Zhu La

Dr. Zhu La

Tibet University, Lhasa, Tibet, China
orcid

Research Focus & Metrics

Academic Career Length

10Years (2017-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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10 June 2017 in Journal of Geophysical Research: Atmospheres
Verified
Journal Article
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YCYingying Chen
Yingying Chen
KYKun Yang
Kun Yang
JQJun Qin
Jun Qin
QCQian Cui
Qian Cui
Hui LuHui Lu
Hui Lu
WTWenjun Tang
Wenjun Tang

17 January 2017 in Geophysical Research Letters
Verified
Journal Article
Closed access
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YLYanbin Lei
Yanbin Lei
TYTandong Yao
Tandong Yao
KYKun Yang
Kun Yang
YSYongwei Sheng
Yongwei Sheng
MKM. Kleinherenbrink
M. Kleinherenbrink
Guoqing ZhangGuoqing Zhang
Guoqing Zhang

21 March 2019 in Journal of Geophysical Research: Atmospheres
Verified
Journal Article
Open access
PDF file
Anning HuangAnning Huang
Anning Huang
Zhu LaZhu La
Zhu La
JWJunbo Wang
Junbo Wang
YDYongjiu Dai
Yongjiu Dai
KYKun Yang
Kun Yang
SCShuxin Cai
Shuxin Cai
The ability of FLake, WRF‐Lake and CoLM‐Lake models in simulating the thermal features of Lake Nam Co in Central Tibetan Plateau has been evaluated in this study. All the three models with default settings exhibited distinct errors in the simulated vertical temperature profile. Then model calibration was conducted by adjusting three (four) key parameters within FLake and CoLM‐Lake (WRF‐Lake) in a series of sensitive experiments. Results showed that each model's performance is sensitive to the key parameters and becomes much better when adjusting all the key parameters relative to tuning single parameter. Overall, setting the temperature of maximum water density to 1.1 oC instead of 4 oC in the three models consistently leads to improved vertical thermal structure simulation during cold seasons; reducing the light extinction coefficient in FLake results in much deeper mixed layer and warmer thermocline during warm seasons in better agreement with the observation. The vertical thermal structure can be clearly improved by decreasing the light extinction coefficient and increasing the turbulent mixing in WRF‐Lake and CoLM‐Lake during warm seasons. Meanwhile, the modeled water temperature profile in warm seasons can be significantly improved by further replacing the constant surface roughness lengths by a parameterized scheme in WRF‐Lake. Further inter‐comparison indicates that among the three calibrated models, FLake (WRF‐Lake) performs the best to simulate the temporal evolution and intensity of temperature in the layers shallower (deeper) than 10 m, while WRF‐Lake is the best at simulating the amplitude and pattern of the temperature variability at all depths.

21 May 2021 in Geophysical Research Letters
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Journal Article
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LOLin Ouyang
Lin Ouyang
Hui LuHui Lu
Hui Lu
KYKun Yang
Kun Yang
LLLai Yung Ruby Leung
Lai Yung Ruby Leung
Yan WangYan Wang
Yan Wang
XYXiangnan Yao
Xiangnan Yao
Ground observation of precipitation over complex terrain is subject to large uncertainties due to inadequate sampling. This study explores a method that combines limited gauge data and a high‐resolution numerical simulation to quantify the precipitation uncertainties in central Himalaya. Specifically, the Coefficient of spatial Variability (CV) of precipitation and the minimum Number of Required Stations (NRS) to obtain areal‐mean precipitation ground truth values within a 0.25° area are investigated using fine‐scale meteorological simulation at 1.5 km grid spacing. Evaluation over a densely‐gauged area demonstrates comparable CV and NRS values between station observations and simulations. The simulated CV and NRS values in a larger area show a strong and positive dependence on each other and an expected positive (negative) correlation with topographic complexity (temporal scale). The proposed method sheds lights on evaluating precipitation products and holds promise for informing the layout of rain gauge networks in complex terrain.

19 April 2017 in Water Resources Research
Verified
Journal Article
Closed access
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BDBaohong Ding
Baohong Ding
KYKun Yang
Kun Yang
Wei YangWei Yang
Wei Yang
XHXiaobo He
Xiaobo He
YCYingying Chen
Yingying Chen
TYTandong Yao
Tandong Yao

2 March 2020 in Journal of Geophysical Research: Atmospheres
Verified
Journal Article
Open access
PDF file
LOLin Ouyang
Lin Ouyang
KYKun Yang
Kun Yang
Hui LuHui Lu
Hui Lu
YCYingying Chen
Yingying Chen
Zhu LaZhu La
Zhu La
Yan WangYan Wang
Yan Wang
While the Himalayas act as a natural barrier to water vapor transport to the Tibetan Plateau, many north‐south‐oriented valleys channel moisture onto the Plateau. However, owing to the lack of in situ data, the spatiotemporal characteristics of precipitation remain unclear along these valleys. In this study, a high‐altitude (2,800–4,500 m above mean sea level) rain‐gauge network was established in the Yadong Valley, one of the main valleys in the central Himalayan Region (CHR). New observations from this network are used to evaluate the Integrated Multi‐satellitE Retrieval for Global Precipitation Measurement (IMERG) precipitation product, with results demonstrating that the IMERG data can reproduce the seasonal and diurnal patterns of precipitation seen in the observational data. This combination of in situ and IMERG precipitation data reveals two unique characteristics in the CHR. First, precipitation during the premonsoon season (March‐May) contributes 20–40% of the annual total, from the high altitudes of the CHR to Southeast Tibetan Plateau, due to water vapor flux conveyed by southwesterlies from the Bay of Bengal, whereas this percentage is much lower in the northern Himalaya and South Asia. Second, diurnal variations in precipitation during the monsoon season (June‐September) vary between the low and high altitudes of the north‐south‐oriented valleys in the CHR: Precipitation at high altitudes has two peaks (one in the afternoon and the other at night), which is different from the single nighttime peak in low altitudes that is usually reported. These two notable spatiotemporal characteristics are indicative of the unique climate that exists at the high altitudes of the CHR.