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Module 6

Power plant

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0% found this document useful (0 votes)
39 views44 pages

Module 6

Power plant

Uploaded by

i.goswamiatul25
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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VELLORE INSTITUTE OF TECHNOLOGY CHENNAI CAMPUS

SCHOOL OF MECHANICAL ENGINEERING

BMEE402L
Heat and Mass Transfer
Winter Semester 2023-2024

Dr. Sanjeev Jakhar


Assistant Professor (Sr.), SMEC
Email Id: sanjeev.jakhar@vit.ac.in
BMEE402L Heat and Mass Transfer
Module 6
Wien's displacement law states that the black-body
radiation curve for different temperatures will peak at
different wavelengths that are inversely proportional to the
temperature.
This law states that the monochromatic emissive power of a black
body depends upon absolute temperature of the black body and also
on wavelength of emission.
F12= Fraction of radiation energy leaving surface 1 that reaches surface 2 = 60/100 =0.6

F21= Fraction of radiation energy leaving surface 2 that reach surface 1 =50/100=0.5
1. When the radiation bodies are infinite parallel planes:
2. When the radiation bodies are concentric cylinder or
sphere
3. When a small body in large cavity
Problem 1:- Two very large parallel plates are maintained at uniform temperatures
T1 = 800 K and T2 = 500 K and have emissivities e1 = 0.2 and e2= 0.7, respectively,
as shown in Figure. Determine the net rate of radiation heat transfer between the
two surfaces per unit surface area of the plates
Problem 2:-
Problem 3:-
Problem 4:-
With no radiation shield, the net heat exchange between the parallel
plates

The heat exchange between surface 1-3 and 3-2.


The emissivity of radiation shield is ε3

The shield does not deliver or remove heat


The heat exchange between surface 1-2
Problem 5:-
Problem 6:-
Thank You

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