Abstract

AbstractLongitudinal and transverse structure functions, $D_{ll}=\langle {\it\delta}u_{l}{\it\delta}u_{l}\rangle$ and $D_{tt}=\langle {\it\delta}u_{t}{\it\delta}u_{t}\rangle$, can be calculated from aircraft data. Here, ${\it\delta}$ denotes the increment between two points separated by a distance $r$, $u_{l}$ and $u_{t}$ the velocity components parallel and perpendicular to the aircraft track respectively and $\langle \,\rangle$ an average. Assuming statistical axisymmetry and making a Helmholtz decomposition of the horizontal velocity, $\boldsymbol{u}=\boldsymbol{u}_{r}+\boldsymbol{u}_{d}$, where $\boldsymbol{u}_{r}$ is the rotational and $\boldsymbol{u}_{d}$ the divergent component of the velocity, we derive expressions relating the structure functions $D_{rr}=\langle {\it\delta}\boldsymbol{u}_{r}\boldsymbol{\cdot }{\it\delta}\boldsymbol{u}_{r}\rangle$ and $D_{dd}=\langle {\it\delta}\boldsymbol{u}_{d}\boldsymbol{\cdot }{\it\delta}\boldsymbol{u}_{d}\rangle$ to $D_{ll}$ and $D_{tt}$. Corresponding expressions are also derived in spectral space. The decomposition is applied to structure functions calculated from aircraft data. In the lower stratosphere, $D_{rr}$ and $D_{dd}$ both show a nice $r^{2/3}$-dependence for $r\in [2,20]\ \text{km}$. In this range, the ratio between rotational and divergent energy is a little larger than unity, excluding gravity waves as the principal agent behind the observations. In the upper troposphere, $D_{rr}$ and $D_{dd}$ show no clean $r^{2/3}$-dependence, although the overall slope of $D_{dd}$ is close to $2/3$ for $r\in [2,400]\ \text{km}$. The ratio between rotational and divergent energy is approximately three for $r<100\ \text{km}$, excluding gravity waves also in this case. We argue that the possible errors in the decomposition at scales of the order of 10 km are marginal.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call