For \( L = 1\,\text{m} \).
---
## 2. **Calculate Each Resistance**
### a. **Contact Resistance per meter**
\[
R_{c,\,\text{per}\,m} = \frac{6 \times 10^{-4}}{2\pi \times 0.001} \ \text{K/W}
= \frac{6 \times 10^{-4}}{0.006283} \ \text{K/W}
\approx 0.0955\,\text{K/W}
\]
### b. **Insulation Resistance**
\[
R_{\text{ins}} = \frac{\ln(0.003/0.001)}{2\pi \times 0.13 \times 1}
\]
\[
\ln(3) \approx 1.0986
\]
\[
R_{\text{ins}} = \frac{1.0986}{2\pi \times 0.13}
= \frac{1.0986}{0.8168}
\approx 1.345\,\text{K/W}
\]
### c. **Convection Resistance**
\[
R_{\text{conv}} = \frac{1}{2\pi \times 0.003 \times 7 \times 1}
= \frac{1}{0.131946}
\approx 7.577\,\text{K/W}
\]
---
## 3. **Total Thermal Resistance**
\[
R_{\text{total}} = R_{c} + R_{\text{ins}} + R_{\text{conv}}
= 0.0955 + 1.345 + 7.577
= 9.0175\,\text{K/W}
\]
---
## 4. **Maximum Power Dissipation (\( \dot{Q}_{\text{max}} \))**
The temperature drop from the insulation surface to the air is:
\[
T_{\text{ins}} - T_\infty = \dot{Q} \cdot R_{\text{conv}}
\]
But to find **maximum power**, use **total resistance from insulation surface (max allowed at \( T_{\text{ins}} \)) to air**:
\[
\dot{Q}_{\text{max}} = \frac{T_{\text{ins,\,max}} - T_\infty}{R_{\text{conv}}}
= \frac{55 - 25}{7.577}
= \frac{30}{7.577}
\approx 3.96\,\text{W/m}
\]
But this is **heat transfer from the insulation surface to air**. The same heat must come from the wire, and all resistances matter.
Instead, the correct approach is:
\[
\dot{Q}_{\text{max}} = \frac{T_{\text{ins,\,max}} - T_\infty}{R_{\text{conv}}}
\]
But, as the insulation surface cannot exceed \( 55^\circ\text{C} \), and the wire will be hotter due to the other resistances.
But power generated by the wire is the same as what exits at the insulation surface, so:
\[
\dot{Q}_{\text{max}} = \frac{T_{\text{ins,\,max}} - T_\infty}{R_{\text{conv}}}
= 3.96\,\text{W/m}
\]
---
## 5. **Wire Surface Temperature**
The temperature at the wire surface:
\[
T_{\text{wire}} = T_{\text{ins}} + \dot{Q}_{\text{max}} \times (R_{\text{ins}} + R_c)
\]
\[
= 55 + 3.96 \times (1.345 + 0.0955)
\]
\[
= 55 + 3.96 \times 1.4405
\]
\[
= 55 + 5.705
\]
\[
= 60.7^\circ\text{C}
\]
---
## **Final Answers**
### 1. **Maximum Electric Power Dissipated per Unit Length**
\[
\boxed{3.96\,\text{W/m}}
\]
### 2. **Corresponding Surface Temperature of the Wire**
\[
\boxed{60.7^\circ\text{C}}
\]
---
## **Summary Table**
| Quantity | Value | Units |
|-----------------------------|--------------|------------|
| Maximum power per length | 3.96 | W/m |
| Wire surface temperature | 60.7 | °C |
---
### **Illustration of Heat Transfer Path**
```
[Wire Surface] -- R_c -- [Inner Insulation Surface] -- R_ins -- [Outer Insulation Surface (max 55°C)] -- R_conv -- [Air (25°C)]
```
---
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