Boundary-layer height detection with a ceilometer at a coastal ... - Orbit
Boundary-layer height detection with a ceilometer at a coastal ... - Orbit
Boundary-layer height detection with a ceilometer at a coastal ... - Orbit
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4 <strong>Boundary</strong>-<strong>layer</strong> <strong>height</strong> <strong>detection</strong><br />
Traditionally, BLH is derived from d<strong>at</strong>a measured <strong>with</strong> radiosondes. The radiosonde measurements<br />
provide measurements of temper<strong>at</strong>ure, dewpoint and pressure through the lower<br />
troposphere. From these measurements vertical profiles of potential temper<strong>at</strong>ure and w<strong>at</strong>er<br />
vapour mixing r<strong>at</strong>io may be <strong>at</strong>tained. The BLH is associ<strong>at</strong>ed <strong>with</strong> sharp changes in the vertical<br />
profiles and is often identified subjectively from the profiles. Objective BLH <strong>detection</strong> from<br />
radiosonde d<strong>at</strong>a exist as well and are described by Seibert et al. (1998). The BLH estim<strong>at</strong>es<br />
derived from radiosonde d<strong>at</strong>a are limited to the launch time of the radiosondes, which is<br />
typically 2–4 times a day.<br />
In this way remote sensing systems have an advantage in BLH estim<strong>at</strong>ions, as they provide<br />
continuous measurements. Besides lidar measurements, remote sensing is often performed<br />
<strong>with</strong> wind profilers or sodars. The sodar basically may be used to derive the BLH from the<br />
backsc<strong>at</strong>ter of sound waves. The intensity of the backsc<strong>at</strong>ter mainly depends on small-scale<br />
temper<strong>at</strong>ure inhomogeneities, used to derive the BLH.<br />
The wind profiler is similar to the acoustic sodar, <strong>with</strong> the main difference being its use<br />
of electromagnetic waves instead of sound waves and th<strong>at</strong> it apart from temper<strong>at</strong>ure also<br />
measures moisture inhomogeneities (Seibert et al., 1998).<br />
As mentioned, the lidar measurements rely on the aerosol concentr<strong>at</strong>ion in the <strong>at</strong>mosphere.<br />
In the ABL the aerosol concentr<strong>at</strong>ion is high compared to the free <strong>at</strong>mosphere above and this<br />
contrast is the basis for BLH <strong>detection</strong> from lidar measurements (Cohn and Angevine, 2000).<br />
It is often seen th<strong>at</strong> the aerosol content is closely rel<strong>at</strong>ed to the temper<strong>at</strong>ure profile, and the<br />
different methods therefore provide similar BLH estim<strong>at</strong>es. Even so, there may be notable differences<br />
in the thermal structure and the aerosol content as mentioned by Emeis et al. (2004).<br />
This is seen on clear days, near sunset, when a SBL starts to form near the surface, changing<br />
the temper<strong>at</strong>ure profile, while the aerosol content in the residual <strong>layer</strong> is not immedi<strong>at</strong>ely<br />
affected by this form<strong>at</strong>ion. The SBL is therefore generally detected l<strong>at</strong>er during the nighttime<br />
<strong>with</strong> aerosol measurements. Although most BLH <strong>detection</strong> methods focus on mixed <strong>layer</strong> <strong>detection</strong>,<br />
it is also possible to detect the SBL <strong>with</strong> lidars and <strong>ceilometer</strong>s (Martucci et al., 2007).<br />
When looking <strong>at</strong> an aerosol backsc<strong>at</strong>ter profile under ideal cloud free conditions during<br />
daytime, the entrainment zone and the mixed <strong>layer</strong> may clearly be seen. In these situ<strong>at</strong>ions<br />
the BLH may be identified by visual inspection. However, when the amount of backsc<strong>at</strong>ter<br />
d<strong>at</strong>a is large, this method will be time consuming. In th<strong>at</strong> case an autom<strong>at</strong>ed BLH <strong>detection</strong><br />
program will be preferable.<br />
There are numerous ways to detect the BLH from aerosol backsc<strong>at</strong>ter d<strong>at</strong>a, e.g. wavelet<br />
analyses (Davis et al., 1997), variance method (Martucci et al., 2010), the vertical gradient<br />
(Schäfer et al., 2004; Emeis et al., 2008), critical threshold (B<strong>at</strong>chvarova et al., 1999) and<br />
fitting of an ideal profile (Steyn et al., 1999). Three of the methods are presented here.<br />
4.1 The vertical gradient of the aerosol profile<br />
The vertical gradient of the backsc<strong>at</strong>ter profile is calcul<strong>at</strong>ed <strong>with</strong> a central-difference formula<br />
∂β<br />
∂z (z i) ≈ β(z i + ∆z) − β(z i − ∆z)<br />
(23)<br />
2∆z<br />
where β is the backsc<strong>at</strong>ter, z i a reference <strong>height</strong> and ∆z = 20m (from the <strong>ceilometer</strong> settings).<br />
The minimum value of the gradient often indic<strong>at</strong>es the BLH.<br />
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