Orientation effect on heat transfer of a shrouded LED backlight panel with a plate-fin array

Orientation effect on heat transfer of a shrouded LED backlight panel with a

plate-

fin array

☆

Jin-Cherng Shyu

, Keng-Wei Hsu

, Kai-Shing Yang

, Chi-Chuan Wang

⁎

Department of Mechanical Engineering, National Kaohsiung University of Applied Sciences, Kaohsiung 80778, Taiwan

b_{Green Energy and Environment Research Laboratories, Industrial Technology Research Institute, Hsinchu 31040, Taiwan} c

Department of Mechanical Engineering, National Chiao Tung University, Hsinchu 30010, Taiwan

a b s t r a c t

a r t i c l e i n f o

Available online 31 December 2012 Keywords:

Orientation Clearance Plate-fin Natural convection

This study reports thermal performance of a shrouded 348 mm × 558 mm aluminum plate-fin heat sink sub-ject to various input powers and orientations. Effects of clearance (C) and the orientation on the heat transfer of the heat sink were investigated. Results show that the clearance effect is detectable only in a“window region” between 5 mm and 10 mm where an appreciable rise of heat transfer coefficient is encountered. As the tilted angle (θ) of the LED panel is increased, the heat transfer coefficient is reduced and the clearance effect on heat transfer becomes more pronounced. The heat transfer coefficients are similar between two cases in which the tilted angles of the LED panel are supplementary irrespective of clearance and input power. Except the cases of a horizontal heat sink, heat transfer coefficient of the shrouded heat sink having afin array facing downward is usually slightly higher than that having supplementary tilted angle.

© 2012 Elsevier Ltd. All rights reserved.

1. Introduction

Among numerous effective ways to remove heat from LEDs, pas-sive means employing heat sink is still the most preferable method in the mainstream applications due to its noiseless, reliable, and cost-effective operation. Considerable researches concerning natural convective heat transfer of a plate-fin heat sink with various geomet-ric parameters were carried out [e.g.,1–4]. Some studies concerning the shroud effect on the thermal performance of afin array[5–7] had also been performed. Fujii and Imura[8]proposed correlations for the prediction of Nusselt number of two flat plates based on Reynolds numbers and the Rayleigh numbers at various orientations. Starner and McManus[9]showed that vertical heat sink showed the best thermal performance among all orientations. Because the inter-action between thermal boundary layers develop over the plate-fin array, a vertically-orientated heat sink having larger _{fin spacing} yielded better thermal performance. An investigation[10]on the nat-ural convection heat transfer of a plate-fin heat sink facing downward with a tilted angle ranging from 0° to 30° showed that heat transfer was enhanced with a tilted heat sink due to the removal of stagnation point of the induced airflow passing over the plate-fin array.

The foregoing studies were conducted for uniform heat sources subject to natural convection. However, LED array used in large-size LED TVs is normally enclosed in a slim housing, and the installation

of a LED panel may be subject to inclination due to space constraint or application needs. Therefore, this study aims to experimentally ex-amine both effects of orientation and the clearance between the shroud and thefin tip of the heat sink on the heat transfer of a plate-fin heat sink attached to a LED array.

2. Experimental apparatus and data reduction

The experimental setup consists of a 558 mm × 348 mm MCPCB having 270 evenly distributed 1-W LEDs enclosed by an acrylic hous-ing, a power supply and a power meter to light up LEDs, an aluminum plate-fin array screwed to the backside of the LED panel and an envi-ronmental chamber, as well as a data acquisition unit to record tem-peratures transmitted from thermocouples. More detailed contents concerning the test facility is referred in a previous study[11]. The clearance (C) and the orientation (_{θ) is depicted in}Fig. 1. Since the overall surface efficiency of the present heat sink was about unity, the average heat transfer coefficient, h, was estimated by

q¼ hA Tð s−TaÞ ð1Þ

where A is the total surface area of the heat sink, and Tsand Taare the

average temperature of the seven longitudinal temperatures in the panel and the ambient temperature in the chamber, respectively. The heat generated by those LEDs, q, is estimated as the 75% of the total power input[12], Q, and ranges from 140 W to 230 W. The un-certainty of the present heat transfer coefficients [13]ranges from 1.88% to 2.88%. The experimental conditions of the present study are shown inTable 1.

International Communications in Heat and Mass Transfer 42 (2013) 51–54

☆ Communicated by W.J. Minkowycz.

⁎ Corresponding author at: Department of Mechanical Engineering, National Chiao Tung University, No. 1001, Ta Hsueh Road, Hsinchu 30010, Taiwan.

E-mail address:[email protected](C.-C. Wang).

0735-1933/$– see front matter © 2012 Elsevier Ltd. All rights reserved.

http://dx.doi.org/10.1016/j.icheatmasstransfer.2012.12.006

Contents lists available atSciVerse ScienceDirect

International Communications in Heat and Mass Transfer

60°≤θ≤120° irrespective of the clearance. Another feature is that the heat transfer coefficient is continuously enhanced as the clearance in-creases from 5 mm to the condition without a shroud. Besides,Fig. 4 also shows that the heat transfer coefficient is gradually reduced as the shrouded heat sink becomes horizontal. The lowest heat transfer coef fi-cients among all tilted angles inFig. 4occur when the shroud heat sink is either 0° or 180°. With C=0 mm, the difference in heat transfer coef fi-cient betweenθ=0° and θ=180° is insignificant. Under such conditions, the air induced by the buoyancy force is confined within the acrylic shroud and is not able to diffuse freely into the ambient air. In essence, the heat transfer from the LED backlight panel to ambient air mainly de-pends on the induced airflow passing over the heated acrylic shroud. Once the clearance is increased, the heat transfer coefficient is initially gradually reduced and followed by a monotonous increase with a mini-mal heat transfer coefficient occurring at C=5 mm and at C=15 mm forθ=0° and θ=180°, respectively as shown inFig. 4. In particular, the heat transfer coefficient for both cases has the greatest difference oc-curring without a shroud. This is because the rising air induced by the buoyancy force over a downwardfinned surface is subject to a much larger frictional force than that passing over an upwardfinned surface, as well as the stagnation point of the induced airflow located at the downward facingfinned surface[9], hence leading to a notable differ-ence in heat transfer coefficient.

4. Conclusions

An experimental study investigating the effects of clearance between the shroud and plate-fin tip and the orientation on the thermal perfor-mance of a shrouded heat sink attached to LED backlight panel was performed. Results show that a“window region” exists concerning the effect of shroud. There is virtually negligible influence of shroud clear-ance on the heat transfer coefficient when C is above 15 mm or below 5 mm but an appreciable rise of heat transfer coefficient is encountered when C is increased from 5 mm to 15 mm. Besides, considering that the tilted angle of the LED panel increases, the heat transfer coefficient is reduced and the clearance effect on heat transfer becomes more pro-nounced with the input powers. In general, irrespective of clearance or input power, the heat transfer coef_{ficients would always be similar} between two cases in which the tilted angles of the LED panel are supple-mentary to each other. The heat transfer coefficient of the shrouded heat sink having afin array facing downward is usually slightly higher than that in the other case having supplementary tilted angle. However, a reverse trend occurs when the LED panel is placed horizontally.

Acknowledgment

Thefinancial support of this study from the National Science Council of Taiwan (NSC 101-2221-E-151-024-MY3) is deeply appreciated. Also, the authors are indebted tofinancial support from the Bureau of Energy of the Ministry of Economic Affairs, Taiwan. The last author appreciates a grant from National Science Council of Taiwan (100-2622-E-009-005-CC2).

References

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Power (W)

Average heat transfer coefficient, (W/m

2K)

h

Fig. 2. Effects of clearances (C) on heat transfer coefficient of the present heat sink with an orientation of 120° at various input powers.

Average heat transfer coefficient, (W/m

2K)

h

Fig. 3. Effects of clearances (C) on heat transfer coefficient of the present heat sink with an orientation of 30° at various input powers.

Average heat transfer coefficient, (W/m

2K)

h

Fig. 4. Effect of tilted angle,θ, on heat transfer coefficient subject to clearance with input power of 140 W.

53 J.-C. Shyu et al. / International Communications in Heat and Mass Transfer 42 (2013) 51–54

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