Optimization including Convex Optimization and Gradient Descent

温馨提示:

    本文将介绍统计学中的优化知识,凸优化和梯度下降,多为公式推导和图形化展示,较为硬核

优化与深度学习

优化与估计

尽管优化方法可以最小化深度学习中的损失函数值,但本质上优化方法达到的目标与深度学习的目标并不相同。

  • 优化方法目标:训练集损失函数值

  • 深度学习目标:测试集损失函数值(泛化性)

  • 借助图形直观比较

%matplotlib inline
import sys
sys.path.append('path to file storge d2lzh1981')
import d2lzh1981 as d2l
from mpl_toolkits import mplot3d # 三维画图
import numpy as np
def f(x): return x * np.cos(np.pi * x)
def g(x): return f(x) + 0.2 * np.cos(5 * np.pi * x)

d2l.set_figsize((5, 3))
x = np.arange(0.5, 1.5, 0.01)
fig_f, = d2l.plt.plot(x, f(x),label="train error")
fig_g, = d2l.plt.plot(x, g(x),'--', c='purple', label="test error")
fig_f.axes.annotate('empirical risk', (1.0, -1.2), (0.5, -1.1),arrowprops=dict(arrowstyle='->'))
fig_g.axes.annotate('expected risk', (1.1, -1.05), (0.95, -0.5),arrowprops=dict(arrowstyle='->'))
d2l.plt.xlabel('x')
d2l.plt.ylabel('risk')
d2l.plt.legend(loc="upper right")

优化在深度学习中的挑战

  1. 局部最小值
  2. 鞍点
  3. 梯度消失
局部最小值

f(x)=xcosπx f(x) = xcos pi x

def f(x):
    return x * np.cos(np.pi * x)

d2l.set_figsize((4.5, 2.5))
x = np.arange(-1.0, 2.0, 0.1)
fig,  = d2l.plt.plot(x, f(x))
fig.axes.annotate('local minimum', xy=(-0.3, -0.25), xytext=(-0.77, -1.0),
                  arrowprops=dict(arrowstyle='->'))
fig.axes.annotate('global minimum', xy=(1.1, -0.95), xytext=(0.6, 0.8),
                  arrowprops=dict(arrowstyle='->'))
d2l.plt.xlabel('x')
d2l.plt.ylabel('f(x)');
鞍点

函数在一阶导数为零处(驻点)的黑塞矩阵为不定矩阵。

x = np.arange(-2.0, 2.0, 0.1)
fig, = d2l.plt.plot(x, x**3)
fig.axes.annotate('saddle point', xy=(0, -0.2), xytext=(-0.52, -5.0),
                  arrowprops=dict(arrowstyle='->'))
d2l.plt.xlabel('x')
d2l.plt.ylabel('f(x)');

海森矩阵

A=[2fx122fx1x22fx1xn2fx2x12fx222fx2xn2fxnx12fxnx22fxn2] A=left[egin{array}{cccc}{frac{partial^{2} f}{partial x_{1}^{2}}} & {frac{partial^{2} f}{partial x_{1} partial x_{2}}} & {cdots} & {frac{partial^{2} f}{partial x_{1} partial x_{n}}} \ {frac{partial^{2} f}{partial x_{2} partial x_{1}}} & {frac{partial^{2} f}{partial x_{2}^{2}}} & {cdots} & {frac{partial^{2} f}{partial x_{2} partial x_{n}}} \ {vdots} & {vdots} & {ddots} & {vdots} \ {frac{partial^{2} f}{partial x_{n} partial x_{1}}} & {frac{partial^{2} f}{partial x_{n} partial x_{2}}} & {cdots} & {frac{partial^{2} f}{partial x_{n}^{2}}}end{array} ight]

海森矩阵特征值和鞍点还有局部极小值的点的关系

偏导数为零的点

  • 特征值都大于零是局部极小值点
  • 都为负数是局部极大指点
  • 有正有负就是鞍点

x, y = np.mgrid[-1: 1: 31j, -1: 1: 31j]
z = x**2 - y**2

d2l.set_figsize((6, 4))
ax = d2l.plt.figure().add_subplot(111, projection='3d')
ax.plot_wireframe(x, y, z, **{'rstride': 2, 'cstride': 2})
ax.plot([0], [0], [0], 'ro', markersize=10)
ticks = [-1,  0, 1]
d2l.plt.xticks(ticks)
d2l.plt.yticks(ticks)
ax.set_zticks(ticks)
d2l.plt.xlabel('x')
d2l.plt.ylabel('y');
梯度消失
x = np.arange(-2.0, 5.0, 0.01)
fig, = d2l.plt.plot(x, np.tanh(x))
d2l.plt.xlabel('x')
d2l.plt.ylabel('f(x)')
fig.axes.annotate('vanishing gradient', (4, 1), (2, 0.0) ,arrowprops=dict(arrowstyle='->'))

梯度下降

%matplotlib inline
import numpy as np
import torch
import time
from torch import nn, optim
import math
import sys
sys.path.append('path to file storge d2lzh1981')
import d2lzh1981 as d2l

一维梯度下降


证明:沿梯度反方向移动自变量可以减小函数值

泰勒展开:

f(x+ϵ)=f(x)+ϵf(x)+O(ϵ2) f(x+epsilon)=f(x)+epsilon f^{prime}(x)+mathcal{O}left(epsilon^{2} ight)

代入沿梯度方向的移动量 ηf(x)eta f^{prime}(x)

f(xηf(x))=f(x)ηf2(x)+O(η2f2(x)) fleft(x-eta f^{prime}(x) ight)=f(x)-eta f^{prime 2}(x)+mathcal{O}left(eta^{2} f^{prime 2}(x) ight)

f(xηf(x))f(x) fleft(x-eta f^{prime}(x) ight) lesssim f(x)

xxηf(x) x leftarrow x-eta f^{prime}(x)


e.g.

f(x)=x2 f(x) = x^2

def f(x):
    return x**2  # Objective function

def gradf(x):
    return 2 * x  # Its derivative

def gd(eta):
    x = 10
    results = [x]
    for i in range(20):
        # eta 学习率
        x -= eta * gradf(x)
        results.append(x)
    print('epoch 20, x:', x)
    return results

res = gd(0.2)

梯度下降轨迹

def show_trace(res):
    n = max(abs(min(res)), abs(max(res)))
    f_line = np.arange(-n, n, 0.01)
    d2l.set_figsize((3.5, 2.5))
    d2l.plt.plot(f_line, [f(x) for x in f_line],'-')
    d2l.plt.plot(res, [f(x) for x in res],'-o')
    d2l.plt.xlabel('x')
    d2l.plt.ylabel('f(x)')
    

show_trace(res)
学习率

学习率过小 Code:show_trace(gd(0.05))
在这里插入图片描述

学习率过大 Code:show_trace(gd(1.1))
在这里插入图片描述

局部极小值

f(x)=xcoscx f(x) = xcos cx

c = 0.15 * np.pi

def f(x):
    return x * np.cos(c * x)

def gradf(x):
    return np.cos(c * x) - c * x * np.sin(c * x)

# 学习率不合适容易导致
show_trace(gd(2))
show_trace(gd(0.5))

多维梯度下降

f(x)=[f(x)x1,f(x)x2,,f(x)xd] abla f(mathbf{x})=left[frac{partial f(mathbf{x})}{partial x_{1}}, frac{partial f(mathbf{x})}{partial x_{2}}, dots, frac{partial f(mathbf{x})}{partial x_{d}} ight]^{ op}

f(x+ϵ)=f(x)+ϵf(x)+O(ϵ2) f(mathbf{x}+epsilon)=f(mathbf{x})+epsilon^{ op} abla f(mathbf{x})+mathcal{O}left(|epsilon|^{2} ight)

xxηf(x) mathbf{x} leftarrow mathbf{x}-eta abla f(mathbf{x})

# 训练 trainer展示x如何更新
def train_2d(trainer, steps=20):
    x1, x2 = -5, -2
    results = [(x1, x2)]
    for i in range(steps):
        x1, x2 = trainer(x1, x2)
        results.append((x1, x2))
    print('epoch %d, x1 %f, x2 %f' % (i + 1, x1, x2))
    return results
# 垂直于等高线梯度下降
def show_trace_2d(f, results): 
    d2l.plt.plot(*zip(*results), '-o', color='#ff7f0e')
    x1, x2 = np.meshgrid(np.arange(-5.5, 1.0, 0.1), np.arange(-3.0, 1.0, 0.1))
    d2l.plt.contour(x1, x2, f(x1, x2), colors='#1f77b4')
    d2l.plt.xlabel('x1')
    d2l.plt.ylabel('x2')

e.g.

f(x)=x12+2x22 f(x) = x_1^2 + 2x_2^2

eta = 0.1

def f_2d(x1, x2):  # 目标函数
    return x1 ** 2 + 2 * x2 ** 2

def gd_2d(x1, x2):
    return (x1 - eta * 2 * x1, x2 - eta * 4 * x2)

show_trace_2d(f_2d, train_2d(gd_2d))

自适应方法

牛顿法

优势 :

梯度下降“步幅”的确定比较困难

而牛顿法相当于可以通过Hessian矩阵来调整“步幅”。

在牛顿法中,局部极小值也可以通过调整学习率来解决。

x+ϵx + epsilon 处泰勒展开:

f(x+ϵ)=f(x)+ϵf(x)+12ϵf(x)ϵ+O(ϵ3) f(mathbf{x}+epsilon)=f(mathbf{x})+epsilon^{ op} abla f(mathbf{x})+frac{1}{2} epsilon^{ op} abla abla^{ op} f(mathbf{x}) epsilon+mathcal{O}left(|epsilon|^{3} ight)

最小值点处满足: f(x)=0 abla f(mathbf{x})=0, 即我们希望 f(x+ϵ)=0 abla f(mathbf{x} + epsilon)=0, 对上式关于 ϵepsilon 求导,忽略高阶无穷小,有:

f(x)+Hfϵ=0 and hence ϵ=Hf1f(x) abla f(mathbf{x})+oldsymbol{H}_{f} oldsymbol{epsilon}=0 ext { and hence } epsilon=-oldsymbol{H}_{f}^{-1} abla f(mathbf{x})

牛顿法需要计算Hessian矩阵的逆,计算量比较大。

c = 0.5

def f(x):
    return np.cosh(c * x)  # Objective

def gradf(x):
    return c * np.sinh(c * x)  # Derivative

def hessf(x):
    return c**2 * np.cosh(c * x)  # Hessian

# Hide learning rate for now
def newton(eta=1):
    x = 10
    results = [x]
    for i in range(10):
        x -= eta * gradf(x) / hessf(x)
        results.append(x)
    print('epoch 10, x:', x)
    return results

show_trace(newton())
# 牛顿法对于有局部极小值的情况
# 和梯度下降的方法有一样的效果
# 正确的方法还是降低学习率
c = 0.15 * np.pi

def f(x):
    return x * np.cos(c * x)

def gradf(x):
    return np.cos(c * x) - c * x * np.sin(c * x)

def hessf(x):
    return - 2 * c * np.sin(c * x) - x * c**2 * np.cos(c * x)

show_trace(newton())

show_trace(newton(0.5))
在这里插入图片描述

收敛性分析

只考虑在函数为凸函数, 且最小值点上 f(x)>0f''(x^*) > 0 时的收敛速度:

xkx_k 为第 kk 次迭代后 xx 的值, ek:=xkxe_{k}:=x_{k}-x^{*} 表示 xkx_k 到最小值点 xx^{*} 的距离,由 f(x)=0f'(x^{*}) = 0:

0=f(xkek)=f(xk)ekf(xk)+12ek2f(ξk)for some ξk[xkek,xk] 0=f^{prime}left(x_{k}-e_{k} ight)=f^{prime}left(x_{k} ight)-e_{k} f^{prime prime}left(x_{k} ight)+frac{1}{2} e_{k}^{2} f^{prime prime prime}left(xi_{k} ight) ext{for some } xi_{k} inleft[x_{k}-e_{k}, x_{k} ight]

两边除以 f(xk)f''(x_k), 有:

ekf(xk)/f(xk)=12ek2f(ξk)/f(xk) e_{k}-f^{prime}left(x_{k} ight) / f^{prime prime}left(x_{k} ight)=frac{1}{2} e_{k}^{2} f^{prime prime prime}left(xi_{k} ight) / f^{prime prime}left(x_{k} ight)

代入更新方程 xk+1=xkf(xk)/f(xk)x_{k+1} = x_{k} - f^{prime}left(x_{k} ight) / f^{prime prime}left(x_{k} ight), 得到:

xkxf(xk)/f(xk)=12ek2f(ξk)/f(xk) x_k - x^{*} - f^{prime}left(x_{k} ight) / f^{prime prime}left(x_{k} ight) =frac{1}{2} e_{k}^{2} f^{prime prime prime}left(xi_{k} ight) / f^{prime prime}left(x_{k} ight)

xk+1x=ek+1=12ek2f(ξk)/f(xk) x_{k+1} - x^{*} = e_{k+1} = frac{1}{2} e_{k}^{2} f^{prime prime prime}left(xi_{k} ight) / f^{prime prime}left(x_{k} ight)

12f(ξk)/f(xk)cfrac{1}{2} f^{prime prime prime}left(xi_{k} ight) / f^{prime prime}left(x_{k} ight) leq c 时,有:

ek+1cek2 e_{k+1} leq c e_{k}^{2}

预处理 (Heissan阵辅助梯度下降)

xxηdiag(Hf)1x mathbf{x} leftarrow mathbf{x}-eta operatorname{diag}left(H_{f} ight)^{-1} abla mathbf{x}

梯度下降与线性搜索(共轭梯度法)

随机梯度下降

随机梯度下降参数更新

对于有 nn 个样本对训练数据集,设 fi(x)f_i(x) 是第 ii 个样本的损失函数, 则目标函数为:

f(x)=1ni=1nfi(x) f(mathbf{x})=frac{1}{n} sum_{i=1}^{n} f_{i}(mathbf{x})

其梯度为:

f(x)=1ni=1nfi(x) abla f(mathbf{x})=frac{1}{n} sum_{i=1}^{n} abla f_{i}(mathbf{x})

每一个样本的梯度是对整体的梯度的无偏估计

使用该梯度的一次更新的时间复杂度为 O(n)mathcal{O}(n)

随机梯度下降更新公式 O(1)mathcal{O}(1):

xxηfi(x) mathbf{x} leftarrow mathbf{x}-eta abla f_{i}(mathbf{x})

且有:

Eifi(x)=1ni=1nfi(x)=f(x) mathbb{E}_{i} abla f_{i}(mathbf{x})=frac{1}{n} sum_{i=1}^{n} abla f_{i}(mathbf{x})= abla f(mathbf{x})
e.g.

f(x1,x2)=x12+2x22 f(x_1, x_2) = x_1^2 + 2 x_2^2

def f(x1, x2):
    return x1 ** 2 + 2 * x2 ** 2  # Objective

def gradf(x1, x2):
    return (2 * x1, 4 * x2)  # Gradient

def sgd(x1, x2):  # Simulate noisy gradient
    global lr  # Learning rate scheduler
    (g1, g2) = gradf(x1, x2)  # Compute gradient
    (g1, g2) = (g1 + np.random.normal(0.1), g2 + np.random.normal(0.1))
    eta_t = eta * lr()  # Learning rate at time t
    return (x1 - eta_t * g1, x2 - eta_t * g2)  # Update variables

eta = 0.1
lr = (lambda: 1)  # Constant learning rate
show_trace_2d(f, train_2d(sgd, steps=50))

动态学习率

  • 在最开始学习率设计比较大,加速收敛
  • 学习率可以设计为指数衰减或多项式衰减
  • 在优化进行一段时间后可以适当减小学习率来避免振荡

η(t)=ηi if titti+1 piecewise constant η(t)=η0eλt exponential η(t)=η0(βt+1)α polynomial  egin{array}{ll}{eta(t)=eta_{i} ext { if } t_{i} leq t leq t_{i+1}} & { ext { piecewise constant }} \ {eta(t)=eta_{0} cdot e^{-lambda t}} & { ext { exponential }} \ {eta(t)=eta_{0} cdot(eta t+1)^{-alpha}} & { ext { polynomial }}end{array}

def exponential():
    global ctr
    ctr += 1
    return math.exp(-0.1 * ctr)

ctr = 1
lr = exponential  # Set up learning rate
show_trace_2d(f, train_2d(sgd, steps=1000))
def polynomial():
    # 迭代次数
    global ctr
    ctr += 1
    return (1 + 0.1 * ctr)**(-0.5)

ctr = 1
lr = polynomial  # Set up learning rate
show_trace_2d(f, train_2d(sgd, steps=50))

小批量随机梯度下降

读取数据

读取数据

def get_data_ch7():
    data = np.genfromtxt('/home/kesci/input/airfoil4755/airfoil_self_noise.dat', delimiter='	')
    data = (data - data.mean(axis=0)) / data.std(axis=0) # 标准化
    return torch.tensor(data[:1500, :-1], dtype=torch.float32), 
           torch.tensor(data[:1500, -1], dtype=torch.float32) # 前1500个样本(每个样本5个特征)

features, labels = get_data_ch7()
features.shape

数据可视化

import pandas as pd
df = pd.read_csv('path to airfoil_self_noise.dat', delimiter='	', header=None)
df.head(10)

Stochastic Gradient Descent (SGD)函数

def sgd(params, states, hyperparams):
    for p in params:
        p.data -= hyperparams['lr'] * p.grad.data

训练

def train_ch7(optimizer_fn, states, hyperparams, features, labels,
              batch_size=10, num_epochs=2):
    # 初始化模型
    net, loss = d2l.linreg, d2l.squared_loss
    
    w = torch.nn.Parameter(torch.tensor(np.random.normal(0, 0.01, size=(features.shape[1], 1)), dtype=torch.float32),
                           requires_grad=True)
    b = torch.nn.Parameter(torch.zeros(1, dtype=torch.float32), requires_grad=True)

    def eval_loss():
        return loss(net(features, w, b), labels).mean().item()

    ls = [eval_loss()]
    data_iter = torch.utils.data.DataLoader(
        torch.utils.data.TensorDataset(features, labels), batch_size, shuffle=True)
    
    for _ in range(num_epochs):
        start = time.time()
        for batch_i, (X, y) in enumerate(data_iter):
            l = loss(net(X, w, b), y).mean()  # 使用平均损失
            
            # 梯度清零
            if w.grad is not None:
                w.grad.data.zero_()
                b.grad.data.zero_()
                
            l.backward()
            optimizer_fn([w, b], states, hyperparams)  # 迭代模型参数
            if (batch_i + 1) * batch_size % 100 == 0:
                ls.append(eval_loss())  # 每100个样本记录下当前训练误差
    # 打印结果和作图
    print('loss: %f, %f sec per epoch' % (ls[-1], time.time() - start))
    d2l.set_figsize()
    d2l.plt.plot(np.linspace(0, num_epochs, len(ls)), ls)
    d2l.plt.xlabel('epoch')
    d2l.plt.ylabel('loss')

测试

def train_sgd(lr, batch_size, num_epochs=2):
    train_ch7(sgd, None, {'lr': lr}, features, labels, batch_size, num_epochs)

Result

  • train_sgd(1, 1500, 6)
    在这里插入图片描述
  • train_sgd(0.005, 1)
    在这里插入图片描述
  • train_sgd(0.05, 10)
    在这里插入图片描述

简化模型

def train_pytorch_ch7(optimizer_fn, optimizer_hyperparams, features, labels,
                    batch_size=10, num_epochs=2):
    # 初始化模型
    net = nn.Sequential(
        nn.Linear(features.shape[-1], 1)
    )
    loss = nn.MSELoss()
    optimizer = optimizer_fn(net.parameters(), **optimizer_hyperparams)

    def eval_loss():
        return loss(net(features).view(-1), labels).item() / 2

    ls = [eval_loss()]
    data_iter = torch.utils.data.DataLoader(
        torch.utils.data.TensorDataset(features, labels), batch_size, shuffle=True)

    for _ in range(num_epochs):
        start = time.time()
        for batch_i, (X, y) in enumerate(data_iter):
            # 除以2是为了和train_ch7保持一致, 因为squared_loss中除了2
            l = loss(net(X).view(-1), y) / 2 
            
            optimizer.zero_grad()
            l.backward()
            optimizer.step()
            if (batch_i + 1) * batch_size % 100 == 0:
                ls.append(eval_loss())
    # 打印结果和作图
    print('loss: %f, %f sec per epoch' % (ls[-1], time.time() - start))
    d2l.set_figsize()
    d2l.plt.plot(np.linspace(0, num_epochs, len(ls)), ls)
    d2l.plt.xlabel('epoch')
    d2l.plt.ylabel('loss')

train_pytorch_ch7(optim.SGD, {“lr”: 0.05}, features, labels, 10)
在这里插入图片描述

让对手感动,让对手恐惧
原文地址:https://www.cnblogs.com/RokoBasilisk/p/12381111.html