载钛羟基磷灰石光催化降解内分泌干扰物双酚A（英文）

对载钛羟基磷灰石(TiHAP)进行了透射电镜、X射线衍射、紫外-可见光谱和Zeta电位表征,并应用液相色谱-质谱技术对比了TiHAP和P25 TiO2对环境内分泌干扰物双酚A(BPA)的吸附和光催化降解性能,探讨了富里酸和Fe3+对TiHAP薄膜光催化性能的影响.结果表明,TiHAP和TiO2粉体对BPA的吸附符合Langmuir吸附等温方程,且前者吸附性能更大.TiHAP薄膜光催化降解BPA的性能优于TiO2薄膜;富里酸和Fe3+对TiHAP和TiO2薄膜光催化性能的影响趋势不同,从能带结构、电子转移和吸光性等角度分析了性能不同的原因.本结果可以为应用TiHAP降解环境内分泌干扰物提供依据.     

利用几何画板教学课件制作简单动画

充分利用现代化的多媒体教学手段,是实现有效教学重要途径之一,动画演示是物理课多媒体辅助教学的精彩环节.几何画板(The Geometer’s Sketchpad & reg)是一个能提供丰富而方便的创造功能,使用户可以随心所欲地编写出自己需要的教学课件的实用软件.沪科教版高中《物理·选修3-4》"简谐运动"教学中,引入单位圆来研究弹簧振子的周期.用几何画     

载钛羟基磷灰石光催化降解内分泌干扰物双酚A

对载钛羟基磷灰石（TiHAP）进行了透射电镜、X射线衍射、紫外-可见光谱和Zeta电位表征,并应用液相色谱-质谱技术对比了TiHAP和P25 TiO₂对环境内分泌干扰物双酚A（BPA）的吸附和光催化降解性能,探讨了富里酸和Fe³⁺对TiHAP薄膜光催化性能的影响。结果表明,TiHAP和TiO₂粉体对BPA的吸附符合Langmuir吸附等温方程,且前者吸附性能更大。TiHAP薄膜光催化降解BPA的性能优于TiO₂薄膜;富里酸和Fe³⁺对TiHAP和TiO₂薄膜光催化性能的影响趋势不同,从能带结构、电子转移和吸光性等角度分析了性能不同的原因。本结果可以为应用TiHAP降解环境内分泌干扰物提供依据。     

一道高考题的新解法

2011年陕西、山西、宁夏等省、自治区高考使用新课程理综卷,物理题延续了往年的稳定,又体现了"稳中有新,稳中有进".第24题是物理力学解答题,该题贴近生活,注重学以致用,主要考查考生对物理定律的基本应用能力,考查考生的分析综合能力,也是对物理模型的建立和应用的考查.该题常规解法     

Enhancement of charging performance of quantum battery via quantum coherence of bath

An open quantum battery (QB) model of a single qubit system charging in a coherent auxiliary bath (CAB) consisting of a series of independent coherent ancillae is considered. According to the collision charging protocol we derive a quantum master equation and obtain the analytical solution of QB in a steady state. We find that the full charging capacity (or the maximal extractable work (MEW)) of QB, in the weak QB-ancilla coupling limit, is positively correlated with the coherence magnitude of ancilla. Combining with the numerical simulations we compare with the charging properties of QB at finite coupling strength, such as the MEW, average charging power and the charging efficiency, when considering the bath to be a thermal auxiliary bath (TAB) and a CAB, respectively. We find that when the QB with CAB, in the weak coupling regime, is in fully charging, both its capacity and charging efficiency can go beyond its classical counterpart, and they increase with the increase of coherence magnitude of ancilla. In addition, the MEW of QB in the regime of relative strong coupling and strong coherent magnitude shows the oscillatory behavior with the charging time increasing, and the first peak value can even be larger than the full charging MEW of QB. This also leads to a much larger average charging power than that of QB with TAB in a short-time charging process. These features suggest that with the help of quantum coherence of CAB it becomes feasible to switch the charging schemes between the long-time slow charging protocol with large capacity and high efficiency and the short-time rapid charging protocol with highly charging power only by adjusting the coupling strength of QB-ancilla. This work clearly demonstrates that the quantum coherence of bath can not only serve as the role of "fuel" of QB to be utilized to improve the QB's charging performance but also provide an alternative way to integrate the different charging protocols into a single QB.