农业工程学报
農業工程學報
농업공정학보
2013年
22期
226-235
,共10页
张绪坤%苏志伟%王学成%马怡光
張緒坤%囌誌偉%王學成%馬怡光
장서곤%소지위%왕학성%마이광
污泥处理%干燥%模型%有效扩散系数%活化能
汙泥處理%榦燥%模型%有效擴散繫數%活化能
오니처리%간조%모형%유효확산계수%활화능
sludge disposal%drying%models%effective diffusivity coefficient%activation energy
为研究污泥薄层在过热蒸汽干燥和热风干燥过程中有效扩散系数及活化能,搭建了常压内循环式干燥试验装置。在160~280℃温度下,分别对4、10 mm污泥薄层进行过热蒸汽干燥和热风干燥。利用Fick扩散模型,建立有效扩散系数和干燥时间的关系,试验得到4 mm污泥薄层过热蒸汽干燥与热风干燥的有效扩散系数范围分别为7.1515×10-9~2.4852×10-8m2/s和1.2414×10-8~2.2769×10-8 m2/s;10 mm污泥薄层过热蒸汽干燥与热风干燥的有效扩散系数范围分别为1.9659×10-8~5.8811×10-8 m2/s和2.8042×10-8~5.6095×10-8 m2/s。根据Arrhenius经验公式建立有效扩散系数与温度的关系,得到4、10 mm污泥薄层过热蒸汽干燥和热风干燥的平均活化能分别为21.173、18.085和9.485、11.191 kJ/mol。用Midilli薄层干燥模型模拟得出的过热蒸汽干燥与热风干燥有效扩散系数和活化能与试验值基本吻合。研究结果表明:当温度超过260℃时,过热蒸汽干燥的有效扩散系数比热风干燥有效扩散系数大。过热蒸汽干燥有效扩散系数随温度增加的趋势近乎成一条斜直线,而热风干燥的有效扩散系数增加趋势则是曲线性,说明热风干燥过程中存在氧化、燃烧的可能。文章确定了污泥薄层干燥有效扩散系数值及过热蒸汽干燥逆转点温度,为污泥过热蒸汽干燥参数优化与干燥设备设计提供参考。
為研究汙泥薄層在過熱蒸汽榦燥和熱風榦燥過程中有效擴散繫數及活化能,搭建瞭常壓內循環式榦燥試驗裝置。在160~280℃溫度下,分彆對4、10 mm汙泥薄層進行過熱蒸汽榦燥和熱風榦燥。利用Fick擴散模型,建立有效擴散繫數和榦燥時間的關繫,試驗得到4 mm汙泥薄層過熱蒸汽榦燥與熱風榦燥的有效擴散繫數範圍分彆為7.1515×10-9~2.4852×10-8m2/s和1.2414×10-8~2.2769×10-8 m2/s;10 mm汙泥薄層過熱蒸汽榦燥與熱風榦燥的有效擴散繫數範圍分彆為1.9659×10-8~5.8811×10-8 m2/s和2.8042×10-8~5.6095×10-8 m2/s。根據Arrhenius經驗公式建立有效擴散繫數與溫度的關繫,得到4、10 mm汙泥薄層過熱蒸汽榦燥和熱風榦燥的平均活化能分彆為21.173、18.085和9.485、11.191 kJ/mol。用Midilli薄層榦燥模型模擬得齣的過熱蒸汽榦燥與熱風榦燥有效擴散繫數和活化能與試驗值基本吻閤。研究結果錶明:噹溫度超過260℃時,過熱蒸汽榦燥的有效擴散繫數比熱風榦燥有效擴散繫數大。過熱蒸汽榦燥有效擴散繫數隨溫度增加的趨勢近乎成一條斜直線,而熱風榦燥的有效擴散繫數增加趨勢則是麯線性,說明熱風榦燥過程中存在氧化、燃燒的可能。文章確定瞭汙泥薄層榦燥有效擴散繫數值及過熱蒸汽榦燥逆轉點溫度,為汙泥過熱蒸汽榦燥參數優化與榦燥設備設計提供參攷。
위연구오니박층재과열증기간조화열풍간조과정중유효확산계수급활화능,탑건료상압내순배식간조시험장치。재160~280℃온도하,분별대4、10 mm오니박층진행과열증기간조화열풍간조。이용Fick확산모형,건립유효확산계수화간조시간적관계,시험득도4 mm오니박층과열증기간조여열풍간조적유효확산계수범위분별위7.1515×10-9~2.4852×10-8m2/s화1.2414×10-8~2.2769×10-8 m2/s;10 mm오니박층과열증기간조여열풍간조적유효확산계수범위분별위1.9659×10-8~5.8811×10-8 m2/s화2.8042×10-8~5.6095×10-8 m2/s。근거Arrhenius경험공식건립유효확산계수여온도적관계,득도4、10 mm오니박층과열증기간조화열풍간조적평균활화능분별위21.173、18.085화9.485、11.191 kJ/mol。용Midilli박층간조모형모의득출적과열증기간조여열풍간조유효확산계수화활화능여시험치기본문합。연구결과표명:당온도초과260℃시,과열증기간조적유효확산계수비열풍간조유효확산계수대。과열증기간조유효확산계수수온도증가적추세근호성일조사직선,이열풍간조적유효확산계수증가추세칙시곡선성,설명열풍간조과정중존재양화、연소적가능。문장학정료오니박층간조유효확산계수치급과열증기간조역전점온도,위오니과열증기간조삼수우화여간조설비설계제공삼고。
Sewage sludge is generated in wastewater treatment processes. It has a solids content of about 1-2%typically. The key step to treating sludge is dewatering.. Dewatering of sludge by belt presses, filters, and centrifuges can lead to dry solids contents in the range of 15-25%. This step can substantially reduce the volume of the sludge. Characteristics of sludge include high water content, bulk mass, and containment of pathogenic microorganisms. Landfilling of sludge has the disadvantages of occupying land and causing secondary pollutions, especially to groundwater. Thermal drying of dewatered sludge is another step to reduce the volume of dewatered sludge. The drying process consists of complex mechanisms such as molecular diffusion, capillary flow, Knudsen flow, water uptake kinetics flow, and surface diffusion. In order to study the effective diffusion coefficient and the activation energy characteristics of the sludge layer in the process of superheated steam drying and hot air drying, an internal-circulation drying test-bed under normal pressure was built to carry out superheated steam drying and hot air drying tests on sludge layers with thicknesses of 4 mm and 10 mm respectively at the temperature range of 160-280℃. The linear relationship between effective diffusion coefficient and drying time was established through the Fick diffusion model. It was found that the effective diffusion coefficients for the 4 mm sludge layer ranged 7.1515×10-9-2.4852×10-8m2/s and 1.2414×10-8-2.2769×10-8 m2/s for superheated steam drying and hot air drying respectively. The effective diffusion coefficients for the 10 mm sludge layer ranged 1.9659×10-8-5.8811×10-8 m2/s and 2.8042×10-8-5.6095×10-8 m2/s for superheated steam drying and hot air drying respectively. The linear relationship between effective diffusion coefficient and temperature was established based on the Arrhenius empirical formula. Thus, the average activation energies of 4 and 10 mm sludge layers can be obtained respectively as 21.173 and 18.085 kJ/mol by superheated steam drying and 9.485, 11.191 kJ/mol by hot air drying. These values are mostly in conformity with the effective diffusion coefficient and activation energy obtained by the Midilli thin layer drying model This test showed that when temperature exceeds 260℃, the effective diffusion coefficient of a sludge layer by superheated steam drying is greater than that created by hot air drying. Values obtained showed a linear increase in diffusion coefficients to temperature by superheated steam drying but a curve in hot air drying, suggesting the possibility of oxidation and combustion of the sludge layer by hot air drying.