Impact of aerosol hygroscopic growth on the direct aerosol radiative
effect in summer on North China Plain
Y. Kuang
a
, C.S. Zhao
a, *
, J.C. Tao
a
, Y.X. Bian
a
, N. Ma
b
a
Department of Atmospheric and Oceanic Sciences, School of Physics, Peking University, Beijing, China
b
Leibniz Institute for Tropospheric Research, Leipzig, Germany
highlights
High frequency of high RH (>80%) profiles within the mixed layer during daytime.
Aerosol optical properties highly depend on RH profiles due to aerosol water uptake.
Aerosol hygroscopicity contributes to direct aerosol radiative effect significantly.
article info
Article history:
Received 8 April 2016
Received in revised form
3 October 2016
Accepted 7 October 2016
Available online 8 October 2016
Keywords:
Relative humidity profiles
Aerosol optical depth
Single scattering albedo
Asymmetry factor
Aerosol optical properties
abstract
In this paper, relative humidity (RH) profiles and their impacts on the vertical variations of aerosol optical
properties and the direct aerosol radiative effect (DARE) have been investigated based on surface
measurements from the Haze in China campaign and sounding data from the North China Plain. Among
the profiles obtained from July to September in 2008, about half have RHs greater than 80% within the
mixed layer. The vertical variations in the aerosol optical properties at ambient RH, including the
extinction coefficient (s
ext
), single scattering albedo (SSA) and asymmetry factor (g), are remarkably
different from the variations in the dry aerosols and are highly dependent on the RH profiles. Increases of
the aerosol optical depth and column-averaged SSA and g due to aerosol water uptake can reach up to
64%, 0.052 and 0.079, respectively. The fractional contribution to the instantaneous DARE at the top of
the atmosphere due to aerosol hygroscopic growth reaches 60% in high RH profiles. DARE estimates can
be significantly biased if the RH dependence of SSA or g is not considered. We suggest that if their vertical
profiles or column-averaged values are absent, then the ambient values of SSA and g at the surface
should be used rather than the values of SSA and g obtained from dry aerosols when estimating DAREs.
© 2016 Elsevier Ltd. All rights reserved.
1. Introduction
Tropospheric aerosols affect the energy balance on the Earth by
directly scattering and absorbing solar radiation and indirectly
changing the properties and lifespans of clouds (Boucher et al.,
2013). The changes in irradiance due to the interaction of aerosol
and radiation are commonly described in terms of the direct
aerosol radiative effect (DARE), and their estimates remain largely
uncertain (Boucher et al., 2013). These uncertainties are mainly
caused by the high temporal, spatial and compositional variability
of aerosols as well as RH fields and an incomplete understanding of
related, integral aerosol optical properties.
Because many components of aerosol particles are hygroscopic,
the particles can take up water and change in size depending on
their chemical composition and the ambient relative humidity
(RH). Hygroscopic growth becomes particularly important when
the RH is greater than 60% and water often comprises more than
50% of the fine particle mass when the RH exceeds 70e80% (Bian
et al., 2014; McMurry, 2000). Therefore, RH is an important
parameter that governs the optical properties of aerosols and DARE.
Previously, numerous studies have investigated the dependence of
aerosol optical properties on RH by considering the aerosol scat-
tering coefficient (s
sp
)(Zieger et al., 2013), single scattering albedo
(SSA) (Tao et al., 2014; Yoon and Kim, 2006), hemispheric scattering
coefficient (Titos et al., 2014) and asymmetry factor (g)(Yoon and
Kim, 2006). However, these studies were mainly based on surface
measurements and only considered the RH at the surface.
Few studies have investigated the influence of RH profiles on the
* Corresponding author.
E-mail address: zcs@pku.edu.cn (C.S. Zhao).
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Atmospheric Environment
journal homepage: www.elsevier.com/locate/atmosenv
http://dx.doi.org/10.1016/j.atmosenv.2016.10.013
1352-2310/© 2016 Elsevier Ltd. All rights reserved.
Atmospheric Environment 147 (2016) 224e233