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solving-equation
此时matlab中求解方程的基本实例，包括线性和非线性的微分和常数方程(At this point the basic matlab examples for solving equations, including linear and nonlinear differential equations and constants)
- 2011-05-11 21:06:08下载
- 积分：1
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daul_ps_sector_2D_4s
光子筛孔分布的例程，环数不同，用于光子筛成像时使用(Photon sieve distribution routines different rings, used for imaging photon sieve)
- 2013-10-14 20:03:02下载
- 积分：1
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-wavefront
波前曲扭和幅度变化对阵列测向中相干源分辨的影响(Twisted and curved wavefront amplitude variation to distinguish the impact of coherent source direction finding in an array)
- 2013-12-26 12:54:01下载
- 积分：1
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PIDMAC
将PID算法与MAC算法相结合，使具有更好的控制效果。(The PID algorithm and MAC algorithm combined with better control effect.)
- 2009-03-04 15:54:22下载
- 积分：1
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trajectory-analysis
Matlab编写的弹道分析算法-MATLAB源代码(Trajectory analysis algorithms written in Matlab-MATLAB source code)
- 2011-06-29 13:22:12下载
- 积分：1
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IEEE_UWB_PDP
根据IEEE802.15.sg3a信道统计模型产生信道冲激响应，并计算信道的功率延迟剖面(Generates the channel impulse response for a multipath channel according to the statistical model proposed by the IEEE 802.15.SG3a. Evaluates the Power Delay Profile PDP .)
- 2020-09-01 17:38:09下载
- 积分：1
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ship2
船舶电力推进 直接转矩控制 船桨数学模型
仿真结果(ship dtc)
- 2020-11-08 15:50:12下载
- 积分：1
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film
根据对真空蒸发镀膜的分析，在40×40的范围内分别蒸
发：1000、5000、10000、20000、30000个粒子。
利用2维数组记录每个点的粒子数。
初始粒的横纵坐标为0～40的均匀分布。
能量为（15，3）的正态分布。
在基体表面自由行走时损失1的能量。
若该点有粒子，即与其他粒子相遇时损失3的能量。
由低处向高处扩散，每扩散一层，损失4的能量，由高处
向低处扩散，损失3的能量。
当粒子的能量小于等于0时停留下来，该点的粒子数加1。
临界核的尺寸为10个粒子。
根据每个点粒子个数的不同，以不同的灰度显示这些点。
点越亮，则表示该点的膜越厚。
以图形方式显示粒子初始能量的正态分布情况(Based on the analysis of the vacuum evaporation coating, respectively, in the range of from 4040 evaporated: 1000,5000,10000,20000,30000 particles. each point using 2-dimensional array to record the number of particles. The initial grains transverse and longitudinal coordinates of a uniform distribution of 0 to 40. The energy as a normal distribution (15,3). 1 energy losses in the substrate surface to walk. point particles that 3 energy loss in the encounter with the other particles. by the lower diffusion tops every diffusion layer, a loss of 4 energy diffusion from high to low, the energy loss of 3. When the energy of the particles is less than or equal to 0:00 stay down, add 1 to the number of particles that point. critical nucleus size of 10 particles. these points, depending on the number of particles of each point is displayed in a different shade. Point, the brighter, the thicker the point of the fi)
- 2012-11-14 21:33:44下载
- 积分：1
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xiashan
MATLAB 牛顿下山法的一个小程序，原理就不详细说了。因牛顿迭代法受初值选取的限制，为防止迭代发散，对迭代过程再附加一项要求:|f(x(k+1))|<|f(x(k))|,将牛顿法迭代的结果:x(k+1) =x(k)-f(x(k))/f (x(k))和前一近似值x(k)适当加权平均做为新的改进值:x(k+1)=u*x(k+1) +(1-u)*x(k),其中u(0<>
迭代时u取1开始，逐次减半计算，直至附加要求符合为止。实例计算中x(k)=x(0)不变，只更新u和x(k+1)，直至:|f(x(k+1))|<|f(x(k))|（即|f(x(1))|<|f(x(0))|)，然后更新下山因子为u=1,继续以牛顿法迭代。(MATLAB Newton-down a small program, the principle is not explained in detail. Newton iteration by the initial value of the selected limit, in order to prevent additional iterative divergence, the iterative process a request: | f (x (k+1)) | < | f (x (k)) | Newton iteration Results: x (k+1) ' = X (k)-f (x (k))/f' (x (k)) and a previous approximation x (k), appropriately weighted average as a new improved value: x (k+1 ) = u* x (k+1) ' + (1-u)* x (k), where u (0 < u> iteration take successive calculated at 50 until the additional requirements found so far. examples of calculation of X ( k) = x (0) unchanged profile u and x (k+1, hungry) until: | f (x (k+1)) | < | f (x (k)) | (i.e. | f (x (1)) | < | f (x (0)) |), then profile downhill factor for u = 1, to continue to Newton iteration.)
- 2013-05-15 08:52:09下载
- 积分：1
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自适应EEMD程序加信号重构
包含：1、eemd程序2、自适应eemd程序3、自适应eemd程序加信号重构。(Contains: 1, eemd Program 2, Program 3 eemd adaptive adaptive eemd program plus signal reconstruction.)
- 2016-04-12 18:49:09下载
- 积分：1
