在不均匀光照条件下,光伏阵列输出特性呈现多峰现象,传统的最大功率点跟踪(maximum power point tracking,MPPT)方法容易陷入局部极值。为了提高复杂阴影下的跟踪速度和跟踪精度,结合改进粒子群算法(improved particle swarm optimizati...在不均匀光照条件下,光伏阵列输出特性呈现多峰现象,传统的最大功率点跟踪(maximum power point tracking,MPPT)方法容易陷入局部极值。为了提高复杂阴影下的跟踪速度和跟踪精度,结合改进粒子群算法(improved particle swarm optimization,IPSO)和自适应步长扰动观察法(adaptive perturbation and observation,AP&O)各自的特点,提出了基于IPSO-AP&O算法的改进MPPT控制方法。其中,IPSO算法采用自适应惯性权重因子,在不同搜索阶段能够充分搜索目标函数,然后与AP&O算法结合实现最大功率的稳定输出。仿真结果表明,所提出的IPSO-AP&O算法减少了传统智能算法的迭代过程,能快速跟踪到全局最大功率点,相比其余几种算法而言,在光照强度突变时均具备快速精准的双重跟踪能力,在4种场景下跟踪效率分别为99.86%、99.91%、87.63%、99.79%,能够更好地减小光伏阵列外部条件变化导致的功率损耗,所提出的MPPT控制方法能够较好地适用于光储混合系统,具备工程实用价值。展开更多
仿射传播(Affinity propagation,AP)聚类算法是将所有待聚类对象作为潜在的聚类中心,通过对象之间传递的可靠性和有效性信息找到合适的聚类中心,从而计算出相应的聚类结果,但不适用子空间聚类。将粒度计算引入到仿射传播聚类算法中,提...仿射传播(Affinity propagation,AP)聚类算法是将所有待聚类对象作为潜在的聚类中心,通过对象之间传递的可靠性和有效性信息找到合适的聚类中心,从而计算出相应的聚类结果,但不适用子空间聚类。将粒度计算引入到仿射传播聚类算法中,提出属性与样本同步粒化的AP熵加权软子空间聚类算法(Entropy weighting AP algorithm for subspace clustering based on asynchronous granulation of attributes and samples,EWAP)。EWAP首先去除冗余属性,然后在每次聚类的迭代过程中修改属性的权重值。在满足一定条件迭代终止时,就会得到构成各兴趣度子空间的属性权重值,从而得到属性集的粒化结果以及相应的子空间聚类结果。理论与实验证明EWAP算法既保留了AP算法的优点,又克服了该聚类算法不能进行子空间聚类的不足。展开更多
It is proved that, for the nondivergence elliptic equations Σi,jn=1aijuxixj=f, if f belongs to the generalized Morrey spaces Lp, (w), then uxixj ∈ Lp, (w), where u is the W2,p-solution of the equations. In order to ...It is proved that, for the nondivergence elliptic equations Σi,jn=1aijuxixj=f, if f belongs to the generalized Morrey spaces Lp, (w), then uxixj ∈ Lp, (w), where u is the W2,p-solution of the equations. In order to obtain this, the author first establish the weighted boundedness for the commutators of some singular integral operators on Lp, (w).展开更多
In this paper, the weighted boundedness of parametric Marcinkiewicz integral and its commutator with rough kernels are considered. In addition, the weak type norm inequalities for parametric Marcinkiewicz integral and...In this paper, the weighted boundedness of parametric Marcinkiewicz integral and its commutator with rough kernels are considered. In addition, the weak type norm inequalities for parametric Marcinkiewicz integral and its commutator with different weight functions and Dini kernel are also discussed.展开更多
In this paper, we shall deal with the boundedness of the Littlewood-Paley operators with rough kernel. We prove the boundedness of the Lusin-area integral μΩs and Littlewood-Paley functions μΩ and μλ^＊ on the w...In this paper, we shall deal with the boundedness of the Littlewood-Paley operators with rough kernel. We prove the boundedness of the Lusin-area integral μΩs and Littlewood-Paley functions μΩ and μλ^＊ on the weighted amalgam spaces （Lω^q,L^p）^α（R^n）as 1〈q≤α〈p≤∞.展开更多
For 0 〈 α 〈 mn and nonnegative integers n ≥ 2, m≥ 1, the multilinear fractional integral is defined bywhere →y= （y1, Y2,…, ym） and 7 denotes the m-tuple （f1, f2,…, fm）. In this note, the one- weighted and ...For 0 〈 α 〈 mn and nonnegative integers n ≥ 2, m≥ 1, the multilinear fractional integral is defined bywhere →y= （y1, Y2,…, ym） and 7 denotes the m-tuple （f1, f2,…, fm）. In this note, the one- weighted and two-weighted boundedness on Lp （JRn） space for multilinear fractional integral operator I（am） and the fractional multi-sublinear maximal operator Mα（m） are established re- spectively. The authors also obtain two-weighted weak type estimate for the operator Mα（m）.展开更多
In this paper, we will obtain the weak type estimates of intrinsic square func- tions including the Lusin area integral, Littlewood-Paley g-function and g^-function on the weighted Morrey spaces L^1,k （w） for 0〈k〈...In this paper, we will obtain the weak type estimates of intrinsic square func- tions including the Lusin area integral, Littlewood-Paley g-function and g^-function on the weighted Morrey spaces L^1,k （w） for 0〈k〈 1 and w ∈ A1.展开更多
In this note the authors give the weighted Lp-boundedness for a class of maximal singular integral operators with rough kernel. The result in this note is an improvement and extension of the result obtained by Chen a...In this note the authors give the weighted Lp-boundedness for a class of maximal singular integral operators with rough kernel. The result in this note is an improvement and extension of the result obtained by Chen and Lin in 1990.展开更多
Let L = -△＋V be a Schrodinger operator acting on L^2（R^n）, n ≥ 1, where V ≠ 0 is a nonnegative locally integrable function on R^n. In this article, we will introduce weighted Hardy spaces Hp （w） associated wit...Let L = -△＋V be a Schrodinger operator acting on L^2（R^n）, n ≥ 1, where V ≠ 0 is a nonnegative locally integrable function on R^n. In this article, we will introduce weighted Hardy spaces Hp （w） associated with L by means of the square function and then study their atomic decomposition theory. We will also show that the Riesz transform △↓L^-1/2 associated with L is bounded from our new space HP（w） to the classical weighted Hardy sp ace HP （ w ） when n / （n ＋ 1 ） 〈 p 〈 1 and w ∈ A 1 ∩ R H（ 2 / p ）＇.展开更多
The Fourier transform and the Littlewood-Paley theory are used to give the weighted boundedness of a strongly singular integral operator defined in this paper. The paper shows that the strongly singular integral opera...The Fourier transform and the Littlewood-Paley theory are used to give the weighted boundedness of a strongly singular integral operator defined in this paper. The paper shows that the strongly singular integral operator is bounded from the Sobolev space to the Lebesgue space.展开更多
Let w be a Muckenhoupt weight and Hwp （JRn） be the weighted Hardy space. In this paper, by using the atomic decomposition of Hwp（Rn）, we will show that the Bochner-Riesz operators TRδ are bounded from Hwp（Rn） t...Let w be a Muckenhoupt weight and Hwp （JRn） be the weighted Hardy space. In this paper, by using the atomic decomposition of Hwp（Rn）, we will show that the Bochner-Riesz operators TRδ are bounded from Hwp（Rn） to the weighted weak Hardy spaces WHwp （Rn） for 0 〈 p 〈 1 and δ = n/p- （n ＋ 1）/2. This result is new even in the unweighted case.展开更多
文摘在不均匀光照条件下,光伏阵列输出特性呈现多峰现象,传统的最大功率点跟踪(maximum power point tracking,MPPT)方法容易陷入局部极值。为了提高复杂阴影下的跟踪速度和跟踪精度,结合改进粒子群算法(improved particle swarm optimization,IPSO)和自适应步长扰动观察法(adaptive perturbation and observation,AP&O)各自的特点,提出了基于IPSO-AP&O算法的改进MPPT控制方法。其中,IPSO算法采用自适应惯性权重因子,在不同搜索阶段能够充分搜索目标函数,然后与AP&O算法结合实现最大功率的稳定输出。仿真结果表明,所提出的IPSO-AP&O算法减少了传统智能算法的迭代过程,能快速跟踪到全局最大功率点,相比其余几种算法而言,在光照强度突变时均具备快速精准的双重跟踪能力,在4种场景下跟踪效率分别为99.86%、99.91%、87.63%、99.79%,能够更好地减小光伏阵列外部条件变化导致的功率损耗,所提出的MPPT控制方法能够较好地适用于光储混合系统,具备工程实用价值。
文摘仿射传播(Affinity propagation,AP)聚类算法是将所有待聚类对象作为潜在的聚类中心,通过对象之间传递的可靠性和有效性信息找到合适的聚类中心,从而计算出相应的聚类结果,但不适用子空间聚类。将粒度计算引入到仿射传播聚类算法中,提出属性与样本同步粒化的AP熵加权软子空间聚类算法(Entropy weighting AP algorithm for subspace clustering based on asynchronous granulation of attributes and samples,EWAP)。EWAP首先去除冗余属性,然后在每次聚类的迭代过程中修改属性的权重值。在满足一定条件迭代终止时,就会得到构成各兴趣度子空间的属性权重值,从而得到属性集的粒化结果以及相应的子空间聚类结果。理论与实验证明EWAP算法既保留了AP算法的优点,又克服了该聚类算法不能进行子空间聚类的不足。
文摘It is proved that, for the nondivergence elliptic equations Σi,jn=1aijuxixj=f, if f belongs to the generalized Morrey spaces Lp, (w), then uxixj ∈ Lp, (w), where u is the W2,p-solution of the equations. In order to obtain this, the author first establish the weighted boundedness for the commutators of some singular integral operators on Lp, (w).
文摘In this paper, the weighted boundedness of parametric Marcinkiewicz integral and its commutator with rough kernels are considered. In addition, the weak type norm inequalities for parametric Marcinkiewicz integral and its commutator with different weight functions and Dini kernel are also discussed.
基金supported in part by National Natural Foundation of China (Grant No. 11161042 and No. 11071250)
文摘In this paper, we shall deal with the boundedness of the Littlewood-Paley operators with rough kernel. We prove the boundedness of the Lusin-area integral μΩs and Littlewood-Paley functions μΩ and μλ^＊ on the weighted amalgam spaces （Lω^q,L^p）^α（R^n）as 1〈q≤α〈p≤∞.
基金the NNSF of China under Grant#10771110NSF of Ningbo City under Grant#2006A610090
文摘For 0 〈 α 〈 mn and nonnegative integers n ≥ 2, m≥ 1, the multilinear fractional integral is defined bywhere →y= （y1, Y2,…, ym） and 7 denotes the m-tuple （f1, f2,…, fm）. In this note, the one- weighted and two-weighted boundedness on Lp （JRn） space for multilinear fractional integral operator I（am） and the fractional multi-sublinear maximal operator Mα（m） are established re- spectively. The authors also obtain two-weighted weak type estimate for the operator Mα（m）.
文摘In this paper, we will obtain the weak type estimates of intrinsic square func- tions including the Lusin area integral, Littlewood-Paley g-function and g^-function on the weighted Morrey spaces L^1,k （w） for 0〈k〈 1 and w ∈ A1.
文摘In this note the authors give the weighted Lp-boundedness for a class of maximal singular integral operators with rough kernel. The result in this note is an improvement and extension of the result obtained by Chen and Lin in 1990.
文摘Let L = -△＋V be a Schrodinger operator acting on L^2（R^n）, n ≥ 1, where V ≠ 0 is a nonnegative locally integrable function on R^n. In this article, we will introduce weighted Hardy spaces Hp （w） associated with L by means of the square function and then study their atomic decomposition theory. We will also show that the Riesz transform △↓L^-1/2 associated with L is bounded from our new space HP（w） to the classical weighted Hardy sp ace HP （ w ） when n / （n ＋ 1 ） 〈 p 〈 1 and w ∈ A 1 ∩ R H（ 2 / p ）＇.
基金Project supported by the National Natural Science Foundation of China (No. 10771110)the Major Project of the Ministry of Education of China (No. 309018)
文摘The Fourier transform and the Littlewood-Paley theory are used to give the weighted boundedness of a strongly singular integral operator defined in this paper. The paper shows that the strongly singular integral operator is bounded from the Sobolev space to the Lebesgue space.
文摘Let w be a Muckenhoupt weight and Hwp （JRn） be the weighted Hardy space. In this paper, by using the atomic decomposition of Hwp（Rn）, we will show that the Bochner-Riesz operators TRδ are bounded from Hwp（Rn） to the weighted weak Hardy spaces WHwp （Rn） for 0 〈 p 〈 1 and δ = n/p- （n ＋ 1）/2. This result is new even in the unweighted case.
