墙体设置接线盒隔声性能影响的实验室研究

在轻质墙体(轻钢龙骨类板墙)及重质墙体(240 mm砖墙)上设置不同数量的接线盒前后,对墙体的空气声隔声性能的影响进行了实验室试验。并对试验结论进行了分析,得出了不同类型墙体设置接线盒后,对墙体空气声隔声性能的影响因素及处理方法。     

飞机内部轻质隔声间的研究

一、机舱内的噪声 本文首先对比了国产某型飞机在地面静止发动和空中飞行时的噪声,结果见图1.噪声以125Hz到250Hz最强,500—1000Hz次之,2000Hz以上的高频噪声比较弱.测试所用的仪器是精密声级计和倍频程滤波器.飞行与静止发动的噪声相比,各频带约高1到2dB,A声级约高3dB.该型国产与国外同类机种对比,     

联合扩散场激励与近场声全息重建的建筑构件隔声测量方法

提出了一种联合扩散场(DAF)激励与近场声全息(NAH)辐射声强重建的建筑构件空气声隔声测量方法。该方法首先通过DAF激励构件振动并获取入射声功率,然后利用NAH技术从辐射声压场中重建构件表面高空间分辨率的法向声强分布,最后根据声强分布来计算辐射声功率和定位辐射热区,从而实现构件隔声量和隔声缺陷测量。隔声室实验研究表明,在测试距离和采样间距均为0.04 m的条件下,该方法测量的隔声量与声压法的误差在100～5000 Hz频带小于3.3 dB,在250～3150 Hz频带小于1.3 dB,对圆孔(直径8 mm)和矩形缝(长80 mm、宽3 mm)的定位精度高达厘米级;同时,该方法在一定混响和背景噪声影响下的稳定性较强,接收室混响时间从1.0 s增至3.4 s (步长0.6 s)以及信噪比从10 dB降至0 dB (步长5 dB),隔声量测量误差分别在0.8 dB和0.3 dB以内,缺陷定位误差在0.037 m和0.035 m以内。所提方法有助于提高实验室中建筑构件隔声特性的测量能力,同时对接收室测试环境具有较强的鲁棒性。     

内墙的隔声改善量

内墙的隔声改善量ΔR是受内、外墙间空腔和内墙的传声损失、以及墙间基础的传递损失所决定.从厚的外墙到比它薄的内墙传声中,不仅是降低了固体声速度级的绝对值,且内墙上的速度级分布,也在一定程度上反映出外墙上的速度级分布.因此,测量内、外墙上速度(或加速度)级差,可得到ΔR的近似值. 分离的双层墙,在最低简正频率以下,相当于质量阻抗时,内墙的ΔR-f曲线才以40dB/decade递增.实用的大面积内墙,其简正频率很快达到足够的密度,其弯曲波阻抗与频率无关,ΔR-f曲线以20dB/decade而递增. 墙间空腔填吸声材料或墙内加阻尼材料都可提高隔声量.双层墙共用基础或分离基础但无隔振器,则内墙的ΔR分别不大于9或18dB.要使内墙有较高的ΔR,应选用适当f_0的隔振器.压缩量随时间而变的隔振材料不宜用做为隔振器.     

提高轻板隔墙的隔声性能

影响轻板隔墙隔声性能的因素是多方面的.本文着重研究了降低龙骨的传声、附加构造的作用以及墙板的选择等方面.文中通过理论分析和实验比较,说明这些措施对提高轻板隔墙的隔声性能是有效而可行的.     

PbWO4晶体中的填隙氧及其对晶体光学性质的影响

运用GULP计算软件模拟计算了PbWO₄(PWO)晶体中不同位置的填隙氧原子点缺陷的生成能，计算结果表明：当填隙氧原子存在于(WO₄)^2-的周围时，填隙氧原子点缺陷的生成能最低；进一步运用基于密度泛函理论的全数值自洽DV-Xα方法计算了包含填隙氧原子的PWO晶体的态密度，计算结果表明：当填隙氧处在(WO₄)^2-的周围时，容易与(WO₄)^2-上的一个或两个氧离子相互作用形成分子离子O₂^2-或O₃^4-，通过分析这些计算结果，认为PWO晶体中350 nm吸收带的出现很可能与晶体中的氧分子离子有关.     

点声源入射下无限大平板的隔声

利用球面波的平面波展开形式,推导了自由场中点声源入射下无限大平板的隔声公式,研究了其隔声性能。数值模拟结果表明,点声源入射下平板隔声规律不同于通常采用的平面波入射条件下的质量隔声定律。在频率较低或板厚度较薄时,频率或板面密度增加一倍,平板隔声量的增加约为3 dB,而插入损失的增加约为6 dB。     

大型透明件透光率和雾度测量装置的研制

为现场测量大型透明件的透光率和雾度,提出了基于双积分球结构的测量和系统参数标定方案,并设计研制了相应的透光率和雾度测量装置。该装置通过六维机械调整装置完成光路调整,基于LED光源的照明准直系统产生调制平行光,最后采用双积分球结构的探测接收装置并结合锁相放大技术,实现光电信号的解调。测试结果表明,该装置对透光率测量的绝对误差不超过1%,对雾度测量的绝对误差不超过0.3%,符合工程应用对系统测量精度提出的要求。另一方面,装置具有很好的重复性,其对透光率和雾度测量的相对标准差分别为0.06 %和0.05%。     

在实验室中测量大电阻的一种新方法

介绍了在实验室中测大电阻的一种方法。依据欧姆定律,并利用灵敏电流计测出数据。被测电阻的实测结果标准误差小于００３ＭΩ,相对误差小于１％。     

CFETR1/32真空室机加工件的激光测量研究

在1/32真空室部件后期机加工时,采用激光跟踪仪对工件进行测量,从而解决了其在机床平台上定位基准的问题。在工件安放在机床平台后,首先通过测量拟合出工件的设计坐标系,确定其装配基准点;其次在工件外部加工出具备XY、YZ、XZ三正交平面特征的辅助标准块,建立机床坐标系;然后使用激光跟踪仪同时测量工件和辅助标准块,确定工件与辅助标准块的相对位置关系;最后机床以辅助标准块作为定位基准来完成工件的加工。使用该方法已完成两个1/32真空室部件的加工,并且加工精度在公差要求范围之内,验证了该方法的合理性和可操作性。     

住宅建筑中相邻房间的侧向传声预测

侧向传声作为建筑中声传递的组成部分,对住宅的整体隔声效果具有重要的影响,通过将建筑中相邻房间的各建筑构件划分为若干子系统,应用统计能量分析(Statistical Energy Analysis,SEA)理论,从系统的声功率平衡的角度建立侧向传声的预测模型,在描述各路径的传声规律的同时确定主要传声路径。研究结果表明:当外围护结构为重质结构,且为匀质单一材料构造时,(1)在低频处,全程通过两相邻房间的侧墙或楼板的非通过隔墙的侧向路径成为主要侧向传声路径;(2)在中高频,各侧向路径的声压级差趋于一致,此时的建筑隔声性能取决于通过隔墙的直接路径上的声传递;(3)采用重质隔墙可以缩小侧向传声影响的频率范围。本研究为改善住宅的声环境质量及建筑隔声设计提供了理论依据。     

Development of multiple drywall with high sound insulation performance

Experimental studies for the development of multiple drywalls with a high sound insulation performance are performed. Firstly, a means of preventing the sound insulation deterioration due to the coincidence effect at high frequencies is investigated by layering two plasterboards with different physical characteristics. Based on the results, a double drywall with a sound insulation performance of R_w = 61 is developed. Further more, a double drywall of R_w = 64 , a triple drywall of R_w = 86 and a quadruple drywall of R_w = 90 are developed.     

Field measurement of airborne sound insulation between rooms with non-diffuse sound fields at low frequencies

Procedures for the field measurement of airborne sound insulation between rooms with diffuse fields are described in International Standard ISO 140-4. However, many dwellings contain rooms with volumes less than 50 m³, where low frequency measurements are less reliable; hence there is a need for a measurement procedure to improve the reliability of field measurements in rooms with non-diffuse fields. Procedures are proposed for sound pressure level and reverberation time measurements for the 50, 63 and 80 Hz third octave bands. The sound pressure level measurement combines corner microphone positions with positions in the central region of each room. This provides a good estimate of the room average sound pressure level with significantly improved repeatability.     

The prediction of airborne sound transmission between two rooms using first-order flanking paths

Airborne sound transmission between adjacent rooms can be predicted using the Standard EN 12354-1 (ISO 15712-1), which is equivalent to a first-order approximation of statistical energy analysis (SEA). This paper analyses airborne sound transmission between adjacent rooms in a masonry building, by comparing results obtained from EN 12354-1 to SEA predictions and measurements. It is shown that the restriction of the Standard to first-order flanking paths can lead to large errors in predictions when compared to measurements and SEA results taking into account all transmission paths. This is observed both for individual flanking paths and overall transmission between rooms, for which the Standard provides results similar to those obtained by the first-order approximation of SEA. The paper also looks at possible reasons why previous studies using the approach in EN 12354 have generally shown good agreement with measurements.     

The use of in-situ test method EN 1793-6 for measuring the airborne sound insulation of noise barriers

The in situ measurement of the airborne sound insulation, as outlined in EN 1793-6:2012, is becoming a common means of quantifying the performance of road traffic noise reducing devices. Newly installed products can be tested to reveal any construction defects and periodic testing can help to identify long term weaknesses in a design. The method permits measurements to be conducted in the presence of background noise from traffic, through the use of impulse response measurement techniques, and is sensitive to sound leakage. Factors influencing the measured airborne sound insulation are discussed, with reference to measurements conducted on a range of traffic noise barriers located around Auckland, New Zealand. These include the influence of sound leakage in the form of hidden defects and visible air gaps, signal-to-noise ratio, and noise barrier height. The measurement results are found to be influenced by the presence of hidden defects and small air gaps, with larger air gaps making the choice of measurement position critical. A signal-to-noise ratio calculation method is proposed, and is used to show how the calculated airborne sound insulation varies with signal-to-noise ratio. It is shown that the measurement results are influenced by barrier height, through the need for reduced length Adrienne temporal windows to remove the diffraction components, prohibiting the direct comparison of results from noise barriers with differing heights.     

Justification of standardized level differences in rating of airborne sound insulation between dwellings

It has long been recognized that single-number quantities R′_w, D_nT,w or D_n,w result in different conclusions in objective rating of airborne sound insulation between dwellings. The difference between the values of these single-number quantities (SNQ), however, does not prove which of them describes the sound transmission between rooms most correctly. The main object of this article was to study which SNQ correspond best with transmitted living sound levels in buildings when reverberation time, volume of receiving room and sound insulation are taken into account. Data of 100 field measurements of airborne sound insulation were collected as well as 207 reverberation times of furnished rooms. The transmitted sound levels of living sounds were evaluated on the basis of known living sound spectra and measured level differences D. The results show that the SNQs standardized to reference reverberation time of 0.5 s lead in all cases to best correlation between the SNQs and the sound levels of transmitted living sounds. It was also checked whether the rating by D_nT,w would lead to higher transmitted sound levels of living sounds in larger rooms, but this was not detected. The use of D_nT,w makes rooms of different volumes equal in regard to required sound insulation between them. It is thus justified to replace R′_w with D_nT,w as the SNQ for rating the airborne sound insulation. Widening the frequency range down to 50 Hz or up to 5000 Hz did not give noteworthy improvement in the correlation.     

Measurement of airborne sound insulation of timber noise barriers: Comparison of in situ method CEN/TS 1793-5 with laboratory method EN 1793-2

Recent progress in the development of European standards has allowed the in situ testing of roadside noise barriers. CEN/TS 1793-5 describes a test method using maximum length sequences (MLS) for the characterisation of airborne sound insulation. However, many barriers are tested according to a laboratory standard, EN 1793-2, based on measurements carried out in reverberant chambers and in the case of timber barriers with a relatively low airborne sound insulation it is not clear to what extent the results of the two tests compare. The paper describes the results of tests carried out using both methods. Six samples of timber barrier were compared including single-leaf and double-leaf constructions and single-leaf constructions with an absorptive core. Very good agreement was found especially when account was taken of the valid frequency range in each test method. The results open up the possibility of routinely evaluating the performance of timber barriers at the roadside where build quality can be variable and there are concerns that the acoustic performance may not match that obtained under laboratory test conditions where typically the barrier is more carefully constructed.     

Determination of the sound energy level of a gunshot and its applications in room acoustics

In some cases an impulsive noise source such as a gunshot can be a preferred alternative when investigating building acoustics, including sound insulation measurements, when compared to conventional steady state noise sources. A gun equipped with blank cartridges is an impulsive noise source that is lightweight and small enough to be easily transported. The differences in the noise characteristics between individual cartridges for the same gun are usually small, so the impulsive source can be replicated to a high degree. This paper is focused on the practical application of the sound exposure levels produced by a gunshot with a known sound energy level in the rooms under investigation. In this way, the equipment and methods required by the conventional method are simplified significantly. Furthermore, reverberation times need not be measured, since the equivalent absorption area can be directly obtained from the measured sound exposure levels. Using Green’s theorem, the roles of the sound source and measuring microphone were exchanged, which simplified the determination of sound insulation as it was easier to change the position of the gun than the microphone. The results obtained using the impulsive noise source were in good agreement with those obtained using the conventional method. Above 100 Hz, their difference in any frequency band of interest was less than 1 dB.