Shape Factor MCQ Quiz in తెలుగు - Objective Question with Answer for Shape Factor - ముఫ్త్ [PDF] డౌన్‌లోడ్ కరెన్

Last updated on Mar 19, 2025

పొందండి Shape Factor సమాధానాలు మరియు వివరణాత్మక పరిష్కారాలతో బహుళ ఎంపిక ప్రశ్నలు (MCQ క్విజ్). వీటిని ఉచితంగా డౌన్‌లోడ్ చేసుకోండి Shape Factor MCQ క్విజ్ Pdf మరియు బ్యాంకింగ్, SSC, రైల్వే, UPSC, స్టేట్ PSC వంటి మీ రాబోయే పరీక్షల కోసం సిద్ధం చేయండి.

Latest Shape Factor MCQ Objective Questions

Top Shape Factor MCQ Objective Questions

Shape Factor Question 1:

Two concentric spheres having radii 25 mm and 45 mm are placed as shown. Determine the shape factor of the outer sphere with itself.

gate me lt3 Q43

Answer (Detailed Solution Below) 0.65 - 0.75

Shape Factor Question 1 Detailed Solution

Concept:

Shape Factor is defined as the fraction of radiation energy leaving a surface that reaches another surface, for example, F12 means the fraction of energy leaving the surface 1 reaches surface 2.

By Reciprocity theorem: A1F12 = A2F21

By summation rule: F21 + F22 = 1

Calculation:

Given:

1 is the outer surface of the inner sphere and 2 is the inner surface of outer-sphere

gate me lt3 Q43

R1 = 25 mm, R2 = 45 mm

All radiations from surface 1 are absorbed by surface 2. ∴ F12 = 1

By reciprocity Theorem, 

A1F12  = A2F21

\({{F}_{21}}=\frac{{{A}_{1}}}{{{A}_{2}}}={{\left( \frac{{{R}_{1}}}{{{R}_{2}}} \right)}^{2}}={{\left( \frac{25}{45} \right)}^{2}}=\frac{25}{81}\)

By summation rule,

F21 + F22 = 1

∴ F22 = 1 - F21

\(F_{22}= 1- {25\over 81} \)

∴ F22 = 0.69

Shape Factor Question 2:

A body 1 in the form of a sphere of 2 cm radius at temperature T1 is located in body 2, which is a hollow cube of 5 cm side and is at temperature T2 (T2 < T1). The shape factor F21 for radiation heat transfer becomes:

  1. 0.34
  2. 0.43
  3. 0.57
  4. 0.63

Answer (Detailed Solution Below)

Option 1 : 0.34

Shape Factor Question 2 Detailed Solution

Concept:

Shape Factor is defined as the fraction of radiation energy leaving a surface that reaches another surface, for example, F12 means the fraction of energy leaving the surface 1 reaches surface 2.

.Summation Rule: F11 + F12 = 1

Reciprocity theorem: AF12 = AF21 (A is the surface area)

Calculation:

Let 1 denote the sphere and 2 denote the cube

2 M.J Madhu 17.04.20 D 1

Given, radius of the sphere = 2 cm, side of the cube = 5 cm

For sphere F11 = 0, F12 = 1 (All radiations from sphere fall on the cube)

A1 = 4πr2

A2 = 6a2

Reciprocity theorem

A1 F12 = A2 F21   

\({F_{21}} = \frac{{{A_1}}}{{{A_2}}} = \;\frac{{4\pi {2^2}}}{{6\; \times \;{5^2}}} = 0.335\;\;\)

Shape Factor Question 3:

An infinitely long furnace of 0.5 m × 0.4 m cross-section is shown in the figure below. Consider all surfaces of the furnace to be black. The top and bottom walls are maintained at temperature T1 = T3 = 927°C while the side walls are at temperature T2 = T4 = 527°C. The view factor, F1-2 is 0.26.

The net radiation heat loss or gain on side 1 is __________ W/m.

Stefan-Boltzmann constant = 5.67 × 10-8 W/m2-K4

F2 S.S Madhu 19.11.19 D 5

Answer (Detailed Solution Below) 24528 - 24532

Shape Factor Question 3 Detailed Solution

Concept:

For similar object the view factor remains the same i.e. F12 = F14

→ Sum of all view factor for an enclosure = 1

Calculation:

F2 S.S Madhu 19.11.19 D 5..

F12 = F14 = 0.26

F12 + F14 + F13 = 1

0.26 + 0.26 + F13 = 1

F13 = 0.48

Net radiation heat loss or gain on side 1 = Q12 + Q14 + Q13

Q12 = Q14 [∵ Temperature & view factor are same]

∴ QNet,1 = 2Q12 + Q13

\(=\frac{2\sigma \left( T_{1}^{4}-T_{2}^{4} \right)}{\frac{1-{{\epsilon }_{1}}}{{{A}_{1}}{{\epsilon }_{1}}}+\frac{1}{{{A}_{1}}{{F}_{12}}}+\frac{1-{{\epsilon }_{2}}}{{{A}_{2}}{{\epsilon }_{2}}}}+\frac{T\left( T_{1}^{4}-T_{3}^{4} \right)}{\frac{1-{{\epsilon }_{1}}}{{{A}_{1}}{{\epsilon }_{1}}}+\frac{1}{{{A}_{1}}{{F}_{13}}}+\frac{1-{{\epsilon }_{3}}}{{{A}_{3}}{{\epsilon }_{3}}}}\)

∵ T1 = T3 ⇒ Q13 = 0

∵ All surfaces are black surface ⇒ ϵ = 1

∴ Net radiation heat loss or gain on side 1 is

QNet,1 = 2Q12 = 2 σ × A1F12 (T14 – T24)

QNet,1 = 2 × 5.67 × 10-8 × 0.5 × L × 0.26 (12004 - 8004)

Qnet/L = 24530.68 W/m

∵ Temperature of side 1 is greater than side 2

So there will be a loss of 24530.68 W/m of heat from side 1.

Shape Factor Question 4:

For the circular tube of equal length and diameter shown in figure below, the view factor F13 = 0.17. The view factor F21 in this case will be

  1. 0.17
  2. 0.21
  3. 0.79
  4. 0.83

Answer (Detailed Solution Below)

Option 2 : 0.21

Shape Factor Question 4 Detailed Solution

Concept:

Summation Rule: F11 + F12 + F13 = 1

F21 + F22 + F23 = 1

Calculation:

Here flat surface (1) cannot see itself: F11 = 0

∴ F12 + F13 = 1

F12 = 1 - F13 = 1 - 0.17 = 0.83

Reciprocity theorem: A1 F12 = A2 F21

\({F_{21}} = \frac{{{A_1}}}{{{A_2}}} \times {F_{12}} = \frac{{\frac{\pi }{4}{d^2}}}{{\pi dL}} \times {F_{12}} = \frac{{{F_{12}}}}{4} = \frac{{0.83}}{4}\)

F21 = 0.21 (∵ L = D)

Shape Factor Question 5:

The shape factor of a hemispherical body placed on a flat surface with respect to itself is

  1. 0
  2. 0.25
  3. 0.5
  4. 1.0

Answer (Detailed Solution Below)

Option 3 : 0.5

Shape Factor Question 5 Detailed Solution

Concept:

Shape Factor is defined as the fraction of radiation energy leaving a surface that reaches another surface, for example, F12 means the fraction of energy leaving the surface 1 reaches surface 2.

Summation Rule: F11 + F12 = 1

Reciprocity theorem: A1 F12 = A2 F21 (A is the surface area)

Calculation:

Given:

SSC JE ME Full test-10 Images-Q68

Let us denote the hemishpherical body as body 1, and the flat surafce as body 2

From the summation rule F22 + F21 = 1, 

Since no radiation leaving the surface 2 will reach surface 2 again 

∴ F22 = 0, F21 = 1

Now from reciprocity theorem,

A1 F12 = A2 F21

2 x π x r2 x F12 = π x r2 x1

∴ F12 = 0.5,

Now from summation rule F12 + F11 = 1, F11 = 1 - 0.5 = 0.5

Therefore the shape factor of hemispherical body with respect to itself is 0.5.

Shape Factor Question 6:

A cylindrical rod of length ℎ and diameter 𝑑 is placed inside a cubic enclosure of side length 𝐿. 𝑆 denotes the inner surface of the cube. The view-factor FS-S is 

  1. 0
  2. 1
  3. \(\rm \frac{(\pi dh+\pi d^2/2)}{6L^2}\)
  4. \(\rm1-\frac{(\pi dh+\pi d^2/2)}{6L^2}\)

Answer (Detailed Solution Below)

Option 4 : \(\rm1-\frac{(\pi dh+\pi d^2/2)}{6L^2}\)

Shape Factor Question 6 Detailed Solution

Explanation:

 

F2 Madhuri Engineering 08.03.2023 D44

\(\rm A_1=\left(\pi dh+\frac{\pi d^2}{2}\right). A_2=6L^2\)

Summation rule (for surface 1 )

F11 + F12 = 1

F12 = 1 {F11 = 0}

Reciprocity rule (1, 2):

A1F12 = A2F21

A1 = A2F21 {F12 = 1}

\(\rm F_{21}=\frac{A_1}{A_2}\)

Summation rule (for surface 2)

F21 + F22 = 1

F22 or FSS = 1 - F21 = \(\rm 1-\frac{A_1}{A_2}\)

F22 = \(\rm 1-\frac{\left(\pi dh+\frac{\pi d^2}{2}\right)}{6L^2}\)

Shape Factor Question 7:

A solid cylinder (surface 2) is located at the centre of a hollow sphere (surface 1). The diameter of the sphere is 1 m, while the cylinder has a diameter and length of 0.5 m each. The radiation configuration  factor F11 is 

  1. 0.375
  2. 0.625
  3. 0.75
  4. 1

Answer (Detailed Solution Below)

Option 2 : 0.625

Shape Factor Question 7 Detailed Solution

Concept:

For the surface-1:

F11 + F12 = 1

For the surface-2:

\(F_{21} + F_{22} =1\)

From the theorem of reciprocity,

\(A_2F_{21} = A_1F_{12}\)

Calculation:

Given:

d1 (diameter of sphere) = 1 m, d(diameter of cylinder) = 0.5 m, h = d (Height of cylinder) = 0.5 m.

\(A_1 =4\pi r_1^2=4π \frac {d_1 ^2}4= π d_1 ^2\Rightarrow π ~m^2\)

\(A_2 =\pi d_2h_2\;+\;2\frac{\pi}{4}d_2^2= \frac{3}{2}\pi d_2^2\Rightarrow 0.375\pi\;m^2\)

And we know that,

\(F_{21}=1\) (as the surface-1 is convex, all the radiation radiated by surface 1 will be absorbed by surface 2).

From the theorem of reciprocity,

A1F12 = A2F21

∴ π × F12 = 0.375π × F21

∴ F12 = 0.375

Now,

F11 + F12 = 1

F11 + 0.375 = 1

F11 = 0.625.

Shape Factor Question 8:

A hollow enclosure is formed between two infinitely long concentric cylinders of radii 1 m and 2 m, respectively. Radiative heat exchange takes place between the inner surface of the larger cylinder (surface - 2) and the outer surface of the smaller cylinder (surface - 1). The radiating surfaces are diffuse and the medium in the enclosure is non-participating. The fraction of the thermal radiation leaving the larger surface and striking itself is

GATE - 2008 M.E Images Q54

  1. 0.25
  2. 0.5
  3. 0.75
  4. 1

Answer (Detailed Solution Below)

Option 2 : 0.5

Shape Factor Question 8 Detailed Solution

GATE - 2008 M.E Images Q54a

To find F22 = ?

But F11 + F12 = 1

Since F11 = 0, then F12 = 1

Also, from the theorem of reciprocity,  A1 F12 = A2 F21

⇒ (πd1L)F1 =  (πd2L) F21

⇒ 2F12 = 4 F21 (since d1 : d2 = 1 : 2)

⇒ F21 = 0.5F12 = 0.5

Also, F22 + F21 = 1

⇒ F22 = 1 - 0.5 = 0.5

Shape Factor Question 9:

The reciprocity theorem is

  1. ϵ 1 F12 = ϵ 2 F21
  2. A2 F12 = A1 F21
  3. A1 F12 = A2 F21
  4. F12 = F21

Answer (Detailed Solution Below)

Option 3 : A1 F12 = A2 F21

Shape Factor Question 9 Detailed Solution

Concept:

Shape Factor is defined as the fraction of radiation energy leaving a surface that reaches another surface, for example, F12 means the fraction of energy leaving the surface 1 reaches surface 2.

Summation Rule: F11 + F12 = 1

Reciprocity theorem: A1 F12 = A2 F21 (A is the surface area)

Shape Factor Question 10:

What is the shape factor between plates inclined at angle 60˚, having common edge of equal width?

  1. 0.25
  2. 0.50
  3. 0.33
  4. 0.66
  5. 0.75

Answer (Detailed Solution Below)

Option 2 : 0.50

Shape Factor Question 10 Detailed Solution

Concept:

Using reciprocity theorem for triangular duct,

\({F_{12}} = \frac{{{A_1} + {A_2} - {A_3}}}{{2{A_1}}}\)

Calculation:

Imagine a surface (3) of equal width using geometry,

F2 S.C Madhu 27.05.20 D2

\({L_3} = 2L\sin \left( {\frac{\alpha }{2}} \right)\)

\({F_{12}} = \frac{{{A_1} + {A_2} - {A_3}}}{{2{A_1}}} = \frac{{{L_1} + {L_2} - {L_3}}}{{2{L_1}}}\)

\({F_{12}} = 1 - \sin \left( {\frac{\alpha }{2}} \right)\)

∴ F12 = 1 – sin (30)

∴ F12 = 0.50

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