Leo H. O. Hellström
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Research Interests
Leo H. O. Hellström has a total of 18 co-authors. Here are the top co-authors by number of shared publications:
Alexander J. Smits
6 shared publications- Alexander J. Smits
Princeton University
5 shared publications Bharathram Ganapathisubramani
2 shared publicationsAlexander J Smits
Monash University
1 shared publicationAman Sinha
Princeton University Department of Mechanical and Aerospace Engineering Princeton, New Jersey 08544, USA
1 shared publication- Bharathram Ganapathisubramani
University of Southampton
1 shared publication
Latest Publications
- 15 May 2024
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 9 (5)
Eddy self-similarity in turbulent pipe flow
- 15 May 2024
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 9 (5)
Eddy self-similarity in turbulent pipe flow
- 3 April 2023
- Published by Elsevier in Journal of Wind Engineering and Industrial Aerodynamics
- Vol. 237
POD analysis of the structure of vertical axis wind turbine wakes
- 3 April 2023
- Published by Elsevier in Journal of Wind Engineering and Industrial Aerodynamics
- Vol. 237
POD analysis of the structure of vertical axis wind turbine wakes
- 15 October 2020
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 904
Turbulent pipe flow response to a step change in surface roughness
The long-lasting response of turbulent pipe flow to a step change in surface roughness from rough to smooth is examined. Global flow characteristics such as the pressure gradient, skin friction and mean streamwise momentum attain their equilibrium values within approximately 20 radii downstream of the step change, but the turbulent stresses are exceedingly slow to adjust to the new wall condition (), and they first fall below their equilibrium values before seemingly asymptoting to the full recovery state. To help understand this response, we develop a model that captures both the long development length and the second-order response of the turbulence, and we use a scale decomposition to connect the large-scale motions to the response behaviour.
- 15 October 2020
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 904
Turbulent pipe flow response to a step change in surface roughness
The long-lasting response of turbulent pipe flow to a step change in surface roughness from rough to smooth is examined. Global flow characteristics such as the pressure gradient, skin friction and mean streamwise momentum attain their equilibrium values within approximately 20 radii downstream of the step change, but the turbulent stresses are exceedingly slow to adjust to the new wall condition (), and they first fall below their equilibrium values before seemingly asymptoting to the full recovery state. To help understand this response, we develop a model that captures both the long development length and the second-order response of the turbulence, and we use a scale decomposition to connect the large-scale motions to the response behaviour.
- Open Access
- 13 March 2017
- Published by The Royal Society in Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences
- Vol. 375 (2089) , 20160086
Structure identification in pipe flow using proper orthogonal decomposition
The energetic motions in direct numerical simulations of turbulent pipe flow at Re τ =685 are investigated using proper orthogonal decomposition. The procedure is extended such that a pressure component is identified in addition to the three-component velocity field for each mode. The pressure component of the modes is shown to align with the streamwise velocity component associated with the large-scale motions, where positive pressure coincides with positive streamwise velocity, and vice versa. The streamwise evolution of structures is then visualized using a conditional mode, which exhibit a strong similarity to the large-scale, low-momentum motions. A low-pressure region is present in the downstream section of the structure, and a high-pressure region is present in the upstream section. This article is part of the themed issue ‘Toward the development of high-fidelity models of wall turbulence at large Reynolds number’.
- 13 March 2017
- Published by The Royal Society in Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences
- Vol. 375 (2089) , 20160086
Open AccessStructure identification in pipe flow using proper orthogonal decomposition
The energetic motions in direct numerical simulations of turbulent pipe flow at Re τ =685 are investigated using proper orthogonal decomposition. The procedure is extended such that a pressure component is identified in addition to the three-component velocity field for each mode. The pressure component of the modes is shown to align with the streamwise velocity component associated with the large-scale motions, where positive pressure coincides with positive streamwise velocity, and vice versa. The streamwise evolution of structures is then visualized using a conditional mode, which exhibit a strong similarity to the large-scale, low-momentum motions. A low-pressure region is present in the downstream section of the structure, and a high-pressure region is present in the upstream section. This article is part of the themed issue ‘Toward the development of high-fidelity models of wall turbulence at large Reynolds number’.
- Open Access
- 14 June 2016
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 1 (2) , 024403
Coherent structures in transitional pipe flow
Transition to turbulence in pipe flow is investigated experimentally using a temporally resolved dual-plane particle image velocimetry approach, at a Reynolds number of 3440. The flow is analyzed using proper orthogonal decomposition and it is shown that the flow can be divided into two regions: a pseudolaminar region governed by the presence of azimuthally steady traveling waves, and turbulent slugs. The evolution of the structures within the slugs is identified by using the temporally resolved data along with the dual-plane velocity field. These structures are shown to be remarkably similar to the large-scale motions found in fully turbulent flows, with a streamwise and spatiotemporal extent about four pipe radii. The transition between structures is characterized by the detachment and decay of an old structure and the initiation of a new structure at the wall.
- 14 June 2016
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 1 (2) , 024403
Open AccessCoherent structures in transitional pipe flow
Transition to turbulence in pipe flow is investigated experimentally using a temporally resolved dual-plane particle image velocimetry approach, at a Reynolds number of 3440. The flow is analyzed using proper orthogonal decomposition and it is shown that the flow can be divided into two regions: a pseudolaminar region governed by the presence of azimuthally steady traveling waves, and turbulent slugs. The evolution of the structures within the slugs is identified by using the temporally resolved data along with the dual-plane velocity field. These structures are shown to be remarkably similar to the large-scale motions found in fully turbulent flows, with a streamwise and spatiotemporal extent about four pipe radii. The transition between structures is characterized by the detachment and decay of an old structure and the initiation of a new structure at the wall.
- 26 April 2016
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 795, 973-974
The evolution of large-scale motions in turbulent pipe flow – CORRIGENDUM
- 26 April 2016
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 795, 973-974
The evolution of large-scale motions in turbulent pipe flow – CORRIGENDUM
- 2 March 2016
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 792
Self-similarity of the large-scale motions in turbulent pipe flow
Townsend’s attached eddy hypothesis assumes the existence of a set of energetic and geometrically self-similar eddies in the logarithmic layer in wall-bounded turbulent flows, which can be scaled with their distance to the wall. To examine the possible self-similarity of the energetic eddies in fully developed turbulent pipe flow, we performed stereo particle image velocimetry measurements together with a proper orthogonal decomposition analysis. For two Reynolds numbers, $Re_{{\it\tau}}=1330$ and 2460, the resulting modes/eddies were shown to exhibit self-similar behaviour for eddies with wall-normal length scales spanning a decade. This single length scale provides a complete description of the cross-sectional shape of the self-similar eddies.- 2 March 2016
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 792
Self-similarity of the large-scale motions in turbulent pipe flow
Townsend’s attached eddy hypothesis assumes the existence of a set of energetic and geometrically self-similar eddies in the logarithmic layer in wall-bounded turbulent flows, which can be scaled with their distance to the wall. To examine the possible self-similarity of the energetic eddies in fully developed turbulent pipe flow, we performed stereo particle image velocimetry measurements together with a proper orthogonal decomposition analysis. For two Reynolds numbers, $Re_{{\it\tau}}=1330$ and 2460, the resulting modes/eddies were shown to exhibit self-similar behaviour for eddies with wall-normal length scales spanning a decade. This single length scale provides a complete description of the cross-sectional shape of the self-similar eddies.- 19 August 2015
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 779, 701-715
The evolution of large-scale motions in turbulent pipe flow
A dual-plane snapshot proper orthogonal decomposition (POD) analysis of turbulent pipe flow at a Reynolds number of 104 000 is presented. The high-speed particle image velocimetry data were simultaneously acquired in two planes, a cross-stream plane (2D–3C) and a streamwise plane (2D–2C) on the pipe centreline. The cross-stream plane analysis revealed large structures with a spatio-temporal extent of $1{-}2R$ , where $R$ is the pipe radius. The temporal evolution of these large-scale structures is examined using the time-shifted correlation of the cross-stream snapshot POD coefficients, identifying the low-energy intermediate modes responsible for the transition between the large-scale modes. By conditionally averaging based on the occurrence/intensity of a given cross-stream snapshot POD mode, a complex structure consisting of wall-attached and -detached large-scale structures is shown to be associated with the most energetic modes. There is a pseudo-alignment of these large structures, which together create structures with a spatio-temporal extent of approximately $6R$ , which appears to explain the formation of the very-large-scale motions previously observed in pipe flow.- 19 August 2015
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 779, 701-715
The evolution of large-scale motions in turbulent pipe flow
A dual-plane snapshot proper orthogonal decomposition (POD) analysis of turbulent pipe flow at a Reynolds number of 104 000 is presented. The high-speed particle image velocimetry data were simultaneously acquired in two planes, a cross-stream plane (2D–3C) and a streamwise plane (2D–2C) on the pipe centreline. The cross-stream plane analysis revealed large structures with a spatio-temporal extent of $1{-}2R$ , where $R$ is the pipe radius. The temporal evolution of these large-scale structures is examined using the time-shifted correlation of the cross-stream snapshot POD coefficients, identifying the low-energy intermediate modes responsible for the transition between the large-scale modes. By conditionally averaging based on the occurrence/intensity of a given cross-stream snapshot POD mode, a complex structure consisting of wall-attached and -detached large-scale structures is shown to be associated with the most energetic modes. There is a pseudo-alignment of these large structures, which together create structures with a spatio-temporal extent of approximately $6R$ , which appears to explain the formation of the very-large-scale motions previously observed in pipe flow.- 1 December 2014
- Published by AIP Publishing in Physics of Fluids
- Vol. 26 (12) , 125102
The energetic motions in turbulent pipe flow
Snapshot and classical proper orthogonal decomposition (POD) are used to examine the large-scale, energetic motions in fully developed turbulent pipe flow at ReD = 47,000 and 93,000. The snapshot POD modes come in pairs, representing the same azimuthal mode number but with a simple phase shift. The first 10 snapshot POD modes, associated with the very large scale motions (VLSMs), contribute 43% of the average Reynolds shear stress, and for first 80 modes u′ and v′ are anti-correlated so that they all contribute to positive shear stress events. The attached motions are contained in the lower order modes, and detached motions do not appear until snapshot POD mode numbers ≥15. We find that snapshot POD can introduce mode mixing, which is avoided in classical POD. Classical POD also gives frequency information, confirming that the low order modes capture well the behavior of the very large scale motions.
- 1 December 2014
- Published by AIP Publishing in Physics of Fluids
- Vol. 26 (12) , 125102
The energetic motions in turbulent pipe flow
Snapshot and classical proper orthogonal decomposition (POD) are used to examine the large-scale, energetic motions in fully developed turbulent pipe flow at ReD = 47,000 and 93,000. The snapshot POD modes come in pairs, representing the same azimuthal mode number but with a simple phase shift. The first 10 snapshot POD modes, associated with the very large scale motions (VLSMs), contribute 43% of the average Reynolds shear stress, and for first 80 modes u′ and v′ are anti-correlated so that they all contribute to positive shear stress events. The attached motions are contained in the lower order modes, and detached motions do not appear until snapshot POD mode numbers ≥15. We find that snapshot POD can introduce mode mixing, which is avoided in classical POD. Classical POD also gives frequency information, confirming that the low order modes capture well the behavior of the very large scale motions.
- 24 November 2014
- Published by IOP Publishing in Measurement Science and Technology
- Vol. 26 (1)
Errors in parallel-plate and cone-plate rheometer measurements due to sample underfill
- 24 November 2014
- Published by IOP Publishing in Measurement Science and Technology
- Vol. 26 (1)
Errors in parallel-plate and cone-plate rheometer measurements due to sample underfill