{"id":37860,"date":"2023-05-15T15:58:10","date_gmt":"2023-05-15T07:58:10","guid":{"rendered":"https:\/\/3t-insulation.com\/fire-plume-and-ceiling-jet\/"},"modified":"2026-01-28T23:28:38","modified_gmt":"2026-01-28T15:28:38","slug":"fire-plume-and-ceiling-jet","status":"publish","type":"post","link":"https:\/\/3t-insulation.com\/en\/fire-plume-and-ceiling-jet\/","title":{"rendered":"Fire Plume and Ceiling Jet"},"content":{"rendered":"

Fire Plume and Ceiling Jet<\/h1><\/div><\/div><\/div>

<\/i><\/i><\/span>Skip to your preferred section<\/span><\/a><\/h4><\/div>
\n
<\/div><\/div>\n<\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div><\/div>

Plume<\/h2><\/div>

A plume is a column of hot smoke and gases produced by combustion that rises vertically due to buoyancy force.<\/p>\n

Buoyancy force is the force created by the density difference between smoke and air. Because smoke has high temperature and lower density than cool air, it rises vertically.<\/p>\n<\/div>

\"Enclosure<\/span>
<\/div>

Image - Enclosure Plume<\/p><\/div><\/div><\/div><\/div><\/div>

Axisymmetric Plume<\/h2><\/div>

The plume is divided into 3 zones:<\/p>\n

Continuous Flame<\/b> zone with continuous flame<\/p>\n

Intermittent Flame<\/b> zone where fuel combustion is nearly complete, with flame appearing partially and intermittently<\/p>\n

Buoyant Plume <\/b>zone where combustion is complete, containing only hot gases<\/p>\n<\/div>

\"Axisymmetric<\/span>
<\/div>

Image - Axisymmetric Plume\n<\/p><\/div><\/div><\/div><\/div><\/div>

Plume Velocity<\/h2><\/div>

We can measure smoke velocity at different heights along the centerline of the plume. The velocity in each zone can be calculated as follows:<\/p>\n

Flame:<\/strong><\/p>\n

z\/Q\u03072\/5 <\/sup>< 0.08 u0<\/sub> = 6.8z1\/2<\/sup><\/p>\n

Intermittent:<\/strong><\/p>\n

0.08 < z\/Q\u03072\/5 <\/sup>< 0.2 u0<\/sub> = 1.9Q\u03071\/5<\/sup><\/p>\n

Plume:<\/strong><\/p>\n

z\/Q\u03072\/5 <\/sup>> 0.2 u0<\/sub> = 1.1z-1\/3<\/sup>Q\u03071\/3<\/sup><\/p>\n<\/div><\/div><\/div>

Plume Temperature<\/h2><\/div>

The temperature of smoke along the centerline changes with increasing height. We can divide these changes into 3 zones:<\/p>\n

Flame:<\/strong><\/p>\n

z\/Q\u03072\/5 <\/sup>< 0.08 \u2206T0 <\/sub>= 2.91T\u221e<\/sub><\/p>\n

Intermittent:<\/strong><\/p>\n

0.08 < z\/Q\u03072\/5 <\/sup>< 0.2 \u2206T0 <\/sub>= 0.227(Q\u03072\/5<\/sup>\/z) T\u221e<\/sub><\/p>\n

Plume:<\/strong><\/p>\n

z\/Q\u03072\/5 <\/sup>> 0.2 \u2206T0 <\/sub>= 0.076T\u221e<\/sub> (Q\u03072\/5<\/sup>\/z)5\/3<\/sup><\/p>\n<\/div><\/div><\/div>

Ceiling Jet<\/h2><\/div>

When smoke hits the ceiling, it flows radially outward. This flow under the ceiling is called a Ceiling Jet. The temperature and velocity of the ceiling jet directly affect the response time of fire detection devices (such as Sprinklers, Heat Detectors, Smoke Detectors).<\/p>\n<\/div>

\"Ceiling<\/span>
<\/div>

Image - Ceiling Jet Flow<\/p><\/div><\/div><\/div>

The ceiling jet flow can be classified into 2 types, depending on the ratio of beam depth (hb<\/sub>) and beam spacing (W) to the height from fuel surface to ceiling (H):<\/p>\n

Unconfined Ceiling jet: <\/span>hb<\/sub>\/H < 0.126(H\/W)1\/3<\/sup> <\/span>and <\/span>W\/H > 1.2<\/p>\n

Confined Ceiling jet: <\/span>hb<\/sub>\/H > 0.126(H\/W)1\/3<\/sup> <\/span>and 0.4 < W\/H > 1.2<\/p>\n<\/div><\/div><\/div>

Unconfined Ceiling<\/h3><\/div>

Temperature of ceiling jet at distance R<\/p>\n

R\/H < 0.18 \u2206TCJ <\/sub>= 16.9 Q\u03072\/3 <\/sup>\/H5\/3<\/sup><\/p>\n

R\/H > 0.18 \u2206TCJ <\/sub>= 5.38 (Q\u0307\/R)2\/3 <\/sup>\/H<\/p>\n

\u2206TCJ <\/span><\/sub>is the temperature difference of the Ceiling Jet<\/p>\n

Velocity of ceiling jet at distance R<\/p>\n

R\/H < 0.18 uCJ <\/sub>= 0.96(Q\u0307\/H)1\/3<\/sup><\/p>\n

R\/H > 0.18 uCJ <\/sub>= 0.195Q\u03071\/3<\/sup>H1\/2<\/sup> \/ R5\/6<\/sup><\/p>\n

uCJ <\/span><\/sub>is the velocity of the Ceiling Jet<\/p>\n<\/div>

\"Unconfined<\/span>
<\/div>

Unconfined Ceiling<\/p><\/div><\/div><\/div><\/div><\/div>

Confined Ceiling<\/h3><\/div>

Temperature of ceiling jet at distance L (L>W\/2)<\/p>\n

\u2206TCJ<\/sub>\/\u2206T0<\/sub> = 0.37(H\/W)1\/3<\/sup> exp[ -0.16(L\/H)(W\/H)1\/3 <\/sup>]\nVelocity of ceiling jet at distance L (L>W\/2)<\/p>\n

uCJ<\/sub>\/u0 <\/sub>= 0.27\/(W\/H)1\/3<\/sup><\/p>\n

When L < W\/2, the velocity and temperature of the smoke can be calculated using unconfined ceiling jet equations<\/p>\n<\/div>

\"Confined<\/span>
<\/div>

Confined Ceiling<\/p><\/div><\/div><\/div><\/div><\/div>

Example 2<\/h3><\/div>

A fire occurs in a room with a height of 3 meters from the fuel surface to the ceiling. If the fire releases a constant energy of 1,000 kW and the air temperature is 25\u00baC, answer the following questions:<\/p>\n

    \n
  • At 3 meters above the fire, which zone of the Fire Plume is it in?<\/li>\n
  • Calculate the temperature and vertical velocity at 3 meters above the fire.<\/li>\n
  • Calculate the temperature and velocity of the Ceiling Jet at a radial distance of 2 meters if the smoke flow is:<\/li>\n<\/ul>\n
      \n
    • \n
        \n
      • Unconfined Ceiling <\/span><\/li>\n
      • Confined Ceiling (W = 1.5 m)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<\/div>
        \"\"<\/span>
        <\/div>

        Image - Illustration for Example 2<\/p><\/div><\/div><\/div>

        Given:<\/p>\n

        Q\u0307 = 1,000 kW, z = 3 m, T\u221e<\/sub> = 25\u00baC = 25 + 273 = 298K<\/p>\n

        Calculate z\/Q 2\/5 <\/sup>to determine which zone the plume is in at 3 m height<\/p>\n

        z\/Q2\/5 <\/sup>= 3\/(1000)2\/5 <\/sup>= 0.19<\/p>\n

        Since 0.08 < z\/Q 2\/5 <\/sup>= 0.19 < 0.20, therefore at 3 m height, the plume is in the Intermittent Flame zone. We can calculate the temperature and velocity of the plume at 3 m using the equation:<\/p>\n

        0.08 < z\/Q2\/5 <\/sup>< 0.20<\/p>\n

        u0<\/sub> = 1.9Q\u03071\/5 <\/sup>= 1.9(1,000)1\/5 <\/sup>= 7.56 m\/s<\/p>\n

        \u2206T0 <\/sub>= 0.227(Q\u03072\/5<\/sup>\/z) T\u221e <\/sub>= <\/span>0.227(1\/0.19)298 <\/span>= 357 K<\/p>\n

        Therefore, the plume temperature will be T0<\/sub> – T\u221e <\/sub>= T0<\/sub> – 298 = 357 or T0<\/sub> = 655K = 382 \u00baC<\/p>\n

        The calculations show that at 3 meters height, the plume is in the Intermittent Flame zone, with a vertical velocity of 7.56 m\/s and a temperature of 382 \u00baC<\/p>\n

        Smoke can flow freely under the ceiling. We can calculate the temperature and velocity of the ceiling jet. From the problem, we know R = 2 m and H (room height) = 3 m, therefore R\/H = 2\/3 = 0.67 > 0.18. Thus, the ceiling jet temperature will be:<\/p>\n

        \u2206TCJ<\/sub> = 5.38 (1000\/2)2\/3<\/sup>\/3 = 112.97<\/p>\n

        \u2206TCJ <\/sub>= 112.97 K or TCJ<\/sub> = 410.97 K = 137.97\u00baC<\/p>\n

        Ceiling jet velocity at R\/H = 0.67 > 0.18<\/p>\n

        uCJ <\/sub>= 0.195Q\u03071\/3<\/sup>H1\/2<\/sup> \/ R5\/6 <\/span><\/sup>= <\/span>0.195(1000)1\/3<\/sup>(3)1\/2<\/sup> \/(3)5\/6 <\/sup>= 1.89<\/p>\n

        The ceiling jet velocity at 2 m is 1.89 m\/s<\/p>\n

        For the unconfined ceiling jet at a radius of 2 m from the plume centerline, the temperature is 137.45\u00baC and the velocity is 1.89 m\/s<\/p>\n

        For smoke flowing under the ceiling between beams with W = 1.5 m at distance L = 2 m, we can calculate the smoke temperature using:<\/p>\n

        \u2206TCJ<\/sub>\/\u2206T0 <\/sub>= <\/span>0.37(H\/W)1\/3<\/sup> exp[ -0.16(L\/H)(W\/H)1\/3 <\/sup>]<\/p>\n

        = <\/span>0.37(3\/1.5)1\/3<\/sup> exp[ -0.16(2\/3)(1.5\/3)1\/3 <\/sup>]<\/p>\n

        = <\/span>0.428<\/p>\n

        u CJ <\/sub>\/ u 0 <\/sub>= <\/span>7.56 <\/span>Therefore: <\/span>uCJ <\/sub>= 0.34(7.56) = 2.57 m\/s<\/p>\n

        In part 2, for smoke flowing between beams with W = 1.5 m at L = 2 m, the temperature is 178 \u00baC and velocity is 2.57 m\/s<\/p>\n

        This example demonstrates that the temperature and velocity of ceiling jet flow in confined spaces are higher than in unconfined spaces. This is because the energy from combustion in confined spaces is channeled in one direction, resulting in higher temperature and velocity compared to smoke that can spread freely under the ceiling.<\/p>\n<\/div><\/div><\/div><\/div><\/div><\/p>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":37868,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[627],"tags":[],"class_list":["post-37860","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-fire-protection-systems"],"_links":{"self":[{"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/posts\/37860","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/comments?post=37860"}],"version-history":[{"count":0,"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/posts\/37860\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/media\/37868"}],"wp:attachment":[{"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/media?parent=37860"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/categories?post=37860"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/3t-insulation.com\/en\/wp-json\/wp\/v2\/tags?post=37860"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}