TW200900153A - A method and a control system for controlling the operation of a last field of an electrostatic precipitator - Google Patents

A method and a control system for controlling the operation of a last field of an electrostatic precipitator Download PDF

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TW200900153A
TW200900153A TW97107538A TW97107538A TW200900153A TW 200900153 A TW200900153 A TW 200900153A TW 97107538 A TW97107538 A TW 97107538A TW 97107538 A TW97107538 A TW 97107538A TW 200900153 A TW200900153 A TW 200900153A
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Prior art keywords
slap
dust
time
peak
emission
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TW97107538A
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Chinese (zh)
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TWI405615B (en
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Scott A Boyden
Anders Karlsson
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Alstom Technology Co Ltd
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B03SEPARATION OF SOLID MATERIALS USING LIQUIDS OR USING PNEUMATIC TABLES OR JIGS; MAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03CMAGNETIC OR ELECTROSTATIC SEPARATION OF SOLID MATERIALS FROM SOLID MATERIALS OR FLUIDS; SEPARATION BY HIGH-VOLTAGE ELECTRIC FIELDS
    • B03C3/00Separating dispersed particles from gases or vapour, e.g. air, by electrostatic effect
    • B03C3/34Constructional details or accessories or operation thereof
    • B03C3/74Cleaning the electrodes
    • B03C3/76Cleaning the electrodes by using a mechanical vibrator, e.g. rapping gear ; by using impact
    • B03C3/763Electricity supply or control systems therefor

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  • Engineering & Computer Science (AREA)
  • Automation & Control Theory (AREA)
  • Mechanical Engineering (AREA)
  • Electrostatic Separation (AREA)

Abstract

An electrostatic precipitator (1) has a last field (14) being provided with discharge electrodes (16), collecting electrodes (18) and a rapping device (22), which is adapted for cleaning the collecting electrodes (18) by means of rapping them. A control system (30) for controlling the dust particle emission from the electrostatic precipitator (1) comprises a control device (38), which is operative for adjusting, based on a relation between a magnitude (H) of a selected dust particle emission peak caused by a selected rapping and the time (t) between said selected rapping and its immediately preceding rapping, at least one parameter chosen from the group of: the time (t) to elapse until a rapping is to be executed in the last field (14), and the type of rapping to be executed in the last field (14).

Description

200900153 九、發明說明: 【發明所屬之技術領域】 本發明係關於一種控制來自靜電集塵器之塵粒發射的方 法,該靜電集塵器具有一最後場,該最後場係提供放電電 極、收集電極、及一拍擊裝置,該拍擊裝置係經調適用以 藉由拍擊該等收集電極來為其除塵。 本發明亦關於一種預測靜電集塵器之最後場之至少一收 集電極之拍擊期間之塵粒之發射的方法。200900153 IX. Description of the Invention: [Technical Field] The present invention relates to a method of controlling dust emission from an electrostatic precipitator having a final field, the last field providing a discharge electrode and a collecting electrode And a slap device adapted to smear the collector electrodes by slap them. The invention also relates to a method of predicting the emission of dust particles during the slap of at least one of the collection electrodes of the last field of the electrostatic precipitator.

本發明亦關於一種用以控制來自上面說明之類型之靜電 集塵器之塵粒發射的控制系統。 本發明亦關於一種用以預測來自上面說明之類型之靜電 集塵器之塵粒發射的控制系統。 【先前技術】 媒、油、工業廢棄物、家庭廢棄物、泥炭、生物體等之 燃燒產生包含塵粒之煙道氣(其常常稱為飛灰ρ塵粒向環 境空氣之發射必須保持處於—低位準,因&,將煙道氣發 射至%境空氣之珂’常常使用一類型靜電集塵器⑽p)之 過濾器來收集來自煙道氣之塵粒。在其他文件中從仍 4,5〇2,872所瞭解的Esp係提供放電電極及收集電極板。放 電電極使塵粒帶電’之後在收集電極板處收集該等塵粒。 當收集電極板載有塵粒時,拍擊收集電極板以便使所收集 之塵粒從收集電極板釋放並落 漏斗中,可從該漏斗 運輸該等塵粒。經由—堆疊將已除塵氣體發射㈣ i兄空氣。 129145.doc 200900153 ESP常常提供數個串聯_合之獨立單元,其亦稱為場。 WO 9!編37(其說明三個串聯輕合之個別場)中可找到此 之一範例。第一場收隹畀+θ ^ 集取大數置之塵粒,因此需要比後續 場頻繁得多的拍擊。昜诒说 後贫僅收集進入ESP之塵粒之總量 的約0至3〇/〇。拍擊(1係力 匕、係在預权規則基礎上進行)一場時, 離開ESP並發射至環境空氣 兄二孔的壓粒之數置在一短週期期間 增加至相當高的位進,甘+ i 旱其在煙道氣中的塵粒經由堆疊而發 射時甚至可視覺上觀察到。 " 【發明内容】 本發明之-目的係提供—種方法,其使得可以控制藉由 靜電集塵器中之最後場之拍擊所造成的臨時大塵粒發射峰 值0 此目的係藉由一種控制來自靜電集塵器之塵粒發射的方 法而實現,該靜電集塵器具有—最後場,該最後場係提供 放電電極、收集電極、及一拍擊裝置,該拍擊裝置係經調 適用以藉由拍擊該等收集電極來為其除塵,該方法係特徵 化為以下步驟 i) 利用藉由一選定拍擊所造成之一選定塵粒發射峰值之 中田度與介於該選定拍擊與其緊接先前拍擊間之一時間之 間的一關係,及 ii) 基於該關係,調整選自以下群組之至少一參數:該最 後場中將要執行一拍擊之前的欲歷時之時間,及該最後場 中欲執行之拍擊類型。 此方法之一優點係可以不超過塵粒發射限制的此一方式 129145.doc 200900153 準確控制該拍擊。因此,藉由本發明’可以在靜電集塵器 中採用較少場、或較小場(與依據―先前技術方法運作時 所必需之場相比)。此係由於依據本發明之一具體實施例 ,該方法運作該靜電集塵器時可減小該靜電集塵器之機械 。又。十中之安王限度的事實。該拍擊之控制可與將要執行一 拍擊之前的欲歷時之時間有關,或可與欲執行之拍擊類型 有關,或可與欲歷時之時間及拍擊類型兩者有關。 依據一具體實施例,該步驟⑴進一步包含 計舁波動平均(rolling請响)值其各對應於一預設週 期期間之平均塵粒發射,及 基於該關係,相對於一預設波動平均限制值調整該最後 場之該等收集電極之該拍擊。此具體實施例有利地提供用 以不會因錯誤時間無意中㈣,或無意中實行錯誤拍擊類 型而超過-塵粒發射限制(該限制係—波動 方式控制拍擊。 依據車又佳具體實施例,在該步驟〇中識別欲採 類型,且選擇般罕 才擊類型特定模型以便在步驟i}中加以利 用’此類選定拍擊類型 夕H 1特疋模型係藉由-選定拍擊所造成 =選疋塵粒發射峰值之—幅度與介於該已 類型之該選定拍擊盥 号疋拍擊 的-模型。拍整/ 拍擊間之時間之間之關係 類型…月間所釋放之灰塵量取決於所執行之拍擊 、a利用為拍擊類型特定之模型,可以實扩 確控制。 』从貫% —更準 較佳地, 在s亥步驟i)中 當利用藉由一 選定拍擊所造成 129145.doc 200900153 之選疋塵粒發射峰值之一幅度與介於該選定拍擊與其緊 接先引拍擊間之—時間之間的該關係時,識別並考量★亥選 定拍擊之前所執行之拍擊類型,該緊接先前拍擊之;已 加以識別。拍擊期間所釋放之灰塵量取決於所述拍擊之前 行之拍擊類型。藉由考量所述拍擊之前所實行之拍擊 類型’可以實施—更準確控制。The invention also relates to a control system for controlling the emission of dust particles from an electrostatic precipitator of the type described above. The invention also relates to a control system for predicting the emission of dust particles from an electrostatic precipitator of the type described above. [Prior Art] Combustion of media, oil, industrial waste, household waste, peat, organisms, etc. produces flue gas containing dust particles (often referred to as fly ash ρ dust particles must be kept in the emission of ambient air - Low level, due to &, the emission of flue gas to the air of the '% of the air' often uses a type of electrostatic precipitator (10) p) filter to collect dust particles from the flue gas. In other documents, the Esp system, which is still known from 4, 5, 2, 872, provides a discharge electrode and a collector electrode plate. The discharge electrode collects the dust particles at the collecting electrode plate after the discharge electrode charges the dust particles. When the collecting electrode plates are loaded with dust particles, the collecting electrode plates are slapped so that the collected dust particles are released from the collecting electrode plates and dropped into the funnel from which the dust particles can be transported. The dust-removed gas is emitted via the stacking (4) air. 129145.doc 200900153 ESP often provides several serial-integrated units, also known as fields. An example of this can be found in WO 9!, ed. 37, which describes an individual field of three series of light combinations. The first field + θ ^ collects a large number of dust particles, so it requires a much more frequent slap than the subsequent field. It is said that the latter is only about 0 to 3 〇 / 〇 of the total amount of dust particles entering the ESP. When the slap (1 line is based on the pre-authorization rule), the number of granules leaving the ESP and emitted to the ambient air brother hole is increased to a relatively high position during a short period of time. + i Drought particles in the flue gas are even visually observed when they are emitted via stacking. < SUMMARY OF THE INVENTION The present invention is directed to providing a method for controlling a temporary large dust particle emission peak caused by a last field slap in an electrostatic precipitator. A method of controlling dust emission from an electrostatic precipitator having a final field, the last field providing a discharge electrode, a collecting electrode, and a slap device, the slap device being adapted To remove dust by slapping the collecting electrodes, the method is characterized as the following steps: i) using one of the selected dust particles to be selected by a selected slap, and the selected slap a relationship between one time immediately before the previous slap, and ii) based on the relationship, adjusting at least one parameter selected from the group consisting of: the time of the last time before the slap is performed in the last field, And the type of slap to be performed in the final game. One of the advantages of this method is that it can not exceed the dust emission limit of this method 129145.doc 200900153 accurately control the slap. Thus, by the present invention, fewer fields, or smaller fields, can be employed in an electrostatic precipitator (as compared to the fields necessary to operate in accordance with prior art methods). This is because, in accordance with an embodiment of the present invention, the method of operating the electrostatic precipitator reduces the mechanics of the electrostatic precipitator. also. The fact that the tenth king of the king is limited. The control of the slap may be related to the time of the slap before the slap is to be performed, or may be related to the type of slap to be performed, or may be related to both the time of the slap and the type of slap. According to a specific embodiment, the step (1) further includes calculating a rolling average value corresponding to an average dust emission during a predetermined period, and based on the relationship, relative to a predetermined fluctuation average limit value. The slap of the collection electrodes of the last field is adjusted. This particular embodiment is advantageously provided to not exceed the dust particle emission limit due to inadvertent (4) inadvertent time, or inadvertently performing the wrong slap type (the restriction system - the wave mode control slap. For example, in the step 〇, the type of the desired type is identified, and the type-specific model is selected to be used in step i} to use the type of the selected slap type H 1 feature model by selecting the slap Cause = the peak of the emission of the dust particles - the magnitude of the relationship between the selected type of slap slaps and the type of the slap. The type of relationship between the time of the beat / slap... the dust released during the month The amount depends on the slap performed, and the slap is a specific model of the slap type, which can be controlled by real expansion. 』%%-more preferably, in shai step i) Identifying and considering the relationship between the peak of the dust emission of 129145.doc 200900153 and the time between the selected slap and the first slap. Previously executed slap The slap of the immediately preceding; has to be identified. The amount of dust released during a slap depends on the type of slap that was taken before the slap. It can be implemented - more accurately controlled by considering the type of slap performed prior to the slap.

、=佳藉由下面的式子來表示藉由—選^拍擊所造成之— 選疋塵粒發射峰值之—幅度與介於該選定拍擊與其 前拍擊間之時間之間的該關係: 、’、 幅度QC函數(時間), 其中從以下函數中選擇該函數:對數函數、及對數函數 ^近似值,該函數較佳為自然、對數函數。自該緊接先前拍 來所歷時之時間越長,拍擊期間所釋放之灰塵越多。 不過’灰塵也會黏聚於收集電極板上,因此-選定塵粒發 射峰值之ψ田度與自其緊接先前拍擊以來所歷時之時間之間 的戎關係並非線性的’而是最好藉由一對數函數加以說 明0 —依據車父佳具體實施例,藉由一選定拍擊所造成之一選 發科值之―幅度與介於該選定㈣與其緊接 =之時間之間之一關係的一數學模型可藉由測量塵粒 ^射峰值之幅度並使其與自該個別緊接先前拍擊以來所歷 時之個別時間輕合而獲 " 備該數學模型。 …貝枓㈣可用於製 較佳藉由以下步驟來更新藉由—選定拍擊所造成之一選 129145.doc 200900153 定塵粒發射峰值之-幅度與介於該選定拍擊與其緊接先前 拍擊間之時間之間之一關係的一數學模型 D) 測里该最後場之後之塵粒發射以識別與該最後場之 至少一收集電極之一拍擊有關的一塵粒發射峰值, E) 使該塵纟發射峰值之該測量幅度與自該最後場之該 至少-收集電極之該緊接先前拍擊以來所歷時之該對應時 間輕合以便形成一資料記錄’此類資料記錄包含該塵粒發 ( 射峰值之§亥幅度及自該緊接先前拍擊以來所歷 時間,及 =基於該資料記錄,更新藉由—選定拍擊所造成之一 選定塵粒發射峰值之一幅度與 又興,丨於忒選定拍擊與其緊接先 則拍擊間之時間之間之一關係的該數 例之一優點係更新該模型,使 八 細 齒带隹使侍該杈型可經調適以適於該 靜電集塵器之運作之變化你杜 φ, . # , 〃牛。此類變化條件可與燃料類 笑古、收集電極板之表面特性之與時間有關之變化等 等有關。該模型之咳t軿尨& a 1 化# …* 較佳(但並非必須)在各新拍擊 i進仃。作為替代,亦可每 _ 該更新。更佳地,步驟F)期門:::三等等拍擊進行 -資料^ )期間更新該數學模型的同時利用 貝枓過濾器。此具體實施例之— 更新該模型,且亦J係以一更準確方式 器之變化條件。 、1乂適於該靜電集塵 依據另-較佳具體實施例,基於該關 組之至少—參數:該最後場中將要執行…乂下 歷時之時間,及續最彳乡ie + 仃一拍擊之前的欲 最後场中欲執行之拍擊類型,的該步驟 129145.doc -10- 200900153 係藉由以下步驟來執行: 測量藉由該最後場之該等 ㈣所在 线杲電極之至少—收集電極之 拍擊所造成之-塵粒發射峰值之幅度, 將關於該塵粒發射峰信 算裝置, 奴迓主 〇t 該計算裝置比較該絲發射峰值之該測 發射峰值幅度目標值,及 -興塵拉 用於最小化該塵粒發射峰值幅度目標值與藉由 之該等收集電極之至少一收集電極之一後續拍擊所造成之 :;續塵粒發射峰值之測量幅度間之差的目的,藉由該計 :裝置’自動調整選自以下群組之至少—參數:該最後場 要執行該後續拍擊之前的欲歷時之時間,及該最後場 中欲執行之後續拍擊類型。此具體實施例之-優點係可利 用:相當簡單的計算裝置,例如PID控制器、、ρι控制器或 無模型適應性控制器。由於不需要—模型,所以不需要與 獲得此一模型有關的任何廣泛工作。此外,拍擊之控制將 相當快地調適以適於該靜電集塵器之變化條件,因為關於 塵粒發射峰值之幅度的測量資料係連續發送至該計算裝 置。 、 本發明之另一目的係提供一種可靠的預測靜電集塵器之 最後場之至少一收集電極之拍擊期間之塵粒之發射的方 法。, = by the following formula to represent the relationship between the selection of the slap - the peak of the emission of the dust particles - the relationship between the selected slap and the time between the previous slap : , ', amplitude QC function (time), where the function is selected from the following functions: a logarithmic function, and a logarithmic function ^ approximation, which is preferably a natural, logarithmic function. The longer the time since the previous shot was taken, the more dust is released during the slap. However, 'dust will also stick to the collecting electrode plate, so the 戎 relationship between the peak of the selected dust emission peak and the time since the previous slap is non-linear' is the best. Described by a one-to-one function 0. According to the specific embodiment of the car father, one of the selected values of the selected value by one selected slap is between one of the selected (4) and the immediately preceding = A mathematical model of the relationship can be obtained by measuring the magnitude of the peak of the dust particle and making it coincide with the individual time of the individual since the previous slap. ...Beibei (4) can be used to make the update by the following steps - one of the selected slaps is selected 129145.doc 200900153 to determine the peak of the dust emission - the amplitude and the selected slap immediately before it a mathematical model of the relationship between the times of the hits D) measuring the dust emission after the last field to identify a dust emission peak associated with one of the at least one collecting electrode of the last field, E) The measured amplitude of the dust mite emission peak is lighted from the corresponding time of the at least-collecting electrode of the last field since the previous slap to form a data record. The granules (the amplitude of the peak of the shot and the time since the previous slap, and = based on the data record, the update by the selected slap, one of the peaks of the selected dust emission amplitude and One of the advantages of the relationship between the selected slap and the time between the slap and the time between the slaps is to update the model so that the eight-toothed belt can be adapted Suitable for the electrostatic precipitator Changes in the operation of your Du φ, . # , yak. Such changes can be related to the fuel-like laughter, the time-dependent changes in the surface characteristics of the collector plates, etc. The model cough t軿尨&a 1化# ...* It is better (but not necessary) to enter each new slap. As an alternative, it can also be updated every _. More preferably, step F) is the door::: three, etc. The data ^) is updated while the mathematical model is being used while using the Bellow filter. This particular embodiment - updates the model, and also J changes the condition in a more accurate manner. According to another preferred embodiment, at least the parameter: the last field will be executed... the time of the last time, and the last time The step 129145.doc -10- 200900153 of the type of slap desired to be executed in the last field is performed by the following steps: measuring at least the collection of the electrodes on the line by the (4) of the last field. The amplitude of the peak of the dust emission caused by the slap of the electrode, the target value of the measured emission peak amplitude of the peak of the emission of the wire will be compared with the calculation device of the dust particle emission peak, and The dusting pull is used to minimize the target value of the peak amplitude of the dust particle emission and the subsequent slap by one of the collecting electrodes of the collecting electrodes: the difference between the measured amplitudes of the peaks of the dust particle emission Purpose, by means of the meter: the device 'automatically adjusts at least from the following group' parameters: the time of the last time before the last field is to be executed, and the subsequent type of slap to be performed in the last field. The advantages of this embodiment are: a relatively simple computing device, such as a PID controller, a ρι controller or a modelless adaptive controller. Since there is no need for a model, there is no need for any extensive work related to obtaining this model. In addition, the control of the slap will be adapted relatively quickly to suit the changing conditions of the electrostatic precipitator since the measurement data relating to the magnitude of the peak of the dust emission is continuously transmitted to the computing device. Another object of the present invention is to provide a reliable method for predicting the emission of dust particles during the slap of at least one of the collection electrodes of the last field of the electrostatic precipitator.

I I 目的係藉由一種預測靜電集塵器之最後場之至少一收 木電極之拍擊期間之塵粒之發射的方法而實現,該最後場 I29145.doc 200900153 係提供放電電極、收集電極、及—拍擊裝置, 係經調適用以狃+ Λ 擊裝置 、用以藉由拍擊該等收集電極來為其除 係特徵化為α下步,驟 5亥方法 =用藉由m自擊所造成之—選定塵粒發射峰值之一 :ΓΓ選定拍擊與其緊接先前拍擊間之時間之間的 幅由—選定拍擊所造成之一選定塵粒發射峰值之-田又、"於該選定拍擊與其緊接先前 該關係’預測-從以下參數中選擇之參數:_間之間的 係基於該選定::::造成之塵粒發射峰值之幅度,其 間,及 $與其緊接先前拍擊間之-欲歷時之時 其::基緊接先前拍擊間之欲歷時之時間, 度。 3、疋拍擊所造成之一塵粒發射峰值之幅 至:=:::點係可以以高準確度預測藉由該最後場之 測起因於Π:;:擊所造成之塵粒發射。因此,可以預 一拍擊頻率 、羊的係哪一塵粒發射,或預測需要哪 大波動平均。此^塵粒發射,例如某一塵粒發射之最 用階段期間靜電::可用於靜電集塵器之設計,,以及啟 本發明之2器之運作之調整中。 除,或至少減少目的係提供一種控制系統,其使得可以消 臨時大塵粒發^之^集塵器之最後場之拍擊期間發生的 I29145.doc 12· 200900153 此目的妄在 種用以控制來自靜電集塵器之塵粒發射 ==而實現,該靜電集塵器具有-最後場,該最後 1 '電電極、收集電極及-拍擊裝置,該拍擊裝置 二調適用以藉由拍擊該等收集電極來為 糸統之特徵為其包含 利 一㈣^置,其係可運作以,基於藉由―狀拍擊所造 私之選疋塵粒發射峰值之—幅度與介於 緊接先前拍擊間之時間之間的一關係,調整選自以下群;^ 之^少一參數:該最後場中將要執行—拍擊之前的欲歷時 之時間,及該最後場中欲執行之拍擊類型。 :此控制系統之-優點係其提供拍擊之有效控制,使得可 最小化來自—靜電集塵器之塵粒發射。 依據-較佳具體實施例,該控制系統進一步包含 一貝料接收器,其係可運作以接收與該最後場之後之塵 T發射有關之測置資料,及在該測量資料_識別與該最後 場之該至少-收集電極之拍擊有關的—塵粒發射峰值, 一資料處理n,其係可運作錢該録發 自該最後場之該至少一收集電極之該緊接先二 擊以來所歷時之該對應時間輕合以便形成一資料記錄,此 類資料記錄包含該峰值之該幅度及自該緊接先前拍擊以來 所歷時之該對應時間,及 -計算裝置,其係可運作以,基於該資料記錄,更新該 數學模型’《學模型係藉由—選定拍擊所造成之 塵粒發射峰值之-幅度與介於該選定拍擊與其緊接先前拍 129145.doc -13· 200900153 擊間之時間之間之該關係的一近似值。 優點係藉由更新#叙風# 〃、體實施例之一 模型二: (例如’藉由如此更新該數學 本:更新,因數,控制系統之控制功能將 準需要:適::電集塵器之變化條件,使得控制更 且而要較少隨時間手動校準。 二=佳具體實施例’一計算裝置係可運作以接收 所造成之-塵粒發射收集電極之拍擊 計算裝置係進—步㈣適用二:又有關的測量資料,該 旦 步調適用以比較該塵粒發射峰值之該測 置幅度與一塵粒發射峰值幅度目標值,及用於最小化該塵 粒發射峰值幅度目標值與藉由該最後場之該等收集電極之 β亥至ν &集電極之-後續拍擊所造成之-後續塵粒發射 峰值之測量幅度間之差的目的,藉由該控制裝置,自動誘 自以下群組之至少一參數之調整:該最後場中將要執 行該後續拍擊之前的欲歷時之時間’及該最後場中欲執行 之後續拍擊X員型。此具體實施例之一優點係其提供拍擊之 簡單但有效控制。該計算裝置可為PID控制器(結合比例、 積分、及微分參數運作之控制器)、ρι控制器(結合比例與 積分參數運作之控制器)、或無模型適應性控制器,即不 利用實體特性之實際模型之情況下基於(例如)神經網路力 爭減小觀察值與目標值間之差的控制器。 本發明之另一目的係提供一種致能藉由靜電集塵器之最 後場之至少一收集電極之拍擊所造成之塵粒發射之準確預 測的控制系統。 129145.doc -14· 200900153 :目的係藉由-種用以預測來自靜電集塵器之塵粒發射 的控制糸統而實現,該靜電集 _ ,a .θ 卞!益具有一取後場,該最後 贫’、鐽供放電電極、收集電極、一 里战, 叹拍擊裝置,該拍擊裝 置係經調適用以藉由拍擊該 為該控制系統包含 4收-電極來為其除塵’特徵 -:料:理器’其係可運作以利用藉由一選定拍擊所造 腎技4·^塵粒發射峰值之—幅度與介於該選定拍擊與其 緊接先前拍擊間之時間之間的一關係,該資料處理器係進 :步可運作以’基於藉由-選定拍擊所造成之—塵粒發射 值之-幅度與介於該選定拍擊與其緊接先前拍擊間之時 間之間的該關係’預測―從以下參數_選擇之參數 )藉由冑疋拍擊所造成之塵粒發射峰值之幅度,直 係基於該選定拍擊與其緊接先前拍擊間之—欲歷時之時 間,及 2)選疋拍擊與其緊接先前拍擊間之欲歷時之時間, 其係基於藉由該選定拍擊所造成之一塵粒發射峰值之一幅 工制系統之-優點係其提供黃爭電集塵 容易調整。 低 從:明與申請專利範圍將明白本發明之其他目的。 【實施方式】 措詞”模型"在本說明中係指-現象(例如物理現象、化學II is achieved by a method for predicting the emission of dust particles during the slap of at least one of the last electrodes of the electrostatic precipitator, the last field I29145.doc 200900153 providing a discharge electrode, a collecting electrode, and - slap device, adapted to 狃 + Λ device, used to slap the collector electrode to characterize it as α next step, step 5 hai = use self-shock by m Caused by - one of the peaks of the selected dust emission: the width between the selected slap and the time between the previous slaps - the selected slap caused by one of the selected dust emission peaks - Tian You, " The selected slap is immediately followed by the relationship 'predicted - the parameter selected from the following parameters: _ is based on the magnitude of the peak of the dust emission caused by the selection::::, and $ is immediately followed The time between the previous slaps and the time of the slap:: the time and degree of the previous slap. 3. The amplitude of one of the dust emission peaks caused by the slap to: =::: The point can be predicted with high accuracy. The detection of the last field is caused by the 尘::: the dust emission caused by the shot. Therefore, it is possible to pre-slap the frequency, which dust particle is emitted by the sheep, or predict which fluctuation average is needed. This dust particle emission, for example, during the most useful phase of a dust particle emission: can be used in the design of an electrostatic precipitator, and in the adjustment of the operation of the device of the present invention. In addition to, or at least reducing, the purpose of providing a control system that allows for the occurrence of temporary dust particles to be generated during the final slap of the dust collector. I29145.doc 12· 200900153 Realizing from the dust emission of the electrostatic precipitator, the electrostatic precipitator has a - last field, the last 1 'electrode, a collecting electrode and a slap device, and the slap device is adapted to shoot The collecting electrodes are characterized by the inclusion of a singularity, which is operable to be based on the peak of the emission of the dust particles selected by the slap slap - the amplitude and the tightness The relationship between the time between the previous slaps, the adjustment is selected from the following group; ^ 少 少 one parameter: the last field will be executed - the time of the slap before the slap, and the last field to be executed The type of slap. The advantage of this control system is that it provides effective control of the slamming, so that dust emission from the electrostatic precipitator can be minimized. According to a preferred embodiment, the control system further includes a bead receiver operative to receive measurement data relating to the dust T emission after the last field, and at the end of the measurement data identification and At least the collector-related dust-collecting peak of the collecting electrode, a data processing n, which is operable to record the at least one collecting electrode of the last field from the first two strikes The corresponding time is lightly combined to form a data record comprising the amplitude of the peak and the corresponding time since the previous slap, and the computing device is operable Based on the data record, the mathematical model is updated. 'The learning model is based on the peak of the dust emission caused by the selected slap - the amplitude and the selected slap is immediately followed by the previous shot 129145.doc -13· 200900153 An approximation of the relationship between the times. The advantage is by updating #叙风# 〃, one of the embodiments of the body model two: (eg 'by updating the mathematics this way: update, factor, control system control function will be required: suitable:: electric dust collector The changing conditions make the control more and less manually calibrated over time. 2 = better embodiment 'a computing device is operable to receive the resulting slap computing device of the dust emission collecting electrode (4) Applicable 2: Relevant measurement data, the step is applied to compare the measured amplitude of the dust emission peak with the target value of the peak emission amplitude of the dust particle, and the target value for minimizing the peak amplitude of the dust emission By means of the control device, the control device automatically induces the difference between the measurement amplitudes of the subsequent dust-emission peaks caused by the subsequent slaps of the collectors of the final field Adjustment from at least one parameter of the following group: the time of the desired duration before the subsequent slap in the last field and the subsequent slap X-type to be executed in the last field. One of the advantages of this embodiment system It provides simple but effective control of the slap. The computing device can be a PID controller (controller that combines proportional, integral, and differential parameter operation), a ρι controller (controller that combines proportional and integral parameter operation), or none A model adaptive controller, i.e., a controller that strives to reduce the difference between an observed value and a target value based on, for example, a neural network without utilizing an actual model of the physical characteristics. Another object of the present invention is to provide an enabler A control system for accurately predicting the emission of dust particles caused by the slap of at least one collecting electrode of the last field of the electrostatic precipitator. 129145.doc -14· 200900153: The purpose is to predict from the electrostatic set by The control system of the dust emission of the dust collector is realized, and the static electricity set _ , a . θ 卞 益 has a back field, the last poor ', the 鐽 supply and discharge electrode, the collecting electrode, the one-mile battle, the slap device The slap device is adapted to be dusted by the slap for the control system to include a 'receiver-electrode' that is operable to utilize a selected slap Renal 4·^The relationship between the peak of the dust emission and the time between the selected slap and the time immediately following the previous slap, the data processor is operative: the step is based on 'based on the selected 拍The relationship between the dust particle emission value and the time between the selected slap and the time immediately following the previous slap 'predicted - the parameter selected from the following parameters _ slap by slap The magnitude of the peak of the dust emission caused is based on the time between the selected slap and the previous slap, and the time required for the slap and the previous slap. It is based on one of the peaks of the dust emission peak caused by the selected slap. The advantage is that it provides easy adjustment of the yellow electric dust collection. Other objects of the invention will be apparent from the scope of the invention. [Embodiment] The wording "model" refers to a phenomenon (such as physical phenomena, chemistry) in this specification.

程序等等)之矣+ L 表不此外,措詞"數學模型,,在本說明中係指 一現象之數學表示。 S “1"生解发靜電集塵器(ESP)l。靜電集塵器丄具有 129145.doc •15- 200900153 -用於煙道氣4(其包含塵粒)之人n2,及—用於煙道氣 8(其中的大多數塵粒已移除)之出口6,器!具有一外殼 9,在該外殼9中提供一第—場1〇、—第二場12、及一最後 場14。如此項技術中(例如從美國專利第4,5〇2,872號中, 該專利係藉由此引用而併入本文中)本質上所熟知,各場 f ί 1〇、12、14係提供放電電極與收集電極(其採用收集電極 板之形式)。最後場係提供放電電極(圖Hf描述直中之一 放電電極16)及收集電極板(圖i僅描述其中之—收集電極板 ⑻。電源20在放電電極16與收集電極板Η間施加一電 流。當煙道氣4穿過放雷雷搞】ή卩女 冤電極16時,塵粒會帶電。帶電塵 粒將朝收集電極板18行進,在收集電極㈣處收集塵粒。 靜電集塵器1係提供一拍擊襄置”,其係經調適用以從收 *電極板18移除所收集之塵粒。拍擊裝置22包含一第—組 錘子’其係經調適用以拍擊收集電極板之上游端。一第— =4係包含於此第—組錘子中,且係經調適用 2電極板18之上游端。拍擊裝置22亦包含一第二組鐘子, 其係經調適用以拍擊收隹 在七八 料集電極板之下游端。-第二錘子26 :3於§亥第二組錘子中,且係經調適用 板丨8之下游端。 字收杲窀極 數極板18之除塵可以不同方式進行。可變化" ’’流情況’即電源20在拍擊期間是否在電極“ 施加-電流。亦可使拍擊 8間 之州,而並非使電产首A,減至(例如)正常電流 擊之方式,拍心可…依據其他替代執行拍 月間可使電流增加或減小(與正常運作期 I29145.doc -16 - 200900153 間所採用之雷滿^ _ ^ )。若施加電流的同時收集電極板1 8 '二又拍擊’則粒子黏著於收集電極板18之能力將高於拍擊 期間不施加電流之條件下粒子黏著於收集電極板18之能 °文化的另一參數係是否在相同場合下採用第一錘子 24與第二錘子26兩者進行該拍擊,或是否僅採用錘子24、 之來執仃該拍擊。此外,使得鐘子24、26拍擊收集電 極板18之場合數將影響所收集塵粒中得以從收集電極板18 移除之數量。因办,六 、卜 存在右干不同的拍擊收集電極板18之 方式母-拍擊收集電極板18之方式將具有一關於從收集 電極板18所移除之塵粒量’且亦關於分散於煙道氣中並與 已除塵煙道氣8-起離開靜電集塵器1之塵粒量(下文中加 以說明)的特定特性。 藉由拍擊而從收集電極板18移除的塵粒係收集 28 中並運走。 圖2解說一控制系統30,其包含資料接收器32、資料處 理器34、計算裝置36、及拍擊控制裝置%。為(例如)一不 透明度计的塵粒濃度分析器4〇在連續或週期性基礎上分析 已穿過最後場14之鹿、爸/·* . 之已除塵煙道氣8中之塵粒之濃度。資料 接收器32從分析器4〇接收關 又關於壓粒發射之資訊。在資料接 收器32已從分析器4〇接收到之杳 伐叹主J之貝科中,資料接收器32識別 與一拍擊事件有關之塵粒發 «牙丁辛值。針對母一塵粒發射峰 值的關於幅度、及出規句r鹿& & Α Λ 、一 見該塵粒發射峰值之時間點的資訊係 轉遞至資料處理器34。資料處Α '了十爽理器3 4亦接收來自拍擊控制 裝置38之資訊。來自拍擊和鈿 擎控fi裝置38之資訊與執行個別拍 129145.doc 200900153 ,之^間點有闕°基於此資訊’資料處理器34使-塵粒發 峰值(其係由—拍擊造成)之幅度與自 擊:來已歷時的-對應時_。資料處理器= 二I!:峰值形成—資料記錄’下文中將對此加以說明。 將〇貝料c錄中所包含之資訊從資料處理器34轉遞料算 裝置%。計算裝置36製備及/或更新一數學模型。 楔型係經調適用以,基於一選定拍擊與其緊接先前拍擊間 之欲歷時之時間,預測藉由該敎拍擊所造成之—選 ^發射峰值(例如,藉由一將來拍擊所造成之一將來塵粒 發射峰值)之一幅度。將該數學模型轉遞至控制裝置38。 基於該數學模型,控制裝置38決定一用於該將來拍擊之人 適時間,及—合適的欲執行拍擊類型。控制裝置38接著自口 動且在-所需時間點將信號發送至拍擊裝置22,且在欲執 行電流(其係施加於放電電極16與收集電極板_授化之 條件下亦發送至電源20’以便執行一所需類型之拍擊。因 此’藉由控制裝置38所發送之該等信號可包括關於拍擊期 間應藉由電源20施加哪-電流、以及關於是否應運作及庫 如何運作第-馬達42(其運作第—組錘子24)、及是否應運 作及應如何運作第二馬達44(其運作第二組錘子叫的資 訊。每當獲得-新資料記錄時’結合下一塵粒發_, 可更新數學模型。因此,控制系統3〇提供最後場Μ中應執 行拍擊之時間、及方式的自動控制以便獲得一所需低塵粒 發射峰值。 圖3摇述藉由分析器40所提供之測量資料之一範例。γ轴 129l45.doc -18- 200900153 r 上描述不透明度信號E(不透明度計上之最大讀數之%),而 X軸上描述時間T(分鐘)。[發現塵粒發射峰值(其在圖3中 係以塵粒發射峰值PMP2之形式描述)對應於最後場从 收集電極板18之拍擊。因此’ -旦在最後場14中執行拍 擊,塵粒發射便增加以形成塵粒發射峰值PI、P2,立持續 通常約3至5分鐘。第一場1〇之拍擊及第二和之拍擊通常 對塵粒發射具有較低影響。此事實之原因係,第一場_ 之拍擊或第二場12中之拍擊造成一來自該特定場1〇、此 已增加塵粒發射。不過,第一場1〇或第二和之拍擊期間 所發射之塵粒會藉由最後場14之收集電極板Η進行有效收 集。因此,拍擊第一場1〇或拍擊第二場以效應常常藉由 最後場14(其係位於第—場1G及第二糾之下游)所吸收。 不過’在最後場14中執行一拍擊時,不存在可收集拍擊期 間所釋放之塵粒的下游場。 塵粒發射峰值P1、P2期間所發射的塵粒量對來自靜電集 塵器1之塵粒發射之波動平均具有大影響。因Λ,拍擊期 間從最後場U之收集電極板18所釋放之塵粒量係與當局所 設定之塵粒發射波動平均限制值有關。視安裝靜電集塵器 i所在之國家而定’該限制值可為(例如)6分鐘波動平均值 或1天波動平均值。藉由圖3所描述之塵粒發射峰值ρι、P2 所造成之塵粒發射之該部分對來自靜電集塵器k塵粒發 射八有重大影響’尤其對於塵粒發射之短期波動平均,例 如參考30分鐘及更短時間週期的波動平均。例如,取自塵 粒發射峰值P1附近的—6分鐘波動平均值將引起無法滿足 129145.doc -19- 200900153 當局之發射限制值的風險。 、已發現’塵粒發射峰值P1、P2之幅度M在很大程度上取 、:自緊接在造成所述塵粒發射峰值p之拍擊之前的 該拍擊以來已歷時之時間。圖3所描述之塵粒發射峰㈣ 之巾田度Μ因此取決於自造成塵粒發射峰值η之拍擊^以來 已歷時之時間t。因此’藉由拍擊R”所造成之塵粒發射峰 值P2之幅度M取決於自緊接在拍擊r ”之前之拍擊以來已 歷時之時間t。’’幅度”應理解為定義塵粒發射峰值 之大h的測ϊ。理論上’塵粒發射峰值p2之幅度Μ係藉由 峰值Ρ2所覆蓋之區域。關於拍擊期間塵粒發射上升及下降 所採用之方式’每一拍擊類型具有其自己的塵粒發射峰值 /曰、’文藉由拍擊裝置22之機械特性、拍擊期間是否施加 電流等等來決定該”指紋"。實際上,藉由塵粒發射峰值Μ 在一基線塵粒發射Β上方延伸之高度H來近似塵粒發射峰 值Ρ2之幅度Μ常常足夠準確。基線塵粒發射㈣附近位於 峰值PI、Ρ2間(即’最後場14中無拍擊時)之塵粒發射。、 圖4示意性描述藉由一拍擊所造成之一塵粒發射峰值 PI、Ρ2、Ρ3、Ρ4及Ρ5之幅度H1、Η2與自緊接先前拍擊以 來已歷時之對應時間tl、t2之間的關係。最初執行拍擊事 件使得一時間tl歷時在各拍擊事件R1、R2'们間。拍擊事 件Rl、R2、R3分別造成塵粒發射峰值卩丨、p2、p3,該等 塵粒發射峰值P1、P2、p3各具有對應於一高度出之—幅 度。不久,各拍擊事件間之欲歷時之時間係增加至時間 t2。因此,拍擊事件R4及拍擊事件R5各在自緊接先前拍擊 129l45.doc -20- 200900153 事件以來已歷時時間t2之後加以執行。拍擊事件114與115分 別導致塵粒發射峰值P4與塵粒發射峰值”。塵粒發射峰值 P4與P5各具有高度H2,其比塵粒發射峰值p1至p3之高度 H1鬲得多。因此,已發現表示為塵粒發射峰值η至w之 高度HI、H2的幅度取決於自緊接在造成所述塵粒發射峰 值之該拍擊事件之前的拍擊事件以來已歷時之時間u、 t2。因此,藉由拍擊事件尺4所造成之塵粒發射峰值以之高 度H2取決於自緊接先前拍擊事件R3以來已歷時之時間u。 圖5描述一數學模型之一範例,其係基於塵粒發射峰值 间度Η、以及自緊接在造成所述塵粒發射峰值之該拍擊事 件之前的拍擊事件以來已歷時之對應時間t的測量。已進 行二個測量,其係描述在圖5中。各測量已導致一資料圮 錄,其包括塵粒發射峄值之高度H、及自緊接先前拍擊事 件以來所歷時之時間t。此外’已添加一虛構資料記錄〇, 其係位於零點附近(實際上係丨分鐘處之丨%峰值)。藉由對 於收集電極板18之連續拍擊不會出現峰值(因為在此類條 件下不會收集塵粒)之事實激發虛構資料記錄〇。 資料記錄編號 自緊接先前拍擊以來所歷時之時間 峰值之高麿 1 t (分鐘) _ 0 ..... 1 I . 330 1 _ II …. 4300 Ο V/ __ III 11540 j / 85 表1 :自緊接先前拍擊以來所歷時之時間及對應峰值之資料 記錄。 129145.doc •21 - 200900153 已發現’藉由—選定拍擊所造成之-選定塵粒發射峰值 之幅^糸與自緊接在造成該選定塵粒發射今值之該選 擊之刖之拍擊以來已歷時之時間的對數自 數碱正比。因此,在蜂值之高度(H)之表 自然對 之自,、,、對數間進行一曲線擬合。所獲得之等式係: H(t) = 7.2*ln(t[min])-5.6[〇/〇](等式 j」) 等式1.1用作數學模型,立句明益 子偶i具說明错由一選定拍 f. :將來拍擊)將造成之-選定塵粒發射峰值(例如,二來 塵粒發射峰值)之高度H,可基於該選定㈣㈣接在= 定拍擊之前之拍擊間將歷時之時 學模型以及合適條件(例如最大許可 Γ)’控制裝置38可決定何時係執行-拍擊之si 間。若(例如)環境規則係使得塵粒發射峰值 夺 鳩之高度Η(因為此時6分鐘 二超過 超過之風險中),則可針㈣解等^值之限制係處於被 t = e_] + 5.6)/7.2 [分鐘] ^ 藉由將Η = 50%引入等式2 (等式2」) t = e〇〇W + 5,v,2rv ^ ^ ^^#,XTBffa1t: [刀鐘]= 2350 [分鐘] (等式22、 自緊接先前拍擊以來已歷時_ " 由數學模型而決定)時,於财二鐘之時㈣其已藉 行一拍擊。 控制裝置38可指示拍擊褒置22執 自然對數函數係適於Μ由目士 Η與介於該較拍擊與Α &射峰值之一幅度 、緊接先前拍擊間之時間t之間的該 129145.doc -22- 200900153 關係之事實 幅度Η與In(時間t)成正比 係藉由以下實體背景而激發:自緊接先前拍擊以來之時 間t越長,累積於收集電極板18上之塵粒就越多。累積於 收集電極板18上之塵粒越多,拍擊期間將釋放之塵粒就越 多。不過,隨著自緊接先前拍擊以來之時間增加,塵粒將 在,於收集電極板18上的同時經受已增加黏聚。該黏聚在 -定程度上抵消塵粒發射峰值之幅度之增加。總效應係自 緊接先前拍擊以來所歷時之較長時間t將導致塵粒發射峰 值之幅度增加,但該增加將小於藉由一線性函數所說明的 由於塵粒在收集電極板上之黏聚而引起之增加。作為自然 對數函數之替代’亦可(儘管有時欠佳)利用其他對數函 數、及對數函數之近似值。藉由對數函數之近似值意指 (例如)與對數函數類似之數學函數、三角函數、分段線性 曲線擬合等等。 圖&解說如何基於一自緊接先前拍擊事件幻以來已歷時 之給定時間t由#式Η預測一將來拍擊事件RF所造成之一 將來塵粒發射峰值PF之高度HF的一範例。 圖6b解說如何基於一將來塵粒發射峰值pF之一給定高度 Η由等式2」預測將要執行一將來拍擊事件rf之前自一:‘ 事件R1欲歷時之時間iF的一範例。 依據等式1.1之數學模型係僅基於三個資料記錄加上— 虛構資料記錄。亦可僅由一或兩個資料記錄加上該虛構資 料記錄來獲得一數學模型。基於此等若干資料記錄之數學 129145.doc -23- 200900153 ::型可視為一”開始模型”。不過,靜電集塵m中之條件 :曰化’因&,若不更新該數學模型,則該數學模型可能變 仔不適於拍擊之控制。或 θ 制為了专夏變化條件(例如所燃燒之 燃料的不同類型等#, 亦用於备運作條件穩定時改善 數學模型之準確慶的θ μ 次, 的’較佳在測量新資料記錄時以新 貧料記錄更新數學模型。 請-流程圖’其描述控制系統3〇工作所依據之方 法。在步驟Α中,測量最後場14之後之塵粒發射。識別— 峰值其係與最後場14之拍擊事件h有關。忽略與灰塵 分析器之校準等等有關的任何”峰值”。 在步驟B中,將蜂值Pn之高度合至自最後場μ之緊 接先前拍擊事件(即,拍擊事件Rn_〇以來已歷時之時間 tN °日守間tN說明執行拍擊事件Rn時最後場μ之收集電極板 18已為收集塵粒而在拍擊事件hi之後運作多長時間。時 間tN與對應高度Hn形成—資料記錄。 在v驟C中,為資料記錄適配一數學模型。若第一次執 :步驟C,則為自靜電集塵器1之運作之啟動以來所獲得之 兩或更多資料記錄適配一數學模型。若,另一方面, 已經存在-可用數學模型,則以包含邮之新資料記錄 更新该數學模型。 在步驟D中’基於該數學模型控制將要執行下—拍擊事 N 1之引欲歷日^之時間1。通常針對該控制使用某一 種類的條件°此—條件之—範例係,塵粒發射峰值之高度 ’、、、不超過某-值Hmax。高度Hn+i係設定為如狀,並 129145.doc -24- 200900153 將其引入數學模型中。拄! 接者’如上文參考圖5及等式2,1所 說明’計算時間tN + i。 序列A、B、c、^di^ 、 具有一迴路,使得步驟D結束時, /. 將Ν»又=為N+1,並開始步驟A,纟係描述在圖7中。以此 甘〆-T田已執〃拍擊事件時’便獲得-新資料記錄, 二3取近塵粒發射峰值之測量高度%及對應時間^。新 —貝料記錄可用以更新數學模型,以便使得數學模型更佳於 預測與時間t成函數關係之塵粒發射峰值高度h。由於該迴 路’因此可連續更新該數學模型,使得該 預測塵粒發射峰值高度。 更仫 合白’靜電集塵器1運作所處之條件在運作期間可能 二:Γ匕。此類變化包括:收集電極板18上所收集之塵 部:二:變化、煙道氣4之特性之變化、靜電集塵器1内 :’化4等。鑑於此等可能變化,當步驟C中更新 數學模型時適合 ^ 模型時賦 、’、過濾态◦可(例如)以更新數學 此一方4 ㈣記錄—較高權重(與舊資料記錄相比)的 器功能該資料過遽器…非常簡單的獲得資料過遽 兩4 曲線擬合(其形成數學模型之基礎)時 人已括新貧料記錄。執行該曲線擬人之卜 資料印铭± 四深擬σ之刖可丟棄最舊的 的同時兩二r:解忒如何在丟棄最舊資料記錄(資料記錄 t人為1v'與1v,,)包括新資料記錄1v的一範m與 表1所描述情況相 祀”(興 合。 接耆在表2之值上執行曲線擬 129145.doc -25- 200900153 Μ%) i值之高度 —--— L 1 ~~~——___430〇__ ~~-__ 11540 ----J / 85 I 2350 | 4R ――—'—. 2350 I" --— __48 T(分鐘) II 111 IV, IV" 資料記錄。 基於表2之值,可執行一新曲線擬合,且可獲 已 更新數學模型: H (t) = 6. 9*ln ⑴-2 2 ' (等式1.2) 當另一資料記錄V係可用時,將該資料記料次用⑽ 與V”’同時僅採用資料記錄IV_次,並在執行曲線擬合等 等之前丢棄資料記錄Π。雖然表2解說—非常簡單的過渡資 料記錄之方法,使得賦予新資料記錄對已更新數學模型之 較大影響(與舊資料記錄相比),但應明白,可使用仵多不 同類型的本質上熟知的資料過據器1習此項技術者藉由 常規實驗可發現針對某一靜電集塵_供適於 件之快速更新的資料過濾器之設定。應明白,可利用許多 替代資料過濾器。較佳地,進行一品質評估以便賦予 資料記錄對數學模型更新之較高影響(與較不可靠資料相 比)。該品質評估可(例如)賦予已偵測程序擾亂期間已獲得 之資料έ己錄一較低權重。 上面已說明每當一新資料記錄變為可用時如何更新數學 129145.doc -26- 200900153Programs, etc.) + L Table In addition, the wording "mathematical model, in this description refers to the mathematical representation of a phenomenon. S “1"Effective electrostatic precipitator (ESP) l. Electrostatic precipitator 129129145.doc •15- 200900153 - for n.2 for flue gas 4 (which contains dust particles), and - for The outlet 6 of the flue gas 8 (most of which has been removed) has a casing 9 in which a first field, a second field 12, and a last field 14 are provided. In the art, as is well known in the art, for example, from U.S. Patent No. 4,5,2,872, the disclosure of which is hereby incorporated by reference in its entirety, each of the entire disclosures of The electrode and the collecting electrode (which is in the form of a collecting electrode plate). The last field provides a discharge electrode (Fig. Hf describes one of the discharge electrodes 16 in the straight line) and a collecting electrode plate (Fig. i only describes the collecting electrode plate (8). 20 applies a current between the discharge electrode 16 and the collector electrode plate. When the flue gas 4 passes through the thunderbolt, the dust particles are charged. The charged dust particles will travel toward the collector electrode plate 18. Collect dust particles at the collecting electrode (4). The electrostatic precipitator 1 provides a slap device, which is adapted to receive The collected particles are removed by the plate 18. The slap device 22 includes a first set of hammers that are adapted to tap the upstream end of the collector plate. A -4 is included in the first set of hammers The middle end is adapted to the upstream end of the 2-electrode plate 18. The slap device 22 also includes a second set of clocks that are adapted to slap the downstream end of the seven-eight collector plate. The second hammer 26:3 is in the second group of hammers of §Hai, and is adjusted to the downstream end of the plate 丨 8. The dust removal of the number of plates 8 can be carried out in different ways. The changeable " ''flow The situation 'that is, whether the power source 20 is "applying-current" at the electrode during the slap. It can also make the slap 8 states, instead of reducing the first A of the electric product, for example, the way of normal current strike, the beat can be... According to other alternatives, the current can be increased or decreased according to the other month (compared with the normal operation period I29145.doc -16 - 200900153). If the current is applied, the electrode plate is collected. Click 'The ability of the particles to adhere to the collector electrode plate 18 will be higher than the current without applying current during the slap Another parameter of the energy culture of the collector electrode plate 18 is whether the first hammer 24 and the second hammer 26 are used for the slap in the same situation, or whether the hammer 24 is used only to perform the slap. In addition, the number of occasions that the bells 24 and 26 slap the collector electrode plate 18 will affect the amount of dust collected in the collected dust particles that can be removed from the collecting electrode plate 18. The manner in which the electrode plate 18 is collected is to be slap-collecting the electrode plate 18 in such a manner as to have a quantity of dust particles removed from the collecting electrode plate 18 and also to be dispersed in the flue gas and with the dust-removed flue gas 8-Specific characteristics of the amount of dust particles (described below) leaving the electrostatic precipitator 1. The dust particles removed from the collecting electrode plate 18 by slap are collected and transported. 2 illustrates a control system 30 that includes a data receiver 32, a data processor 34, a computing device 36, and a slam control device %. For example, the dust concentration analyzer 4 of an opacity meter analyzes the dust particles in the dust-removed flue gas 8 that has passed through the last field 14 of the deer, dad/** on a continuous or periodic basis. concentration. The data receiver 32 receives information about the pellet emission from the analyzer 4. In the case where the data receiver 32 has received the analyzer from the analyzer 4, the data receiver 32 identifies the dust particles associated with a slap event. Information about the magnitude of the mother-dust particle emission peak and the time point at which the peak of the dust emission is seen is transmitted to the data processor 34. The data section 了 'The Ten Cooler 3 4 also receives information from the slam control device 38. The information from the slap and smash control device 38 and the execution of the individual shot 129145.doc 200900153, the point between the 阙 ° based on this information 'data processor 34 to make - dust particles peak (its caused by - slap The magnitude and self-hit: the time-corresponding _. Data Processor = II I!: Peak Formation - Data Recording - This will be explained below. The information contained in the mussel material is transferred from the data processor 34 to the device %. Computing device 36 prepares and/or updates a mathematical model. The wedge type is adapted to predict the peak of the emission caused by the slap shot based on a desired duration of the slap and the slap of the previous slap (eg, by a future slap One of the magnitudes of the peak of the future emission of dust particles. The mathematical model is forwarded to the control device 38. Based on the mathematical model, control device 38 determines a suitable time for the future slap, and - a suitable type of slap to perform. The control device 38 then self-ports and transmits a signal to the slap device 22 at the desired time point, and also to the power source 20 under the condition that the current is applied to the discharge electrode 16 and the collector electrode plate. 'To perform a desired type of slap. Therefore, the signals transmitted by the control device 38 may include which current should be applied by the power source 20 during the slap, and as to whether it should operate and how the library operates. - Motor 42 (which operates the first set of hammers 24), and whether it should operate and how the second motor 44 should be operated (the information of the second group of hammers that it operates). Whenever a new data record is obtained, the next dust particle is combined. _, the mathematical model can be updated. Therefore, the control system 3 provides automatic control of the time and manner of the slap in the final field to obtain a desired low dust emission peak. Figure 3 is described by the analyzer An example of the measurement data provided by 40. The gamma axis 129l45.doc -18- 200900153 r describes the opacity signal E (% of the maximum reading on the opacity meter) and the time T (minutes) on the X axis. Dust emission peak (which is described in the form of dust particle emission peak PMP2 in Fig. 3) corresponding to the last field slap from the collecting electrode plate 18. Therefore, when the slap is performed in the last field 14, the dust emission is increased to form The dust emission peaks PI and P2 are usually about 3 to 5 minutes. The first slap and the second slap usually have a low impact on the dust emission. The reason for this fact is that The slap of the field _ or the slap of the second field 12 causes one shot from the particular field, which has increased the emission of dust particles. However, the dust particles emitted during the first slap or the second slap It will be effectively collected by the collecting electrode plate of the last field 14. Therefore, the first field is slammed or the second field is slammed with the effect often by the last field 14 (the system is located in the first field 1G and the second correction Downstream) absorbed. However, when performing a slap in the final field 14, there is no downstream field that collects the dust particles released during the slap. The amount of dust particles emitted during the dust emission peaks P1 and P2 The fluctuation of the emission of dust particles from the electrostatic precipitator 1 has a large influence on average. The amount of dust released from the collecting electrode plate 18 of the last field U is related to the average fluctuation limit of the dust emission emitted by the authority. Depending on the country in which the electrostatic precipitator i is installed, the limit value may be (for example, a 6-minute fluctuation average or a 1-day fluctuation average. This portion of the dust emission caused by the dust particle emission peaks ρι, P2 described in Fig. 3 has a significant influence on the dust emission from the electrostatic precipitator k 'Especially for short-term fluctuations in dust emission, such as the average of fluctuations in 30 minutes and shorter time periods. For example, a mean value of -6 minutes from the peak of dust emission P1 will not be met. 129145.doc -19 - 200900153 Risk of emission limits for the authorities. It has been found that the amplitude M of the dust particle emission peaks P1, P2 is largely taken as the time elapsed since the slap immediately before the slap of the dust particle emission peak p. The extent of the dust particle emission peak (4) described in Fig. 3 therefore depends on the time t elapsed since the slap of the peak η of the dust particle emission. Therefore, the amplitude M of the dust emission peak value P2 caused by the "slap R" depends on the time t elapsed since the slap immediately before the slap r". ''Amplitude' should be understood as the measurement of the large h of the dust emission peak. Theoretically, the amplitude of the dust particle emission peak p2 is the area covered by the peak Ρ2. The rise and fall of the dust emission during the slap The manner in which each slap type has its own dust emission peak/曰, 'by the mechanical characteristics of the slap device 22, whether current is applied during the slap, etc., determines the "fingerprint". In fact, it is often accurate enough to approximate the magnitude of the dust emission peak Ρ2 by the height H of the dust particle emission peak 延伸 extending above a baseline dust particle Β. The dust particle emission near the baseline dust emission (4) is between the peak PI and Ρ2 (that is, when there is no slap in the last field 14). 4 schematically illustrates the amplitudes of the dust emission peaks PI, Ρ2, Ρ3, Ρ4, and Ρ5, H1, Η2, and the corresponding time t1, t2, which have elapsed since the previous slap, by a slap. Relationship between. The slap event is initially executed such that a time tl is durationd between the slap events R1, R2'. The slap events Rl, R2, and R3 respectively cause dust emission peaks 卩丨, p2, and p3, and the dust particle emission peaks P1, P2, and p3 each have a height corresponding to a height. Soon, the time spent in each slap event increased to time t2. Therefore, the slap event R4 and the slap event R5 are each executed after the time t2 has elapsed since the previous slap 129l45.doc -20-200900153 event. The slap events 114 and 115 respectively cause the dust particle emission peak P4 and the dust particle emission peak. The dust particle emission peaks P4 and P5 each have a height H2 which is much higher than the height H1 of the dust particle emission peaks p1 to p3. It has been found that the magnitudes of the heights HI, H2 expressed as dust particle emission peaks η to w depend on the time u, t2 that has elapsed since the slap event immediately before the slap event that caused the dust particle emission peak. Therefore, the peak of the dust emission caused by the slamming event ruler 4 is determined by the height H2 depending on the time u that has elapsed since the previous slamming event R3. Figure 5 depicts an example of a mathematical model based on The peak of the dust particle emission Η, and the measurement of the corresponding time t since the slamming event immediately before the slamming event that caused the peak of the dust emission. Two measurements have been made, which are described in In Figure 5, each measurement has resulted in a data record that includes the height H of the dust emission threshold and the time t since the previous slam event. In addition, a fictitious data record has been added, Is located near zero (real The peak value of the 丨% at the minute is). The fictitious data is recorded by the fact that the continuous slap of the collecting electrode plate 18 does not appear to be peak (because dust particles are not collected under such conditions). The time is the peak of the time since the previous slap. t 1 t (minutes) _ 0 ..... 1 I . 330 1 _ II .... 4300 Ο V/ __ III 11540 j / 85 Table 1: Record of the time and corresponding peaks since the previous slap. 129145.doc •21 - 200900153 It has been found that 'by the selected slap--the peak of the selected dust emission peak 自 and self-tightening The logarithm of the time that has elapsed since the slap of the selection of the dust particles that caused the selection of the dust particles is proportional to the number of bases. Therefore, the height of the bee value (H) is naturally correct, A curve fit is performed between the logarithms. The obtained equation is: H(t) = 7.2*ln(t[min])-5.6[〇/〇] (equation j)) Equation 1.1 is used as a mathematical model , the sentence of the sentence Yizi I have a description of the wrong by a selected shot f.: future slap) will cause - the selected dust emission peak (for example, The height H of the dust emission peak) can be determined based on the selected (four) (four) connected to the slap prior to the slap shot, and the timed learning model and appropriate conditions (eg, maximum license Γ) control device 38 can determine when Execution - slap between si. If, for example, the environmental rule is such that the peak of the dust emission peak is high (because the 6-minute two exceeds the risk), then the limit of the needle (four) solution is at t = e_] + 5.6. ) / 7.2 [minutes ] ^ by introducing Η = 50% into Equation 2 (Equation 2)) t = e〇〇W + 5,v,2rv ^ ^ ^^#,XTBffa1t: [刀刀]= 2350 [Minute] (Equation 22, since the previous slap has been _ " determined by the mathematical model), at the time of Cai Zhongzhong (four), he has borrowed a slap. The control device 38 can instruct the slap device 22 to perform a natural logarithmic function adapted to be between the gaze and the time between one of the slap and the slap and the previous slap. The 129145.doc -22- 200900153 relationship fact magnitude 成 is proportional to In (time t) by the following physical background: the longer the time t since the previous slap, the accumulation on the collecting electrode plate 18 The more dust particles there are. The more dust particles accumulated on the collecting electrode plate 18, the more dust particles will be released during the slap. However, as the time since the previous slap is increased, the dust particles will experience increased cohesion while collecting on the electrode plate 18. This cohesion compensates for the increase in the magnitude of the peak of the dust emission. The total effect of the longer time t since the previous slap will result in an increase in the amplitude of the dust emission peak, but the increase will be less than the viscosity of the dust particles on the collecting electrode plate as illustrated by a linear function The increase caused by the gathering. As an alternative to the natural logarithmic function, it is also possible (although sometimes poor) to utilize other logarithmic functions, as well as approximations of logarithmic functions. An approximation by a logarithmic function means, for example, a mathematical function similar to a logarithmic function, a trigonometric function, a piecewise linear curve fitting, and the like. Figure & illustrates an example of how to predict the height HF of a future dust particle emission peak PF due to a given time t from the previous slap event. . Figure 6b illustrates an example of how the time iF of the event R1 to be elapsed is predicted from Equation 2" based on a given height of a future dust emission peak pF. The mathematical model according to Equation 1.1 is based on only three data records plus fictitious data records. A mathematical model can also be obtained from only one or two data records plus the fictitious data record. Mathematics based on these data records 129145.doc -23- 200900153 :: Type can be regarded as a "starting model". However, the condition in the electrostatic dust collection m: 曰化'因&, if the mathematical model is not updated, the mathematical model may become unsuitable for the control of the slap. Or θ is used to adjust the conditions of the summer (such as the different types of fuels burned, etc., and is also used to improve the accuracy of the mathematical model when the operating conditions are stable, θ μ times, The new poor material record updates the mathematical model. Please - the flow chart 'describes the method by which the control system 3 works. In the step Α, the dust particle emission after the last field 14 is measured. Identification - peak system and last field 14 The slap event h is related. Any "peak" related to the calibration of the dust analyzer, etc. is ignored. In step B, the height of the bee value Pn is merged to the previous slap event from the last field μ (ie, the beat The time elapsed since the event Rn_〇 tN ° daytime tN indicates how long the collecting electrode plate 18 of the last field μ has been operating after the slamming event hi when the slap event Rn is executed. Time tN Forming a data record with the corresponding height Hn. In vC, a mathematical model is adapted for the data record. If the first time: step C, the two obtained since the start of the operation of the electrostatic precipitator 1 Or more information records A mathematical model is provided. If, on the other hand, a mathematical model is available, the mathematical model is updated with a new data record containing the post. In step D, 'based on the mathematical model control is to be executed - the slap N 1 The time of introduction is 1. The time is usually used for the control. This condition—the example—the height of the dust emission peak', does not exceed a certain value Hmax. Height Hn+i It is set as in the form, and is introduced into the mathematical model by 129145.doc -24- 200900153. 接! The receiver' is as described above with reference to Figure 5 and Equation 2,1 'calculation time tN + i. Sequence A, B , c, ^di^, has a loop, so that at the end of step D, /. will be 又»又=为N+1, and start step A, which is described in Figure 7. This is Ganzi-T Tian has When you slap the slap event, you will get a new data record, 2 and 3 take the measurement height of the peak of the dust particle emission and the corresponding time ^. The new-before material record can be used to update the mathematical model to make the mathematical model better than the prediction. The dust particle emission peak height h as a function of time t. Because of the loop 'cause This can continuously update the mathematical model such that the predicted dust particle emission peak height. More suitable for the white 'electrostatic precipitator 1 operating conditions may be two during operation: such changes include: collecting electrode plate 18 The dust collected on the second part: two: change, the change of the characteristics of the flue gas 4, the electrostatic precipitator 1: 'chemical 4, etc.. In view of such possible changes, when the mathematical model is updated in step C, it is suitable for the ^ model. Assign, ', filter state can (for example) update mathematics this side 4 (four) record - higher weight (compared to the old data record) the function of the data filter device ... very simple to obtain data over two 4 curve The fit (which forms the basis of the mathematical model) is already included in the new poor material record. Execute the curve anthropomorphic data imprinting ± four deep σ 刖 can discard the oldest while two two r: how to discard the oldest data record (data record t artificial 1v' and 1v,,) including new The data of 1v is the same as the one described in Table 1 ((Xinghe. The execution of the curve on the value of Table 2 is 129145.doc -25- 200900153 Μ%) The height of the value of i————— L 1 ~~~——___430〇__ ~~-__ 11540 ----J / 85 I 2350 | 4R ————'-. 2350 I" --- __48 T (minutes) II 111 IV, IV" Record. Based on the values in Table 2, a new curve fit can be performed and the updated mathematical model can be obtained: H (t) = 6. 9*ln (1)-2 2 ' (Equation 1.2) When another data record V When available, the data is recorded sub-use (10) and V"' simultaneously using only data records IV_ times, and data records are discarded before performing curve fitting and the like. Although Table 2 illustrates—a very simple method of transitioning data records, giving new data records a greater impact on the updated mathematical model (compared to the old data records), it should be understood that many different types of nature can be used. A well-known data filter device 1 can learn the setting of a data filter for a static electrostatic dust collection of a suitable component by routine experimentation. It should be understood that many alternative data filters are available. Preferably, a quality assessment is performed to give the data record a higher impact on the mathematical model update (as compared to less reliable data). The quality assessment may, for example, give a lower weight to the information that has been obtained during the disturbance of the detected program. How to update math whenever a new data record becomes available 129145.doc -26- 200900153

模型。依據一替代具體實施例,為數學模型添加偏項以允 許連續運作期間自動調整所利用的藉由-選定拍擊所造成 之k疋塵粒發射峰值之一幅度與介於該選定拍擊與其緊 接先前拍擊間之-時間之間的關係。基於各新資料記錄更 新該偏項,而非如此更新數學模型之核心。因&,經由該 偏項更新數學模型’且藉此在不改變基本關係之情況下對 :、力乂調整以適於實際運作條件。該偏項使數學模型在一 系列曲線間移動,但並不如此重新定義曲線之形狀。可藉 由利用以下形式之等式來實施該控制: 9model. According to an alternative embodiment, a bias term is added to the mathematical model to allow for automatic adjustment during continuous operation by utilizing one of the peaks of the k-dust emission peak caused by the selected slap and the tightness between the selected slaps The relationship between the time between the previous slaps and the time. This bias is updated based on each new data record rather than updating the core of the mathematical model. Because &, the mathematical model is updated via the partial term and thereby adjusting the force to suit the actual operating conditions without changing the basic relationship. This bias term causes the mathematical model to move between a series of curves, but does not redefine the shape of the curve. This control can be implemented by using an equation of the form: 9

Hpredictcd (t) = in (t) + biaSN (等式 3 1) 精由-《周整項(其係作為—塵粒發射峰值之測量與預測 幅度間之差加以計算)來更新該偏項: 、 (專式3·2) biasadjust = Hmeasured(t) . Hpredicted(t) 現在可藉由以下等式來更新該偏項: bias>j+i — bias^ + bias a- adjust (#^3.3) 在實際運作中,如上所句日日M, 上所說明藉由利用偏項的拍擊裝置22 之控制可在—控制區塊(其採用上述數學模型之微分)中加 以實施。在該控制區塊中’使用擬合曲線之斜率作為開始 偏移。由·#式1.1可導出72之级玄 导出7.2之斜率,且可將其 移。控制區塊將執行以下運作·· 节对偈 針對塵粒發射峰 (專式3.4) (等式3.5) 首先,基於選定峰值及緊接先前峰值 值高度Η及已歷時時間t計算差△ ·· ΔΗ = HN - Hn., Δί — ϊν - tjsj.] I29145.doc -27- 200900153 接著計算所需峰值高度變化,以便達到所需峰值高度 Hdesired · (專式3.6) (等式3.7) △Hrequired = Hdesired - HN 之後,若Δί不為零,則計算biaSnew : biasnew = ΔΗ / At 現在可更新偏移: biasN+1 = biasN * biasfilter + biaSnew * (i_biasfiIter)(等式 3 8) 接著可計算已歷時時間之所需變化: △^required = AHrequired / biaSN+1 (等式 3 9) 接著可從數學模型將下一已排程拍擊事件之時^點 計算為: 〜N+1 一 =tN +(等式 3.10) 最後,N = ,且再次以新資料記錄開始該程序。 ,視適於變化條件之較佳快速調適之 快速程度’通常將該因數設^為—在GuG8之範圍内之 值。該MaSfilier因數考量測量誤差、測量值之意外失常等 等。 圖8解說不同類型之拍擊的效應。上文已說明,可以不 同方式執行拍擊。例如,可藉由㈣㈣第—錘子准第 二錘子26,或藉由僅運作錘子24、%之一來執行拍擊。、在 ,中’RA表示僅採用第一錘子24之拍擊。各拍擊^導致 -具有高度出之塵粒發射峰值…以及⑴不過 用錘子24之拍擊可能導致未對 木対收集電極板18進行充分除 塵。因此’採用某也間隔热彡-、富 千一間隔執仃運作兩錘子24、%之拍擊 129145.doc •28- 200900153 灿。當執行第-RB類型之拍擊時,該拍_導致一非常 向的塵粒發射峰值P4(其具有高度H4),其係由於ra類型 之拍擊期間已累積於收集電極板】8上之某些塵粒得以釋放 ::實。當執行一第二RB類型之拍擊時,在其上無累積 火塵之收集電極板18上執行該拍擊,因此塵粒發射峰值p5 之南度H5係低於塵粒發射峰值p4之高度m。從圖8中會明 白’各拍擊間所歷時之時間係恆定的,為時_。藉由採 用RA拍擊類型之拍擊所獲得之峰、㈣藉由採 謂拍擊類型之拍擊所獲得之峰值p4、p5不同。此外, RA拍擊類型之拍擊之後直接執行一 rb拍擊類型之拍擊 時所獲得之塵粒發射峰值比另一仙拍擊類型之拍擊 之後直接執行-獅擊類型之拍擊時所獲得之塵粒發射 峰值P5高。為了考量此特性’較佳針對各拍擊類型採用一 特定數學模型,使得可針對各拍擊類型準確預測塵粒發射 峰值高度。因此,藉由圖8所描述之範例,可較佳地針對 RA拍擊類型之各拍擊採用—數學模型,並針對仙拍擊類 型之各拍擊採用另一數學模型。若一靜電集塵器i係經設 計用以採用一個以上類型之拍馨 I拍擎(例如,來自收集電極板 18之兩側之拍擊及僅來自收集電極板18之-側之拍擊), 則較佳地’該方法及該控制系統3〇係經調適用以相對於欲 執行拍擊類型選擇適當數學模型,及在計算執行下一該特 定類型之拍擊之前的欲歷時時間時應用該數學模型。各資 料記錄(其包含關於塵粒發射峰值高度H及已歷時時間= 資訊)可額外提供-第一標籤尺,其指示所執行之拍擊係何 129145.doc -29- 200900153 種類型。採用此第-標鐵R以便確保更新相關數學模型, 即對應於該特定拍擊類型之數學模型、 :射峰值Η之資料記錄較佳包含高㈣、時間 ==拍擊類_。此資料記錄係用以更新對應於 RB拍擊類型之該數學模型。 此外’較佳㈣整各數學模型以考量㈣歷史 所述拍擊之前的拍擊類型。較佳以該數學模型考量以下事 ^此-方式進行此一調整:藉由一 RA拍擊類型之= 在導致塵粒發射峰值P4之第一仙拍擊類型之拍擊 而=一RB拍擊類型之拍擊在導致塵粒發射峰值朽之第 拍擊類型之拍擊之前。為了使得可以考量歷史資 二各資料記錄較佳提供一第二標鐵。第二標鐵指示在緊 接先前拍擊事件下’或視需要在數個先前拍擊事件下,執 型的拍擊。有數個不同的可考量關於拍擊類型之 二史=的方法。一方法係針對一欲執行拍擊類型與該欲 :二:擊:前已執行的一拍擊類型之各組合採用一特定數 :二擊二一情況T,參考圖8’在之前為,拍擊類 型,:擊時將針對一 RB拍擊類型之拍擊利用—數學模 之則為另一 RB拍擊類型之拍擊時將針對一 _ 擊類型之拍擊利用另一數學模型。 行!::用某一種類的補償因數’其考量先前拍擊中所執 類型。例如,藉由對應於-RB拍擊類型之數學 拍擊Γ:算之塵粒發料值高度在先前拍擊事件為-RA 4之拍擊的情況下可增加(例如)5%,且在先前拍擊 129I45.doc •30· 200900153 為RB拍擊類型之拍擊的情況下可減少“列如)5%。因 此’ -說明塵粒發射峰值P4之資料記錄將較佳包含塵粒發 射高度H4、已歷時時間u、作為第一標籤的仙拍擊類型 之拍擊及作為第二標籤的—RA拍擊類型之拍擊在造成 峰值卩4之„亥拍擊之前之事實。此資料記錄係用以更新對應 於-仙拍擊類型之拍擊之數學模型,及補償一 ra拍擊: 型之拍擊在該rB拍擊類型之拍擊之前的事實。 °依據所述國豕中在使用之發射標準來設定控制震置3 8 扛制拍擊所處之條件。最後場14之後之塵粒之發射限制可 (Η )為1〇 mg/Nm乾氣(其係作為6分鐘波動平均,或作為 一天波動平均)。因此’通常存在-預設波動平均限制 值,^要相對於該預設波動平均限制值來控制拍擊。例 如’採用一不透明度計時的實際波動平均值可計算為: g—average (等式4 A ) 其中η係波動平均週期期間(例如,6分鐘期間或一天 取樣點數。基於已測量基線塵粒發射(即,兩個拍 ^事件間之塵粒發射)之知識,在藉由—拍擊所造成之一 塵粒發射夺值將在6分鐘一 〆 天之週期期間出現的條件 大::模擬將產生哪一波動平均。基於此模擬,可決定 塵粒發射峰值幅度,例如最大塵粒發射峰值高 又置此類最大塵粒發射峰值高度作為—輸人輸入至控制 塵鄉射Γ更控制農置38可基於數學模型以避免超過最大 χ值间度之塵粒發射峰值的此—方式控㈣電集 I29145.doc 200900153 塵盗1之最後場14之拍擊。因此,意指控制裝置38藉由控 制一拍擊與一將來拍擊間之欲歷時之時間、及/或應執行 之拍擊類型來控制拍擊。 圖9解說依據一替代具體實施例的一靜電集塵器I"。靜 電集塵器101之設計係類似於上文已說明之靜電集塵器】之 設計。控制系統丨30包含一計算裝置136、及一拍擊控制裝 置138(其係可運作以起始靜電集塵器101之最後場114中之 拍擊)。拍擊控制裝置138控制拍擊期間最後場之電流 f月況,即電源120是否在電極(圖9未顯示)間施加一電流。 此外,拍擊控制裝置138亦控制一拍擊裝置122進而控制是 否應運作及應如何運作第一馬達〗42(其運作第一組錘子(圖 9未顯示))、及是否應運作及應如何運作第二馬達144(其運 作第二組錘子(圖9未顯示))。 計算裝置具有PID控制器136之形式且係可運作以決定拍 擊控制裝置138何時應起始最後場114中之拍擊。pm控制 器以從塵粒濃度分析器14〇接收資訊。可(例如)為^透 明度計的塵粒分析器140在連續或週期性基礎上分析已穿 過最後場U4之已除塵煙道氣8中之塵粒之濃度。關於已測 量不透明度(即 拍擊所造成之一塵 藉由最後場114中之— 分析器140發送至 粒發射峰值幅度 粒發射峰值之測量幅度)的資訊係從塵粒 PID控制器1 36(其比較該測量幅度與—塵 目標值)。㈣控制器136必要時相應地調整指示拍擊控制 裝置138執行最後場114之收集電極板之另—拍擊之前的欲 歷時之時間。因此PID控制器136用於自動追蹤該已歷時時 129M5.doc -32- 200900153 ::塵目::二導致—儘可能接近塵粒發射峰值幅“標 值的壓粒發射蜂值之幅唐1 〜厪)利用藉由一選定拍擊所造赤 之一選定塵粒發射峰值之一幅 成 接先前拍擊間之—時…/:、…選定拍擊與其緊 單間之日寺間之間存在一關係的事實 ^控制器136提供何時應執行拍擊之自動控制以便獲得_: 2塵=射峰值之幅度。應明白,該仙控制器】%利用 «-選U擊所造叙—以塵粒發射 於該選定拍擊與1緊接亦俞舳教叫 化度與;丨 Μ在w 擊1之—時_之間存在一 \ ,而不利用表示該關係之實際數學模型。因 2 ’ β亥PID控制器可以說成係依據一無模型演算法運作。 #代控制器類型(包括ΡΙ控制器、及無模型適應 亦可用以控制最後場之拍擊,且亦依據-無模型演算法運 ::更高級控制器可具有與控制執行拍擊之前之= «或代替控制執行拍擊之前之時間,控制拍擊控制裝置 138應執行哪一類型之拍擊的其他功能。 應明白,在所附申請專利範圍之範轉内可以有上面說明 之具體實施例之許多變化。 :列如,上面已說明控制系統3〇可利用數學模型來決定自 :接先前拍擊以來已歷時某一時間之後的預期峰值高度, 或決定為了獲得某-高度之塵粒發射峰值欲料之時間。 應明白’亦可採用其他控制策略。例如,可以調適控制裝 ㈣以進行迭代計算而獲得—欲歷時之時間與欲採用拍擊 韦序列’該序列提供低塵粒發射。該序列可作為範例 類似於圖8所描述之序列。 I29I45.doc -33· 200900153 工又匕詋明 仃柏 類型之拍擊器’例如採用所謂磁脈衝重力撞擊 稱為刪拍擊器)’來執行拍擊。另一可能性:(亦 組鍾子’例如僅採用錘子24,藉此僅拍擊收集電此 一側。 心 :文已說明,數學模型採用一關係’在該關係中塵粒笋 射峰值之高度係與自緊接先前拍擊以來所歷時之時 數(特定言之自,然對數)成正比。應明白可採用其他數學模 型類型。例如,在某些情況下為資料記錄適配'線性模 型、或-指數模型可能會足夠準確,尤其在資料記錄盘相 關運作範圍關於自緊接先前拍擊以來所歷時之時間係指一 相當窄範圍的條件下。 ' 上文已說明,塵粒發射峰值之高度H常常係塵粒發射峰 值之幅度的良好近似值。作為峰值高度H之替代,亦可藉 由其他數量(例如塵粒發射峰值之面積等等)來表示塵粒發 射峰值之幅度。 又 上文已說明,較佳採用一獨立數學模型來預測各拍擊類 型之峰值高度。應明白,若發現某些拍擊類型之峰值高度 係類似的,則此等拍擊類型可使用相同數學模型。例如, 右發現僅採用第一組錘子24之拍擊提供與僅採用第二組錘 子26之拍擊類似的峰值高度,則此等兩個拍擊類型可利用 相同數學模型。 如上所說明,常常較佳地控制最後場14中將要執行—拍 擊之前的欲歷時之時間◦不過,亦可運作固定次數以執行 129I45.doc •34- 200900153 拍擊,例如每天在固定鐘點執行拍擊—二欠或兩次。在此一 情況下,控制系統30可基於用於不同拍擊類型之數學模型 ㈣欲執行之哪種拍擊類型以便避免大塵粒發射峰值,、且 仍g理以避免灰塵隨時間累積於收集電極板1 8上。如上所 說明’常常較佳地使控制系統3()控制將要執行一拍擊之前 欲歷時之時間、及欲執行之拍擊類型。 雖然上文已說明該控制系統3〇及該方法係用以控制何時Hpredictcd (t) = in (t) + biaSN (Equation 3 1) Refinement - The whole term (which is calculated as the difference between the measured and predicted amplitude of the dust emission peak) is used to update the partial term: (Special Formula 3·2) biasadjust = Hmeasured(t) . Hpredicted(t) The partial term can now be updated by the following equation: bias>j+i — bias^ + bias a- adjust (#^3.3) In actual operation, as described above, the control of the slap device 22 using the partial term can be implemented in the control block (which uses the differential of the above mathematical model). In the control block, the slope of the fitted curve is used as the starting offset. From ##1.1, you can derive the level of 72. The slope of 7.2 is derived and can be shifted. The control block will perform the following operations: • Pairing the dust emission peak (Special Formula 3.4) (Equation 3.5) First, calculate the difference based on the selected peak value and the height of the previous peak value and the elapsed time t. ΔΗ = HN - Hn., Δί — ϊν - tjsj.] I29145.doc -27- 200900153 Then calculate the desired peak height change to reach the desired peak height Hdesired · (Special 3.6) (Equation 3.7) △Hrequired = After Hdesired - HN, if Δί is not zero, then calculate biaSnew : biasnew = ΔΗ / At Now the offset can be updated: biasN+1 = biasN * biasfilter + biaSnew * (i_biasfiIter) (Equation 3 8) Then you can calculate the duration The required change in time: △^required = AHrequired / biaSN+1 (Equation 3 9) Then the time from the mathematical model to the next scheduled slap event is calculated as: ~N+1 ==== (Equation 3.10) Finally, N = and start the procedure again with the new data record. The speed of the preferred rapid adaptation to the changing conditions is typically set to a value within the range of GuG8. The MaSfilier factor takes into account measurement errors, accidental aberrations of measured values, and the like. Figure 8 illustrates the effects of different types of slaps. As explained above, the slap can be performed in different ways. For example, the slap can be performed by (4) (4) the first hammer, the second hammer 26, or by operating only one of the hammers 24, %. , at , 'RA indicates that only the first hammer 24 is used for the slap. Each slap ^ results in - having a height of the dust emission peak... and (1) but the slap with the hammer 24 may result in the raft collecting electrode plate 18 not being sufficiently dusted. Therefore, the use of a certain interval of enthusiasm -, the rich one thousand intervals to operate two hammers 24,% of the slap 129145.doc • 28- 200900153 Can. When the slap of the -RB type is performed, the beat_ results in a very large dust emission peak P4 (which has a height H4) which is accumulated on the collecting electrode plate during the slap of the ra type. Some dust particles are released: true. When a second RB type slap is performed, the slap is performed on the collecting electrode plate 18 on which no accumulated dust is accumulated, so that the southmost H5 of the dust particle emission peak p5 is lower than the height of the dust emission peak p4. m. It will be clear from Fig. 8 that the time elapsed between the slaps is constant, and is _. The peaks obtained by the slap of the RA slap type are used, and (b) the peaks p4 and p5 obtained by the slap of the slap type are different. In addition, after the slap type of the RA slap type directly performs a rb slap type slap, the dust particle emission peak obtained is directly executed after the other slap slap type slap - the lion strike type slap The obtained dust particle emission peak P5 is high. In order to consider this characteristic, it is preferable to use a specific mathematical model for each type of slap, so that the peak height of the dust emission can be accurately predicted for each slap type. Thus, with the example depicted in Figure 8, it is preferred to employ a mathematical model for each slap of the RA slap type and another mathematical model for each slap of the slap type. If an electrostatic precipitator i is designed to employ more than one type of slap I (for example, slap from both sides of the collecting electrode plate 18 and slap only from the side of the collecting electrode plate 18) Preferably, the method and the control system 3 are adapted to select an appropriate mathematical model relative to the type of slap to be performed, and to apply the time duration prior to the calculation of the next slap of the particular type of application. The mathematical model. Each data record (which contains the peak height H of the dust emission and the elapsed time = information) can be additionally provided - a first label ruler indicating which type of slap is performed 129145.doc -29- 200900153 types. This first-standard iron R is used to ensure that the relevant mathematical model is updated, that is, the mathematical model corresponding to the specific type of slap, the data record of the peak value 较佳 preferably contains high (four), time == slap type _. This data record is used to update the mathematical model corresponding to the RB tap type. In addition, the mathematical model is better (four) to consider the type of slap before the slap as described in (4) History. Preferably, the mathematical model considers the following: this method is performed by: an RA slap type = slap in the first slap type that causes the dust particle emission peak P4 = RB slap The type of slap is before the slap of the type of slap that causes the peak of the dust emission. In order to make it possible to consider the historical data, it is better to provide a second standard. The second indicator indicates a successful slap under the previous slamming event or as needed for several previous slamming events. There are several different ways to consider the second history of the type of slap. One method is for a type of slap to be executed and the desire: two: slap: each combination of a slap type that has been executed before adopts a specific number: two strikes, a case T, with reference to FIG. 8' before Type of hit: When hitting, it will be used for the slap type of one RB slap type—the math model will use another mathematical model for the slap of one slap type when slap of another RB type. Row! :: Use a certain type of compensation factor' to consider the type of the previous slap. For example, by a mathematical slap corresponding to the -RB slap type: the calculated dust particle height can be increased (for example) by 5% if the previous slap event is a slap of -RA 4 The previous slap 129I45.doc •30· 200900153 can reduce the “column” 5% for the slap type slap. Therefore, the data record of the dust emission peak P4 will preferably contain the dust emission height. H4, the elapsed time u, the slap of the slap type as the first tag, and the slap of the RA slap type as the second tag before the slap of the peak 卩4. This data record is used to update the mathematical model corresponding to the slap type of the slap slap type, and to compensate for the fact that a rabe is the type of slap before the slap of the rB slap type. ° According to the emission standard used in the country, the conditions for controlling the shock 3 扛 slap are set. The emission limit of the dust particles after the last field 14 may be (〇) 1 〇 mg/Nm dry gas (which is a 6-minute fluctuation average, or as a one-day fluctuation average). Therefore, there is usually a preset fluctuation average limit value, and the tap is controlled relative to the preset fluctuation average limit value. For example, the actual fluctuation average using an opacity count can be calculated as: g—average (Equation 4 A ) where η is the average period of the fluctuation period (for example, 6 minutes or one day of sampling points. Based on measured baseline dust particles The knowledge of the launch (ie, the emission of dust particles between two beat events), one of the conditions that occurs during the 6-minute day period by one of the dust-emissions caused by the slap: large: Based on this simulation, the peak amplitude of the dust emission can be determined. For example, the peak of the maximum dust emission is high and the peak height of the maximum dust emission is set as the input to the control of the dust. The set 38 can be based on a mathematical model to avoid the slap of the last field 14 of the dust thief 1 of this dust-like emission peak exceeding the maximum enthalpy interval. Therefore, the control device 38 borrows The slap is controlled by controlling the time between the slap and a future slap, and/or the type of slap to be performed. Figure 9 illustrates an electrostatic precipitator I" in accordance with an alternate embodiment. The design of the dust collector 101 is similar to that of the electrostatic precipitator described above. The control system 30 includes a computing device 136 and a slam control device 138 (which is operable to initiate electrostatic precipitator) The slap control device 138 controls the current f month condition of the last field during the slap, that is, whether the power source 120 applies a current between the electrodes (not shown in Fig. 9). The control device 138 also controls a slap device 122 to control whether it should operate and how the first motor 42 should be operated (which operates the first group of hammers (not shown in Figure 9)), and whether it should operate and how the second motor should operate. 144 (which operates a second set of hammers (not shown in Figure 9)). The computing device is in the form of a PID controller 136 and is operable to determine when the slam control device 138 should initiate a slap in the last field 114. pm control The information is received from the dust concentration analyzer 14A. The dust particle analyzer 140, for example, a transparency meter, analyzes the dust-removed flue gas 8 that has passed through the last field U4 on a continuous or periodic basis. The concentration of dust particles. About the measured The amount of opacity (i.e., the amount of dust caused by the slap by the last field 114 - the amplitude of the particle emission peak amplitude of the particle emission peak sent by the analyzer 140) is from the dust particle controller 1 36 (comparison The measurement amplitude and the dust target value. (4) The controller 136 adjusts, as necessary, the time required to indicate the slap control device 138 to perform another slap of the collecting electrode plate of the last field 114. Therefore, the PID controller 136 Used for automatic tracking of the time 129M5.doc -32- 200900153: dust:: two leads - as close as possible to the peak of the dust emission peak "the value of the granule emission of the bee value of the Tang 1 ~ 厪) use The fact that one of the peaks of the dust emission selected by one of the selected slaps is selected to be connected to the previous slap-time.../:,...There is a relationship between the selected slap and the day between the temples ^ The controller 136 provides when the automatic control of the slap should be performed in order to obtain the magnitude of the _: 2 dust = shot peak. It should be understood that the controller of the immortality] uses the «-selected U-striking----------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------- There is a \ between them, without using the actual mathematical model that represents the relationship. Because the 2' β Hai PID controller can be said to operate according to a model-free algorithm. #代控制器 type (including ΡΙ controller, and no model adaptation can also be used to control the final field slap, and also based on - no model algorithm:: The advanced controller can have the control before the execution slap = «Or alternatively to controlling the time before the slap is performed, the control slap control device 138 should perform other functions of which type of slap. It should be understood that the specific embodiments described above may be within the scope of the appended claims. Many variations. : As shown above, the control system 3 can be used to determine the expected peak height after a certain time since the previous slap, or to determine the dust emission in order to obtain a certain height. The peak time is expected. It should be understood that other control strategies can also be used. For example, the control device (4) can be adapted for iterative calculations to obtain the time and the desire to use the slap protocol sequence to provide low dust emission. This sequence can be used as an example similar to the sequence described in Fig. 8. I29I45.doc -33· 200900153 The slapper of the cypress type is used for example, so-called magnetic Red is heavy impact referred slap deleted) 'slap performed. Another possibility: (also set the clock 'for example, only the hammer 24 is used, so that only the side of the slap is collected by the slap. Heart: The text has stated that the mathematical model adopts a relationship 'the peak of the dust shot in the relationship The height is proportional to the number of hours since the previous slap (specifically, the logarithm). It should be understood that other mathematical model types can be used. For example, in some cases, the data record is adapted to 'linear. The model, or -index model may be sufficiently accurate, especially in the context of the relevant operating range of the data record disc for a relatively narrow range of time since the previous slap. ' As explained above, dust emission The height H of the peak is often a good approximation of the magnitude of the peak of the dust emission. As an alternative to the peak height H, the magnitude of the peak of the dust emission can also be represented by other quantities (such as the area of the peak of the dust emission, etc.). As explained above, an independent mathematical model is preferably used to predict the peak height of each type of slap. It should be understood that if the peak heights of some types of slaps are found to be similar, then slaps The same mathematical model can be used for the type. For example, the right finds that only the slap of the first set of hammers 24 provides a peak height similar to that of the second set of hammers 26, then the two slap types can utilize the same mathematics. Model. As explained above, it is often better to control the time in the last field 14 to be executed - the time before the slap, but it can also be operated a fixed number of times to perform the 129I45.doc •34-200900153 slap, for example, fixed every day. The hour is performed by slap-two owing or twice. In this case, the control system 30 can be based on a mathematical model for different types of slaps (4) which type of slap is to be performed in order to avoid large dust emission peaks, and Still avoiding the accumulation of dust over time on the collecting electrode plate 18. As explained above, it is often preferred to have the control system 3() control the time it takes to perform a slap and the type of slap to be performed. Although the control system 3 and the method have been described above to control when

及/或如何執行一拍擊,但亦可利用該控制系統取/或該 方法來預測某—已歷時時間之塵粒發射峰值之幅度,或預 測獲得某-幅度之塵粒發射峰值之前之時間。此類資訊可 :於靜電集塵器之開發與設計中,及靜電集塵器之啟用 中0 上又已說明一更新數學模型 』 〜月π〜平丨tf,j C冽重貢料 δ己錄更新模型,及賦予 、 4㈣—較大權重(與較 —己錄相比)。應明白,存在其他更新模型之方法。 二::法=一或多個"桶"中收集資料記錄。從此-中才δ取 > 料記錄以更新數聲摄刑 7 t f 載條件利用一 ”桶,,"广可以針對全負 =於低負載條件。若(例如)欲更新模型以與半負載條件 資料,一Μ 負载條件之條件)有關之 學模型:含?類資料之η桶”中收集且可用以更新數 相關爲礎以:A將提供一用以在半負载條件下控制拍擊的 TO基·礎。因此,琴丨丨4 情庫… 3 _包含貧料記錄之-來源、或”記 庫’㈣可拾取合《料記錄以相對於本運作條件製 129M5.doc •35· 200900153 備或更新一相關數學模型。 t ' 新貝枓5己錄係放置於相關"桶” 且可取代该相同,,桶"之舊資料 南 剛剛載入之運作停件;^ π t 拥U、田然可與 “ 不同的其他運作條件有關)之使用你 加模型之準確度,因為 ’關)之使用增 模型,來相關”桶”之資料記錄更新 棵S ’因此並不藉由盥另^ 丨 ^ m /、另—運作條件類型有關的大量資料 §己錄來偏移該模型。 里貢枓 上文已說明,控制糸1 '、、、先30可用以控制靜電集塵琴1之喿 後場14之拍擊,及/或 罕塵器1之最 4+ , 頂州果自靜電集塵器1之塵粒發 二:制系統30可為一獨立控制系統,或可整合於控 制整個燃燒設備之運相總體㈣電財。另-可能非常 ^引力(尤其當預測塵粒之發射時)的選項係使用袖 冰如 次個人數位助理(PDA)作為控制系 、’。此—情況下,只是將該數學模型程式化於所述裝置 中,'而使用該裝置之微處理器作為資料處理器34,該裝 置可接著用作一用以進行來自靜 測的手持卫具。以自靜電集塵K塵粒發射之預 【圖式簡單說明】 已筝考附圖更詳細地說明本發明,其中: 圖1係一斷面圖,且解說一靜電集塵器。 圖2係-側視圖,且解說該靜電集塵器及—控制系統。 圖3解說所測量之塵粒發射峰值的圖式。 圖4解說塵粒發射峰值之示意圖。 圖5解說—模型之—範例,其制藉由-選定拍擊所造 成之塵粒發射峰值高度對自緊接先前拍擊以來所歷時之時 129145.doc -36- 200900153 之一高度 圖6a係解說如何決定— 疋將來塵粒發射峰值 …一 圖6b係解說執行一將來此 ?日擎之刖之欲歷時之時間的決 圖7解說控制最後場 ^ _ 你牮之方法的流程圖。 圖8係一示意圖,且解 粒發射峰值。 藉由不同拍擊類型所獲得之塵 =係-側視圖’且解說依據—替代具體實施例的一靜 電集塵器及一控制系統。 【主要元件符號說明】 1 靜電集塵器 2 入口 4 煙道氣 6 出口 8 煙道氣 9 外殼 10 第一場 12 第二場 14 最後場 16 放電電極 18 收集電極/收集電極板 20 電源 22 拍擊裝置 24 第一鐘子 129145.doc •37- 200900153 ί 26 第二錘子 28 漏斗 30 控制系統 32 資料接收器 34 資料處理器 36 計算裝置 38 拍擊控制裝置 40 塵粒濃度分析器 42 第一馬達 44 第二馬達 101 靜電集塵器 114 最後場 i 120 電源 122 拍擊裝置 130 控制系統 136 計算裝置/PID控制器 138 拍擊控制裝置 140 塵粒濃度分析器 142 第一馬達 144 第二馬達 129145.doc -38-And/or how to perform a slap, but the control system can also be used to/or predict the magnitude of the peak of the dust emission over a certain period of time, or the time before the peak of the dust emission of a certain amplitude is predicted. . Such information can be: in the development and design of electrostatic precipitators, and in the activation of electrostatic precipitators, an updated mathematical model has been described. ~月π~平丨tf,j C冽重贡料Record the updated model, and give, 4 (four) - a larger weight (compared with the comparison - recorded). It should be understood that there are other ways to update the model. Two:: Law = one or more "bucket" in the collection of data records. From this - only δ 取 取 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料 料Conditional data, a condition of the load condition) related learning model: η bucket containing data, and can be based on the update number correlation: A will provide a control slap under semi-load conditions TO base. Therefore, the Qinqin 4 love library... 3 _ contains the poor material record - source, or "repository" (four) can pick up the material record in relation to the operating conditions 129M5.doc •35· 200900153 prepare or update a related Mathematical model. t 'New Bellow 5 has been placed in the relevant "bucket" and can replace the same, the old data of the barrel" is just loaded into the operation stop; ^ π t U, Tian Ran can The use of the model is related to the accuracy of the other operating conditions. Because the 'off' is used to increase the model, the relevant "bucket" data record updates the tree S 'and therefore does not rely on 盥^ 丨^ m / And a large amount of information related to the type of operating conditions § has been recorded to offset the model. Ligong 枓 has explained above, control 糸 1 ',,, first 30 can be used to control the electrostatic field dust 1 after the field 14 Strike, and / or the most 4+ of the dust collector 1 , Dingzhou fruit from the dust collector of the electrostatic precipitator 1: the system 30 can be an independent control system, or can be integrated into the control of the entire combustion equipment Overall (four) electricity. Another - may be very gravitational (especially when predicting the emission of dust particles) The item uses sleeve ice, such as the secondary personal digital assistant (PDA), as the control system, '. In this case, the mathematical model is only programmed into the device, and the microprocessor using the device is used as the data processor. 34, the device can then be used as a hand-held harness for performing static measurements. The invention is described in more detail in the pre-supplement of the self-electrostatic dust collection K dust particles. Figure 1 is a cross-sectional view of an electrostatic precipitator. Figure 2 is a side view and illustrates the electrostatic precipitator and control system. Figure 3 illustrates a plot of measured dust particle emission peaks. Figure 4 illustrates a schematic diagram of the peak emission of dust particles. Figure 5 illustrates an example of a model that produces a peak height of the dust emission caused by a selected slap for the time since the previous slap. 129145.doc -36- 200900153 One height map 6a explains how to decide - 疋 the peak of dust emission in the future... Figure 6b shows the execution of a future. The time of the day of the engine is determined. Figure 7 illustrates the last field of control ^ _ The flow chart of your method. 8 is a schematic diagram, and the granulating emission peak. The dust obtained by different slap types = side view 'and the explanation basis - instead of an electrostatic precipitator and a control system of the specific embodiment. Description] 1 electrostatic precipitator 2 inlet 4 flue gas 6 outlet 8 flue gas 9 housing 10 first field 12 second field 14 last field 16 discharge electrode 18 collecting electrode / collecting electrode plate 20 power supply 22 slap device 24 One clock 129145.doc •37- 200900153 ί 26 Second hammer 28 Funnel 30 Control system 32 Data receiver 34 Data processor 36 Calculation device 38 Slam control device 40 Dust particle concentration analyzer 42 First motor 44 Second motor 101 electrostatic precipitator 114 final field i 120 power supply 122 slap device 130 control system 136 computing device / PID controller 138 slam control device 140 dust particle concentration analyzer 142 first motor 144 second motor 129145.doc -38-

Claims (1)

200900153 十、申請專利範圍: ι_ -種控制來自一靜電集塵器⑴之塵粒發射的方法,該靜 電集塵器⑴具有一最後場(14),該最後場(14)係提供放 電電極(16)、收集電極(18)、及一拍擊裝置(22),該拍擊 裝置C 2)係ί周適用以藉由拍擊該等收集電極(1 8)來為 其除塵, 其係特徵化為以下步驟 )利用藉由選疋拍擊所造成之一選定塵粒發射峰 值之-幅度(H)與介於該選定拍擊與其緊接先前拍擊間之 一時間⑴之間的一關係,及 ϋ)基於該關係’調整選自以下群組之至少一參數: 該最後場(14)中將要執行一拍擊之前的該欲歷時之時間 ⑴’及该最後場(14)中欲執行之拍擊類型。 2·如請求項1之方法,該步驟ii)進一步包含 計算波動平均值,t久# 塵粒發射,及各對應於-預設週期期間之平均 3. 基於β亥關係’相對於一預今、'古叙正 後場(―集電極u㈣㈣ϋ值調整該最 如請求項1至2中任一項之方 識別欲採用該拍擊類型在°亥步驟0中, 便在步—此ii定::::_以 藉由一選定拍擊所造成之一選 寺疋杈型係 (Η)與介於已識別特定拍擊類型之該選一幅度 前拍擊間之該時間⑴之間之該關係的—模型。〜、緊接先 129145.doc 200900153 4. 5· 如請求項1至2中任一項之方 丹Τ,在該步驟i)中, 當利用藉由一選定拍擊所造成— 战< 選疋塵粒發射峰值之 一幅度(H)與介於該選定拍擊 、八緊接先刖拍擊間之一時 間⑴之間的該關係時,識別並 可里《亥選疋拍擊之前所執 行之拍擊類型,該緊接先前 、 叫罕您頒型已加以識別。 如6月求項1至2中任' —項之太、+.. . 貝之方法,其中藉由下面的式子來 表示藉由一選定拍擊所造成之一 遠疋塵粒發射峰值之一 幅度(H)與介於該選定拍擊盥豆豎 相罕,、具緊接先前拍擊間之該時間 ⑴之間的該關係: 幅度(H)〇c函數(時間⑴), 其中從以下函數中選擇該函數: 對數函數,及 對數函數之近似值, 該函數較佳為一自然對數函數。 6·如請求項!至2中任-項之方法,其中藉由以下步驟來獲 得藉由一選定拍擊所造成之一選定塵粒發射峰值之一幅 度(H)與介於該選定拍擊與其緊接先前拍擊間之該時間 (t)之間之一關係的一數學模型 A) 測量該最後場(14)之後之該塵粒發射以識別與該最 後場(14)之至少一收集電極(18)之拍擊(R2 ; R4)有關的 塵粒發射峰值(P2 ; P4), B) 使該等塵粒發射峰值(P2 ; P4)之每一者之測量幅度 (HI ; H2)與自該最後場(14)之該至少一收集電極(18)之 緊接先前拍擊(Rl ; R3)以來所歷時之對應時間(u ; t2)耦 129145.doc 200900153 。以便形成育料記錄’各此類資料記錄包含該塵粒 峰值(P2,P4)之該幅度(H1 ; H2)及自該緊接先前拍擊 (R1,R3)以來所歷時之該對應時間⑴;⑺,及 C)基於該等資料記錄’製備藉由一選定拍擊所造成 之‘定塵粒發射峰值之一幅度(H)與介於該選定拍擊與 其緊接先前拍擊間之該時_之間之—關係的該模型。、 7. 如請求項6之方法,該步_進一步包含在各資料記錄 中G括第一標籤,其指示獲得該所述塵粒發射峰^ (二)時所採用之該拍擊類型,該步驟〇進一步包含依據 名第払籤針對各拍擊類型製備一拍擊類型特定模型。 8. 如請求項7之方法,該步驟B)進一步包含在各資料記錄 中包括一第二標籤,其包含與該資料記錄之該幅度、時 間及第-標籤有關之該拍擊之前所騎之該特定拍擊類 型的有關歷史資訊,該步驟❼進—步包含在各該拍擊類 型特定模型中考量該歷史資訊。 、 9· 士明求項1至2中任一項之方法,其中藉由以下步驟來更 新藉由璉疋拍擊所造成之一選定塵粒發射峰值之一幅 度(H)與介於該選定拍擊與其緊接先前拍擊間之該時間 (t)之間之一關係的一數學模型 eD)測量該最後場⑽之後之塵粒發射以識別與該最後 場(1 4)之至少—收集電極(1 8)之—拍擊㈣有關的一塵粒 發射峰值, E)使該塵粒發射峰值(p5)之測量幅度旧2)與自該最後 場(14)之該至少—收集電極(18)之緊接先前拍擊㈣以來 129145.doc 200900153 所歷時之對應時間(t2)耦合以便形成一資料記錄,此類 負料°己錄包含該塵粒發射峰值(P5)之該幅度(H2)及自該 緊接先則拍擊(R4)以來所歷時之該對應時間(t2),及 F)基於該資料記錄,更新藉由一選定拍擊所造成之 t疋塵粒發射峰值之一幅度(H)與介於該選定拍擊與其 緊接先前拍擊間之該時間⑴之間之一關係的該數學模 型。 ' 1〇·如凊求項9之方法,該步驟E)進一步包含在各資料記錄 中包括一第一標籤,其指示獲得該所述塵粒發射峰值時 所知用之該拍擊類型,該步驟F)進一步包含更新對應於 藉由忒第一標籤所表示之該拍擊類型的一拍擊類型特定 數學模型。 η·如請求項10之方法,該步_進一步包含在各資料記錄 中包括-第二標籤,纟包含與該資料記錄之該幅度、時 門及第標籤有關之拍擊之前所執行之該特定拍擊類型 的有關歷史資訊,該步㈣進—步包含更新藉由一選定 拍擊所^成之一選定塵粒發射峰值之一幅度(Η)與介於該 選疋拍擊與其緊接先前拍擊間之該時間⑴之間之 的該數學模型時考量該歷史資訊。 ’、 12.如請求項9之方法,其中步驟F)期間更新該數學模 用一資料過濾器。 、 13.如凊求項1之方法,其中基於該關係,調整選自以下 組之至少一參數:該最後場(14)中將要執行—拍擊义 的該欲歷時之時間⑴,及該最後場(14)中欲執行之I:: 129145.doc 200900153 擊類型’的該步驟係藉由以下步驟來執行: 測量藉由該最後場(14)之該等收集電極(18)之至少一 收集電極之拍擊所造成之一塵粒發射峰值之該幅度, 將關於該塵粒發射峰值之該測量幅度的資訊發送至一 計算裝置(136), 該計算裝置(136)比較該塵粒發射峰值之該測量幅度與 一塵粒發射峰值幅度目標值,及200900153 X. Patent application scope: ι_ - A method for controlling the emission of dust particles from an electrostatic precipitator (1) having a final field (14) which provides a discharge electrode ( 16) a collecting electrode (18) and a slap device (22), wherein the slap device C 2) is adapted to be dusted by slapping the collecting electrodes (18), the characteristics of which are Turning to the following step: using a relationship between the amplitude (H) of the selected dust emission peak caused by the selective slap and the time (1) between the selected slap and the previous slap And ϋ) based on the relationship 'adjusting at least one parameter selected from the group consisting of: the last field (14) is to perform a time (1)' before the slap and the last field (14) is to be executed The type of slap. 2) The method of claim 1, wherein the step ii) further comprises calculating a mean value of fluctuations, t-times of dust particles, and an average corresponding to a period of -predetermined period 3. Based on the relationship between β and Hai , '古叙正后场(-collector u(4)(4) ϋ value adjustment. The party that most of the requirements of items 1 to 2 is identified to use the slap type in step 0, then in step - this ii:: ::_ to select the relationship between the selected temple type (Η) and the time (1) between the selections before the selection of a specific type of tapping by a selected slap. - model. ~, immediately following 129145.doc 200900153 4. 5 · According to any of the items 1 to 2 of the square Dan, in this step i), when using a selected slap caused by - Battle < Select one of the peak amplitudes (H) of the dust emission peak and the relationship between the selected slap, the time between the first slap and the first slap (1), identify and select The type of slap that was performed before the slap, which was identified immediately before the slap. For example, in June, items 1 to 2 are used as the method of '------------., which is the method of the following formula, which indicates that one of the peaks of the dust emission is caused by a selected slap. A relationship between a magnitude (H) and the time (1) between the previous slaps of the selected slap 盥: amplitude (H) 〇 c function (time (1)), where The function is selected in the following function: a logarithmic function, and an approximation of a logarithmic function, which is preferably a natural logarithmic function. 6. If requested! The method of any of the preceding claims, wherein the following step is performed to obtain one of the selected dust particle emission peaks (H) caused by a selected slap and the selected slap is immediately adjacent to the previous slap A mathematical model of the relationship between the times (t) between the measurements A) measuring the dust emission after the last field (14) to identify the at least one collecting electrode (18) of the last field (14) The peak of the dust emission associated with (R2; R4) (P2; P4), B) the measured amplitude (HI; H2) of each of the dust emission peaks (P2; P4) and from the last field ( 14) The corresponding time (u; t2) of the at least one collecting electrode (18) immediately after the previous slap (R1; R3) is coupled to 129145.doc 200900153. In order to form a breeding record, each such data record includes the amplitude (H1; H2) of the peak of the dust particle (P2, P4) and the corresponding time since the previous slap (R1, R3) (1) (7), and C) based on the data records 'preparation of a certain amplitude (H) of the peak of the dust particle emission caused by a selected slap and the interval between the selected slap and the previous slap The model of the relationship between time and _. 7. The method of claim 6, the step further comprising: in each of the data records, a first label indicating the type of the shot used to obtain the dust emission peak ^ (2), The step further includes preparing a slap type specific model for each slap type according to the name 払 。. 8. The method of claim 7, the step B) further comprising including in the data record a second label comprising the amplitude, time and the first label associated with the data record before the slap For historical information about the specific type of slap, the step-by-step method includes considering the historical information in each of the slap type specific models. The method of any one of items 1 to 2, wherein the amplitude (H) of one of the peaks of the selected dust emission caused by the slap is updated by the following step A mathematical model eD of the relationship between the slap and the time (t) between the previous slaps measures the dust emission after the last field (10) to identify at least the collection with the last field (14) Electrode (18) - slap (four) related dust particle emission peak, E) the dust particle emission peak (p5) measured amplitude old 2) and the last field (14) of the at least - collecting electrode ( 18) Immediately after the previous slap (4), the corresponding time (t2) of 129145.doc 200900153 is coupled to form a data record, which includes the amplitude of the dust emission peak (P5) (H2) And the corresponding time (t2) since the first slap (R4), and F) based on the data record, updating one of the peaks of the dust emission caused by a selected slap One of the amplitude (H) and the time (1) between the selected slap and its previous slap The mathematical model system. In the method of claim 9, the step E) further includes including, in each data record, a first label indicating the type of the tap that is known to be obtained when the peak of the dust emission is obtained, Step F) further includes updating a slap type specific mathematical model corresponding to the slap type represented by the first label. η. The method of claim 10, the step _ further comprising including in the data records a second label, the 纟 comprising the specific execution performed prior to the slap associated with the amplitude, the time gate and the label of the data record The historical information about the type of slap, the step (4) further includes updating the amplitude of one of the peaks of the dust emission (Η) selected by one of the selected slaps and the slap between the selection and the previous The mathematical model between the time (1) of the slap is taken into account by the historical information. The method of claim 9, wherein the mathematical model is updated during the step F). 13. The method of claim 1, wherein, based on the relationship, adjusting at least one parameter selected from the group consisting of: the last field (14) to be executed - the time of the desired duration (1), and the last I want to perform the I:: 129145.doc 200900153 in the field (14). This step of the hit type is performed by the following steps: measuring at least one of the collection electrodes (18) by the last field (14) The amplitude of one of the dust emission peaks caused by the slap of the electrode transmits information about the measured amplitude of the dust emission peak to a computing device (136), and the computing device (136) compares the peak of the dust emission The measured amplitude and the target value of the peak amplitude of a dust emission, and 用於最小化該塵粒發射峰值幅度目標值與藉由該最後 場(14)之㈣收集電極(18)之至少—收集電極之一後續 拍擊所le成之一後縯塵粒發射峰值之該測量幅度間之差 的目的’藉由該計算裝置(136) ’自動調整選自以下群組 之至少H該最後場(14)中將要執行該後續拍擊之 前的該欲歷時之時間⑴,及該最後場(14)中欲執行之後 續拍擊類型。 1 4,如5月求項1 3之方法,盆φ -fir ^ 八中該汁异裝置(136)包含依據一無 模型演算法運作的一控制琴, 枉刺盎,例如一PI控制器、一pm 控制器、或一無模型適應性控制器。 15. —種預測一靜電集塵器(1) 破後%(I4)之至少一收集 電極(18)之該拍擊期間之塵粒 、 艾毛射的方法,該最後場 (14)係提供放電電極(16) ’吹集電極(18)、及一拍擊裝置 (f’該拍擊裝置(22)係經調適用以藉由拍擊該等收华 電極⑽來為其除塵,該方法係特徵化為以下步驟:、 利用藉由一選定拍擊所造成 战之—選定塵粒發射峰值之 一幅度(H)與介於該選定拍擊與发 ^ 、“緊接先前拍擊間之該時 129145.doc 200900153 間⑴之間的一關係,及 基於藉由一選定拍整所_ # 士、β „ — 、疋祁擎所&成之一選定塵粒發射峰值之 一幅度(H)與介於該選定拍擊 事’、具緊接先刖拍擊間之該時 間⑴之間的該關係,預測一從以下參數中選擇之參數: υ藉由-選定拍擊所造成之塵粒發射峰值㈣之幅产 (HF),其係基於該選定拍擊與其緊接先前拍擊間之 歷時時間⑴,及 欲 拍擊間之欲歷時之時間 所造成之一塵粒發射峰 2) 一選定拍擊與其緊接先前 (tF) ’其係基於藉由該選定拍擊 值(PF)之該幅度(H)。 16.如:求項15之方法,其中藉由下面的式子來表示藉由_ 選足拍擊所造成之—選定塵粒發射峰值之一幅度 於該選定拍擊與其緊接“拍擊間之該時 的 關係: ^ 幅度(H)cc函數(時間⑴), 其中從以下函數中選擇該函數: 對數函數,及 對數函數之近似值, 該函數較佳為一自然對數函數。 17·如請求項15或16之方法,其中預測該參數時利用-數風 模型’其係藉由-選定拍擊所造成之—選定塵粒發射^ 值之-幅度(H)與介於該選定拍擊與其緊接先前拍 該時間(t)之間之該關係的—近似值。 1 8 ·如睛求項15或16之方法 其中藉由以下步驟獲得一數學 129145.doc 200900153 模型 A )測量該最後場(14)之後之塵粒發射以識別與該最後 場(14)之該至少一收集電極(1 8)之拍擊(R2 ; R4)有關的 塵粒發射峰值(P2 ; P4), B) 使該等塵粒發射峰值(P2 ; P4)之每一者之該測量幅 度(Η 1 ; H2)與自該最後場(14)之該至少一收集電極(is) • 之該緊接先前拍擊(R1 ; R3)以來所歷時之該對應時間 (tl ; t2)耦合以便形成資料記錄,各此類資料記錄包含該 ( 峰值(p2 ; P4)之該幅度(HI ; H2)及自該緊接先前拍擊 (Rl ; R3)以來所歷時之該對應時間(U ; t2),及 C) 基於該等資料記錄’製備藉由一選定拍擊所造成 之一選定塵粒發射峰值之一幅度(H)與介於該選定拍擊與 其緊接先前拍擊間之該時間⑴之間之—關係的該數學模 型。 19·如請求項1 5或16之方法’其中藉由以下步驟來更新藉由 一選定拍擊所造成之一選定塵粒發射峰值之一幅度饵)與 I 介於該選定拍擊與其緊接先前拍擊間之該時間⑴之間之 ㊁亥關係的一數學模型 ' D)測1该最後場(14)之後之該塵粒發射以識別與該最 後場(14)之該等收集電極(18)之一拍擊(R5)有關的一塵粒 發射峰值(P5), E)使該塵粒發射峰值(P5)之該測量幅度(H2)與自該最 後場(14)之該至少一收集電極〇8)之該緊接先前拍擊(R4) 以來所歷時之該對應時間(t2)耦合以便形成一資料記 129145.doc 200900153 錄’此類資料記錄包含該峰值(P5)之該幅度(H2)及自該 緊接先前拍擊(R4)以來所歷時之該對應時間(t2),及 F)基於該資料記錄’更新藉由一選定拍擊所造成之 一選定塵粒發射峰值之一幅度(H)與介於該選定拍擊與其 緊接先前拍擊間之該時間⑴之間之一關係的該數學模 型。 20. 一種控制系統,其用以控制來自一靜電集塵器〇)之該塵 粒發射’該靜電集塵器(1)具有一最後場(14),該最後場 U4)係提供放電電極(16)、收集電極〇8)及一拍擊裝置 (22) °亥拍擊裝置(22)係經調適用以藉由拍擊該等收集 電極(18)來為其除塵, 其特徵為該控制系統(30)包含 一控制裝置(38 ; 138),其係可運作以,基於藉由一選 疋拍擊所造成之一選定塵粒發射峰值之一幅度(H)與介於 °亥選疋拍擊與其緊接先前拍擊間之該時間⑴之間的一關 係,調整選自以下群組之至少—參數:該最後場(14)中 將要執仃一拍擊之前的該欲歷時之時間(t),及該最後場 U4)中欲執行之該拍擊類型。 如。月求項20之控制系統,纟中該控制裝置(38)係可運作 以在控制該參數時利用—數學模型,其係藉由一選定拍 斤k成之選疋塵粒發射峰值之一幅度(η)與介於該緊 先月〕拍擊與"亥選定拍擊間之該時間⑴之間之該關係的 一近似值。 々叫求項21之控制系統,其中該控制系統(3進—步包含 129145.doc 200900153 一資料接收器(32) ’其係可運作以接收與該最後場 (14)之後之該塵粒發射有關之測量資料,及在該測量資 料中識別與該最後場(14)之該至少一收集電極(18)之拍 擊(R5)有關的一塵粒發射峰值(P5), 一資料處理器(34),其係可運作以使該塵粒發射峰值 (P5)之該測量幅度(H2)與自該最後場(14)之該至少—收集 電極(1 8)之該緊接先前拍擊(R4)以來所歷時之該對應時 間(t2)耦合以便形成一資料記錄,此類資料記錄包含該 峰值(P5)之該幅度(H2)及自該緊接先前拍擊(R4)以來所 歷時之該對應時間(t2),及 -計算裝置(36) ’其係可運作以,基於該資料記錄, 更新該數學模型,該數學模型係藉由一選定拍擊所造成 之-選定塵粒發射峰值之—幅度(H)與介於該選定拍擊與 其緊接先前拍擊間之該時間⑴之間之該關係的—近: 23,如請求項2〇至22中任一瑁夕地庄丨< 項之控制系統,其中藉由下面的 ^ 示藉由—選定拍擊所造成之-選定塵粒發射峰 ^ 一幅度(H)與介於該選定拍擊與其緊減前拍擊^ 该時間⑴之間的該關係: 之 幅度(H)〇c函數(時間⑴), 其中從以下函數中選擇該函數 對數函數,及 對數函數之近似值, 該函數較佳為—自然對數函數 129145.doc 200900153 24·如π求項20至22中任一項之控制系統,其中該控制裝置 (38)係可用於調整欲執行之該拍擊類型及將要執行一拍 擊之前之該欲歷時之時間之目的而運作。 Α如請求項2G之控制线,其中―計算|置⑽)係可運作 以接收與藉由該最後場⑽之該等收集電極(18)之至少 -收集電極之拍擊所造成之一塵粒發射峰值之該測量幅 度有關的測量資料,該計算裝置〇36)係進一步經調適用 以比較該塵粒發射峰值之該測量幅度與—塵粒發射峰值 幅度目標值,及用於最小化該塵粒發射峰值幅度目標值 與藉由該最後場(14)之該等收集電極⑽之該至少―收 集電極之-後續拍擊所造成之一後續塵粒發射峰值之該 測量幅度間之該差的目的,藉由該控制裝置(138),自動 誘發選自以下群組之至少—參數之調整:該最後場⑽ 中將要執行該後續拍擊之前的該欲歷時之時間,及該 最後場(14)中欲執行之該後續拍擊類型。 I -種控制系統,其用以預測來自—靜電集塵器⑴之該塵 粒發射,該靜電集塵器⑴具有一最後場〇4),該最後場 (M)係提供放電電極(16)、收集電極(18)及—拍擊裝置 ㈣’該拍擊裝置(22)係經調適用以藉由拍擊該等:集 電極(18)來為其除塵, 其特徵為該控制系統(3〇)包含 一資料處理器(3 4 ),其係可運作以利用藉由一選定拍 ,所造成之-敎塵粒發射峰值之—幅度(H)與介於該選 定拍擊與其緊接先前拍擊間之該時間⑴之間的一關係, 129145.doc 10 200900153 ::料處理器(34)係進-步可運作以,基於藉由一選定 =所造叙-録發料值之—幅度(h)與介於該 ㈣與其緊接先前拍擊間之該時間⑴之間的該關係,預 測一從以下參數中選擇之參數 /藉由-選定拍擊所造成之該塵粒發料值㈣之該 巾田度(HF) ’其係基於該選定拍擊與其緊接先前拍擊間之 一欲歷時之時間(t),及 2) -選定拍擊與其緊接先前拍擊間之該欲歷時之時 間(tF),其係基於藉由該選定拍擊所造成之—塵粒發射 峰值(PF)之該幅度(H)。 27. 28. 如請求項26之控制系統,其中該控制裝置(38)係可運作 以在預測該參數時利用一數學模型,其係藉由一選定拍 擊所造成之一選定塵粒發射峰值之一幅度(H)與介於該選 定拍擊與其緊接先前拍擊間之該時間⑴之間之該關係的 一近似值。 如凊求項2 7之控制系統,其中該控制系統進一步包含 一資料接收器(32),其係可運作以識別與該最後場 (14)之該等收集電極(1 8)之至少一收集電極之拍擊(R5)有 關的塵粒發射峰值(P5)及使該等塵粒發射峰值(p5)之每 一者之該測量幅度(H2)與自該最後場(1 4)之該等收集電 極(18)之該至少一收集電極之該緊接先前拍擊(R4)以來 所歷時之該對應時間(t2)耦合以便形成一資料記錄,各 此類資料記錄包含該峰值(P5)之該幅度(H2)及自該緊接 先前拍擊(R4)以來所歷時之該對應時間(t2), 129145.doc 200900153 基於該資料記 該資料處理器(34)係進一步可運作以 錄,更新該數學模型。 (. 129145.doc 12-For minimizing the peak value of the dust particle emission amplitude and at least one of the collecting electrodes (18) of the last field (14), one of the collecting electrodes, and then performing a dust particle emission peak The purpose of the difference between the measured amplitudes 'automatically adjusts the time (1) of the desired time period before the subsequent slap in the last field (14) selected by the computing device (136), And the type of subsequent slaps to be executed in the last field (14). 1 4, as in May, the method of claim 1 3, the pot φ -fir ^ 8 in the juice device (136) comprises a control piano operating according to a model-free algorithm, such as a PI controller, A pm controller, or a model-free adaptive controller. 15. A method for predicting dust particles and AI hair during the slap of at least one collecting electrode (18) of an electrostatic precipitator (1) after breaking (1), the last field (14) providing Discharge electrode (16) 'Blowing electrode (18), and a slap device (f' slap device (22) is adapted to dust the pulverizing electrode (10) by slap it, the method The system is characterized by the following steps: using a selected slap to cause a selected amplitude of the dust emission peak (H) and between the selected slap and the slap, "between the previous slaps At this time, a relationship between 129145.doc 200900153 (1) is based on one of the peaks of the dust emission peak selected by one of the selected _#士, β „ 、, 疋祁擎所& And the relationship between the time (1) between the selected slap and the first slap, predicting a parameter selected from the following parameters: υ by selecting - the dust caused by the slap The peak of the particle emission peak (4) (HF), based on the duration of the selected slap and its previous slap (1) And one of the dust particle emission peaks caused by the time required to slap the slap 2) a selected slap followed by the previous (tF) 'based on the amplitude of the selected slap (PF) H). 16. The method of claim 15, wherein the method of slapping by _ is selected by the following formula: one of the peaks of the selected dust emission is between the selected slap and the "slap" The relationship at that time: ^ Amplitude (H)cc function (time (1)), where the function is selected from the following functions: a logarithmic function, and an approximation of a logarithmic function, which is preferably a natural logarithmic function. The method of clause 15 or 16, wherein the parameter is predicted using a -number wind model 'which is caused by the selected slap" - the selected dust particle emission value - amplitude (H) and the selected slap The approximation of the relationship between the previous time (t) is taken. 1 8 · The method of claim 15 or 16 wherein a mathematics is obtained by the following steps 129145.doc 200900153 Model A) Measuring the last field ( 14) subsequent dust emission to identify a dust emission peak (P2; P4) associated with the slap (R2; R4) of the at least one collecting electrode (18) of the last field (14), B) The measured amplitude of each of the dust particle emission peaks (P2; P4) Η 1 ; H2) coupled with the corresponding time (tl; t2) of the at least one collecting electrode (is) from the last field (14) since the previous tap (R1; R3) Data record, each such data record contains the amplitude (HI; H2) of the peak (p2; P4) and the corresponding time (U; t2) since the previous slap (Rl; R3) And C) based on the data records 'preparation of one of the selected dust particle emission peaks (H) caused by a selected slap and the time between the selected slap and its previous slap (1) Between the mathematical model of the relationship - 19. The method of claim 1 or 5 wherein the following step is used to update one of the peaks of the selected dust emission peak caused by a selected slap and I is a mathematical model of the relationship between the selected slap and the time (1) between the previous slaps, and the dust particle emission after the last field (14) is identified and the last One of the collecting electrodes (18) of the field (14) is slap (R5) related to a dust emission peak (P5), E) making the measured amplitude (H2) of the dust particle emission peak (P5) and the subsequent slap (R4) of the at least one collecting electrode 〇 8) of the last field (14) Coupling with time (t2) to form a data record 129145.doc 200900153 Record 'This data record contains the amplitude (H2) of the peak (P5) and the corresponding time since the previous slap (R4) Time (t2), and F) based on the data record 'update one of the selected dust particle emission peaks (H) caused by a selected slap and between the selected slap and its previous slap The mathematical model of the relationship between one of the time (1). 20. A control system for controlling the emission of the dust particles from an electrostatic precipitator" (the electrostatic precipitator (1) having a final field (14), the last field U4) providing a discharge electrode ( 16), collecting electrode 8) and a slamming device (22) The slap device (22) is adapted to be dusted by slapping the collecting electrodes (18), characterized by the control The system (30) includes a control device (38; 138) operable to select one of the peaks (H) of the selected dust emission peaks based on one of the selected slaps by a selective slap. A relationship between the slap and the time (1) between the previous slaps, adjusted to at least the following parameter - the parameter: the last field (14) is about to hold the desired time before the slap (t), and the type of slap to be performed in the last field U4). Such as. In the control system of the monthly claim 20, the control device (38) is operable to utilize the mathematical model when controlling the parameter, which is selected by the selected one of the dust particles. An approximation of the relationship between (η) and the time (1) between the slap and the selected slap. The control system of claim 21, wherein the control system (3) includes a 129145.doc 200900153 data receiver (32) that is operable to receive the dust emission after the last field (14) Corresponding measurement data, and identifying, in the measurement data, a dust emission peak (P5) related to the slap (R5) of the at least one collecting electrode (18) of the last field (14), a data processor ( 34), which is operable to cause the measured amplitude (H2) of the dust particle emission peak (P5) and the at least the collecting electrode (18) from the last field (14) to be immediately slammed ( The corresponding time (t2) elapsed since R4) is coupled to form a data record containing the amplitude (H2) of the peak (P5) and the time since the previous slap (R4) The corresponding time (t2), and - computing device (36) 'is operable to update the mathematical model based on the data record, the mathematical model is caused by a selected slap - the selected dust emission peak Between the amplitude (H) and the selected slap followed by the previous slap The relationship between the time (1) - near: 23, as in any of the request items 2 〇 22, the control system of the item, wherein the slap is selected by the following Caused by the selected dust particle emission peak ^ a magnitude (H) and the relationship between the selected slap and the slap before the slamming ^ the time (1): the amplitude (H) 〇 c function (time (1)), Wherein the logarithmic function of the function and the approximation of the logarithmic function are selected from the following functions, the function is preferably a natural logarithmic function 129145.doc 200900153 24. A control system according to any one of items 20 to 22, wherein the control The device (38) is operable to adjust the type of the slap to be performed and the time of the desired slap before the slap is performed. For example, the control line of claim 2G, where "computation|set (10)) Operable to receive measurement data relating to the measurement amplitude of one of the dust emission peaks caused by the slap of at least the collection electrode of the collection electrode (18) of the last field (10), the computing device 〇 36) The system is further adapted to compare the dust The measured amplitude of the emission peak and the target value of the peak amplitude of the dust emission, and the target value for minimizing the peak amplitude of the dust particle emission and the at least "collecting electrode" of the collecting electrode (10) by the last field (14) For the purpose of the difference between the measured amplitudes of one of the subsequent dust emission peaks caused by the subsequent slap, the control device (138) automatically induces at least the adjustment of the parameter selected from the following group: the last The time of the desired duration before the subsequent slap in field (10), and the subsequent slap type to be executed in the last field (14). a control system for predicting the emission of the dust particles from the electrostatic precipitator (1), the electrostatic precipitator (1) having a final field 〇4), the last field (M) providing a discharge electrode (16) Collecting electrode (18) and slap device (4) 'The slamming device (22) is adapted to be dusted by tapping the collector: (18), characterized by the control system (3) 〇) includes a data processor (34) that is operable to utilize a selected beat, resulting in a peak of the dust emission (amplitude (H) and immediately before the selected slap A relationship between the time (1) between the slaps, 129145.doc 10 200900153: The material processor (34) is operable to be based on a selected = written-recorded value - The relationship between the amplitude (h) and the time (1) between the (4) and the immediately preceding slap, predicting a parameter selected from the following parameters/by the selected slap caused by the dust blasting The value (4) of the towel (HF) is based on the time between the selected slap and the previous slap (t) And 2) - the time (tF) of the desired duration of the slap and its immediately following slap, based on the amplitude of the dust emission peak (PF) caused by the selected slap (H) . 27. The control system of claim 26, wherein the control device (38) is operative to utilize a mathematical model for predicting the parameter, the selected dust particle emission peak being selected by a selected slap An approximation of one of the magnitude (H) and the relationship between the selected slap and the time (1) between the previous slaps. The control system of claim 27, wherein the control system further comprises a data receiver (32) operative to identify at least one of the collection electrodes (18) of the last field (14) The peak of the dust emission (P5) associated with the slap (R5) of the electrode and the measured amplitude (H2) of each of the peaks of the dust emission (p5) and the last field (1 4) The corresponding time (t2) of the at least one collecting electrode of the collecting electrode (18) immediately after the previous tap (R4) is coupled to form a data record, each such data record comprising the peak (P5) The amplitude (H2) and the corresponding time (t2) since the previous slap (R4), 129145.doc 200900153 based on the data, the data processor (34) is further operable to record, update The mathematical model. (. 129145.doc 12-
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