Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths

The flow distribution across automotive exhaust catalysts has a significant effect on their conversion efficiency. The exhaust gas is pulsating and flow distribution is a function of engine operating condition, namely speed (frequency) and load (flow rate). This study reports on flow measurements ma...

Full description

Saved in:
Bibliographic Details
Main Authors: Mat Yamin, Ahmad Kamal, Benjamin, Stephen, Roberts, Carol A.
Format: Article
Language:English
Published: ELSEVIER 2013
Online Access:http://eprints.utem.edu.my/id/eprint/11147/1/Pulsating_flow_in_a_planar_diffuser_upstream_of_automotive_catalyst_monoliths.pdf
http://eprints.utem.edu.my/id/eprint/11147/
https://www.sciencedirect.com/science/article/abs/pii/S0142727X13000283#!
http://dx.doi.org/10.1016/j.ijheatfluidflow.2013.01.014
Tags: Add Tag
No Tags, Be the first to tag this record!
Institution: Universiti Teknikal Malaysia Melaka
Language: English
id my.utem.eprints.11147
record_format eprints
spelling my.utem.eprints.111472023-08-03T10:15:26Z http://eprints.utem.edu.my/id/eprint/11147/ Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths Mat Yamin, Ahmad Kamal Benjamin, Stephen Roberts, Carol A. The flow distribution across automotive exhaust catalysts has a significant effect on their conversion efficiency. The exhaust gas is pulsating and flow distribution is a function of engine operating condition, namely speed (frequency) and load (flow rate). This study reports on flow measurements made across catalyst monoliths placed downstream of a wide-angled planar diffuser presented with pulsating flow. Cycle-resolved particle image velocimetry (PIV) measurements were made in the diffuser and hot wire anemometry (HWA) downstream of the monoliths. The ratio of pulse period to residence time within the diffuser (defined as the J factor) characterises the flow distribution. During acceleration the flow remained attached to the diffuser walls for some distance before separating near the diffuser inlet later in the cycle. Two cases with J ∼ 3.5 resulted in very similar flow fields with the flow able to reattach downstream of the separation bubbles. With J = 6.8 separation occurred earlier with the flow field resembling, at the time of deceleration, the steady flow field. Increasing J from 3.5 to 6.8 resulted in greater flow maldistribution within the monoliths; steady flow producing the highest maldistribution in all cases for the same Re. ELSEVIER 2013 Article PeerReviewed application/pdf en http://eprints.utem.edu.my/id/eprint/11147/1/Pulsating_flow_in_a_planar_diffuser_upstream_of_automotive_catalyst_monoliths.pdf Mat Yamin, Ahmad Kamal and Benjamin, Stephen and Roberts, Carol A. (2013) Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths. International Journal of Heat and Fluid Flow, 40 (2013). pp. 43-53. ISSN 0142-727X https://www.sciencedirect.com/science/article/abs/pii/S0142727X13000283#! http://dx.doi.org/10.1016/j.ijheatfluidflow.2013.01.014
institution Universiti Teknikal Malaysia Melaka
building UTEM Library
collection Institutional Repository
continent Asia
country Malaysia
content_provider Universiti Teknikal Malaysia Melaka
content_source UTEM Institutional Repository
url_provider http://eprints.utem.edu.my/
language English
description The flow distribution across automotive exhaust catalysts has a significant effect on their conversion efficiency. The exhaust gas is pulsating and flow distribution is a function of engine operating condition, namely speed (frequency) and load (flow rate). This study reports on flow measurements made across catalyst monoliths placed downstream of a wide-angled planar diffuser presented with pulsating flow. Cycle-resolved particle image velocimetry (PIV) measurements were made in the diffuser and hot wire anemometry (HWA) downstream of the monoliths. The ratio of pulse period to residence time within the diffuser (defined as the J factor) characterises the flow distribution. During acceleration the flow remained attached to the diffuser walls for some distance before separating near the diffuser inlet later in the cycle. Two cases with J ∼ 3.5 resulted in very similar flow fields with the flow able to reattach downstream of the separation bubbles. With J = 6.8 separation occurred earlier with the flow field resembling, at the time of deceleration, the steady flow field. Increasing J from 3.5 to 6.8 resulted in greater flow maldistribution within the monoliths; steady flow producing the highest maldistribution in all cases for the same Re.
format Article
author Mat Yamin, Ahmad Kamal
Benjamin, Stephen
Roberts, Carol A.
spellingShingle Mat Yamin, Ahmad Kamal
Benjamin, Stephen
Roberts, Carol A.
Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths
author_facet Mat Yamin, Ahmad Kamal
Benjamin, Stephen
Roberts, Carol A.
author_sort Mat Yamin, Ahmad Kamal
title Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths
title_short Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths
title_full Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths
title_fullStr Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths
title_full_unstemmed Pulsating flow in a planar diffuser upstream of automotive catalyst monoliths
title_sort pulsating flow in a planar diffuser upstream of automotive catalyst monoliths
publisher ELSEVIER
publishDate 2013
url http://eprints.utem.edu.my/id/eprint/11147/1/Pulsating_flow_in_a_planar_diffuser_upstream_of_automotive_catalyst_monoliths.pdf
http://eprints.utem.edu.my/id/eprint/11147/
https://www.sciencedirect.com/science/article/abs/pii/S0142727X13000283#!
http://dx.doi.org/10.1016/j.ijheatfluidflow.2013.01.014
_version_ 1773547659868504064