<?xml version="1.0" encoding="utf-8"?><feed xmlns="http://www.w3.org/2005/Atom" ><generator uri="https://jekyllrb.com/" version="3.10.0">Jekyll</generator><link href="https://hingong.github.io/feed.xml" rel="self" type="application/atom+xml" /><link href="https://hingong.github.io/" rel="alternate" type="text/html" /><updated>2026-04-05T22:36:36-07:00</updated><id>https://hingong.github.io/feed.xml</id><title type="html">Hing Ong</title><subtitle>Independent Scholar</subtitle><author><name>Hing Ong</name><email>hing5ong5@gmail.com</email></author><entry><title type="html">My Posters at AGU 2025 Annual Meeting</title><link href="https://hingong.github.io/posts/2025/12/blog-post-6/" rel="alternate" type="text/html" title="My Posters at AGU 2025 Annual Meeting" /><published>2025-12-10T00:00:00-08:00</published><updated>2025-12-10T00:00:00-08:00</updated><id>https://hingong.github.io/posts/2025/12/blog-post-6</id><content type="html" xml:base="https://hingong.github.io/posts/2025/12/blog-post-6/"><![CDATA[<p>Poster 1: <a href="https://HingOng.github.io/files/HingOng_AGU_NCT_ITCZ.pdf">Intertropical Convergence Zone (ITCZ) and the Nontraditional Coriolis Terms (NCTs)</a></p>

<p>The NCTs concentrate tropical precipitation toward the equator in <a href="https://www.cesm.ucar.edu/">CESM3</a> driven by deep-atmosphere <a href="https://www.mmm.ucar.edu/models/mpas">MPAS</a>.</p>

<p>Poster 2: <a href="https://HingOng.github.io/files/HingOng_AGU_MJOscaling.pdf">Scale analysis for the Madden–Julian oscillation (MJO)</a></p>

<p>The time scale of the MJO arises from its length scale.</p>]]></content><author><name>Hing Ong</name><email>hing5ong5@gmail.com</email></author><category term="Poster" /><summary type="html"><![CDATA[Poster 1: Intertropical Convergence Zone (ITCZ) and the Nontraditional Coriolis Terms (NCTs)]]></summary></entry><entry><title type="html">Talk in Tâigí about some basic meteorologic terms</title><link href="https://hingong.github.io/posts/2023/03/blog-post-5/" rel="alternate" type="text/html" title="Talk in Tâigí about some basic meteorologic terms" /><published>2023-03-24T00:00:00-07:00</published><updated>2023-03-24T00:00:00-07:00</updated><id>https://hingong.github.io/posts/2023/03/blog-post-5</id><content type="html" xml:base="https://hingong.github.io/posts/2023/03/blog-post-5/"><![CDATA[<p>I gave an online talk titled “Káng 風 soat 雨 ōe 大氣” (Talk about wind, rain, and atmosphere) in Sè-kài Tâi-oân Bûn-hòa Lūn-tôaⁿ (World Taiwanese Culture Forum) on 12 Nov 2022.</p>

<p><a href="https://HingOng.github.io/files/講風說雨話大氣.pptx">Slides</a></p>

<p>The first 36 minutes of the following video shows my talk</p>

<iframe width="560" height="315" src="https://www.youtube.com/embed/vFWnxO2FNa0" title="YouTube video player" frameborder="0" allow="accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture; web-share" allowfullscreen=""></iframe>]]></content><author><name>Hing Ong</name><email>hing5ong5@gmail.com</email></author><category term="popular science" /><category term="Taiwanese" /><summary type="html"><![CDATA[I gave an online talk titled “Káng 風 soat 雨 ōe 大氣” (Talk about wind, rain, and atmosphere) in Sè-kài Tâi-oân Bûn-hòa Lūn-tôaⁿ (World Taiwanese Culture Forum) on 12 Nov 2022.]]></summary></entry><entry><title type="html">Talk in Tâigí about Atmospheric Rivers</title><link href="https://hingong.github.io/posts/2021/12/blog-post-4/" rel="alternate" type="text/html" title="Talk in Tâigí about Atmospheric Rivers" /><published>2021-12-26T00:00:00-08:00</published><updated>2021-12-26T00:00:00-08:00</updated><id>https://hingong.github.io/posts/2021/12/blog-post-4</id><content type="html" xml:base="https://hingong.github.io/posts/2021/12/blog-post-4/"><![CDATA[<p>I gave a talk in Department of Atmospheric Sciences at National Taiwan University on 16 Dec 2021.
<a href="https://HingOng.github.io/files/大氣河.pdf">Slides</a>
<a href="https://HingOng.github.io/files/20211216台大演講.mp3">Audio Record</a></p>]]></content><author><name>Hing Ong</name><email>hing5ong5@gmail.com</email></author><category term="research" /><category term="Taiwanese" /><summary type="html"><![CDATA[I gave a talk in Department of Atmospheric Sciences at National Taiwan University on 16 Dec 2021. Slides Audio Record]]></summary></entry><entry><title type="html">Comments on Hitchman and Rowe’s Reply</title><link href="https://hingong.github.io/posts/2020/11/blog-post-2/" rel="alternate" type="text/html" title="Comments on Hitchman and Rowe’s Reply" /><published>2020-11-19T00:00:00-08:00</published><updated>2020-11-19T00:00:00-08:00</updated><id>https://hingong.github.io/posts/2020/11/blog-post-2</id><content type="html" xml:base="https://hingong.github.io/posts/2020/11/blog-post-2/"><![CDATA[<p>The comment-reply correspondence between <a href="https://doi.org/10.1175/MWR-D-20-0300.1">Hitchman &amp; Rowe</a> and <a href="https://hingong.github.io/publication/2020-11-19-paper-title-number-5">me</a> has been published. We did not reach plenary agreement as their reply was published in the original form without accounting for my comments on their reply during the correspondence. The following is a record of my comments.</p>

<h1 id="recommendation">Recommendation</h1>

<p>Minor Revision</p>

<h1 id="summary">Summary</h1>

<p>I thank the authors for the thoughtful reply, with which I am mostly satisfied. I recommend minor revisions to ask the authors to give another consideration to the following four points.</p>

<h1 id="minor-comments">Minor comments</h1>
<ol>
  <li>“We agree with his interpretation, except for mis-characterizing our canoe paddle analogy as a “flaw”.” This reads like attacking a straw man because my comment paper does not explicitly mention the canoe paddle analogy. Whether the analogy is helpful for qualitative explanation is subject to personal opinion (see the next point), so I prefer not to discuss that in my comment paper. However, using the analogy for budget analysis like in section 8 of HR2019 results in double counting, and my comment paper argues that a double-counting budget analysis is flawed.</li>
  <li>Please consider replying to the proposed remedy. I believe the proposed remedy is more analogous to a canoe paddle. I agree that the convective momentum transport is like a canoe paddle impinging on the interface. However, I feel ill to relate the canoe paddle to a term usually associated with turbulence. The proposed remedy associates the convective momentum transport to the product of diabatic forcing and vertical shear. To me, the vertical shear is analogous to the velocity difference between paddle motion and water flow, and the diabatic forcing is analogous to the paddle impingement on the interface. These ingredients together (take the product) yield the PV dipole.</li>
  <li>“PV anomalies that are advected upward… in agreement with Ong’s (2020) interpretation.” This reads like misinterpretation. In my proposed remedy, cross-isentropic (vertical) advection of momentum yields along-isentropic (horizontal) non-advective flux of PV. My comment paper does not mention any advection or flux of PV that is vertical.</li>
  <li>“In considering his Fig. 1b… an array of values in altitude.” These statements may be acceptable because the authors have stated that they “calculate the vertical component of PV based on relative vorticity at constant height.” However, I would like to remind the authors that the complete PV can be calculated in altitude coordinates. PV is defined as the dot product of absolute vorticity and theta gradient divided by density, so the complete PV equals to the vertical component plus the horizontal component, i.e., horizonal absolute vorticity dotting horizontal theta gradient. In my Figure 1b, there is indeed a nonzero vertical component of PV, but it is offset by the horizontal component of PV, leaving the complete PV zero. People prefer PV analysis in isentropic coordinates, where PV only has a vertical component.</li>
</ol>]]></content><author><name>Hing Ong</name><email>hing5ong5@gmail.com</email></author><category term="research" /><summary type="html"><![CDATA[The comment-reply correspondence between Hitchman &amp; Rowe and me has been published. We did not reach plenary agreement as their reply was published in the original form without accounting for my comments on their reply during the correspondence. The following is a record of my comments.]]></summary></entry><entry><title type="html">The Role of Diabatic Vorticity Tilting in PV Distribution in the Outflow Layer of Hurricane Epsilon (2020)</title><link href="https://hingong.github.io/posts/2020/11/blog-post-3/" rel="alternate" type="text/html" title="The Role of Diabatic Vorticity Tilting in PV Distribution in the Outflow Layer of Hurricane Epsilon (2020)" /><published>2020-11-19T00:00:00-08:00</published><updated>2020-11-19T00:00:00-08:00</updated><id>https://hingong.github.io/posts/2020/11/blog-post-3</id><content type="html" xml:base="https://hingong.github.io/posts/2020/11/blog-post-3/"><![CDATA[<p><img src="/images/BlogPost3_1.PNG" /></p>

<p>This post explains why diabatic vorticity tilting plays an essential role in the distribution of potential vorticity (PV) in the outflow layer of the hurricane. In the zonal vertical cross section through the center of Hurricane Epsilon (2020) above, I highlight the region from the center to 300 km toward the east between 345 K and 350 K isentropes. Why is PV near the center so strongly cyclonic (&gt; 2 PVU)? Why is PV on the skirt anticyclonic (&lt; 0 PVU)?</p>

<p>For the strongly cyclonic PV near the center, vertical advection of PV seems an appealing explanation. Indeed, it is positive owing to the upward motion and the vertically decreasing PV. However, such advection cannot conserve PV because it is cross-isentropic (i.e., diabatic), and diabatic vorticity squeezing due to vertically decreasing heating rate is a negative effect here. Nonetheless, diabatic vorticity tilting is positive here. These contributors of different signs complicate the qualitative PV analysis. Fortunately, <a href="https://doi.org/10.1175/1520-0469(1990)047&lt;2021:OTCAIT&gt;2.0.CO;2">Haynes and McIntyre (1990)</a> gave insight to eliminate some contributors. They proved that the net effect of all cross-isentropic PV density fluxes is displacement of the isentropes (scientific statements cannot be proved, but this is a provable mathematical consequence of how PV is defined). Hence, cross-isentropic PV density fluxes are dynamically insignificant because they offset one another leaving no net flux through the isentropes.</p>

<p>Focusing on small <a href="https://en.wikipedia.org/wiki/Rossby_number">Rossby number</a>, <a href="https://doi.org/10.1175/1520-0469(1990)047&lt;2021:OTCAIT&gt;2.0.CO;2">Haynes and McIntyre (1990)</a> explained that diabatic heating changes PV through concentration and dilution. While PV density cannot permeate an isentropic level, diabatic heating transports mass from a lower isentropic layer to higher, concentrating the PV below the heating maximum and diluting above. In terms of PV density flux, the dilution and concentration are associated with divergence and convergence of advective flux along the isentropes. This conceptual model predicts that PV in the outflow layer of a hurricane should be diluted and thus anomalously weak and still cyclonic. However, this is not observed.</p>

<p>My paper (<a href="https://hingong.github.io/publication/2020-11-19-paper-title-number-5">Ong 2020</a>) gives a proper conceptual model considering the diabatic flux along the isentropes derived by <a href="https://doi.org/10.1175/1520-0469(1990)047&lt;2021:OTCAIT&gt;2.0.CO;2">Haynes and McIntyre (1990)</a> but ignored for small <a href="https://en.wikipedia.org/wiki/Rossby_number">Rossby number</a>. In short, diabatic heating transports momentum from a lower isentropic layer to higher, which yields a PV density flux opposing the along-isentropic vorticity vector. To illustrate, I annotate the cross section as below. With respect to the hurricane center, given the radially outward vorticity, diabatic heating fluxes PV radially inward, which explains both the strongly cyclonic PV near the center and the anticyclonic PV on the skirt. As explained in <a href="https://hingong.github.io/publication/2020-11-19-paper-title-number-5">Ong 2020</a>, the diabatic flux along the isentropes is equivalent to diabatic tilting of vorticity from along-isentropic to cross-isentropic. Therefore, the diabatic tilting is essential for creating the radially inward PV gradient in the outflow layer of the hurricane. This may explain the symmetric instability (i.e., anticyclonic PV) in the outflow layer of Hurricane Ivan (2004) found by <a href="https://doi.org/10.1175/JAS-D-14-0117.1">Molinari and Vollaro (2014)</a>.</p>

<p><img src="/images/BlogPost3_2.PNG" /></p>

<p>All graphics in this blog post are based on a vertical cross section created at <a href="https://www.tropicaltidbits.com/">tropicaltidbits.com</a></p>

<p>Related research project: <a href="https://hingong.github.io/portfolio/portfolio-3/">diabatic tilting of potential vorticity</a></p>]]></content><author><name>Hing Ong</name><email>hing5ong5@gmail.com</email></author><category term="research" /><summary type="html"><![CDATA[]]></summary></entry><entry><title type="html">Tiong-tshiu khuài-lo̍k</title><link href="https://hingong.github.io/posts/2020/10/blog-post-1/" rel="alternate" type="text/html" title="Tiong-tshiu khuài-lo̍k" /><published>2020-10-01T00:00:00-07:00</published><updated>2020-10-01T00:00:00-07:00</updated><id>https://hingong.github.io/posts/2020/10/blog-post-1</id><content type="html" xml:base="https://hingong.github.io/posts/2020/10/blog-post-1/"><![CDATA[<p>Tiong-tshiu khuài-lo̍k (in Taiwanese Hokkien). Happy Mid-Autumn.</p>]]></content><author><name>Hing Ong</name><email>hing5ong5@gmail.com</email></author><category term="miscellaneous" /><summary type="html"><![CDATA[Tiong-tshiu khuài-lo̍k (in Taiwanese Hokkien). Happy Mid-Autumn.]]></summary></entry></feed>