TensorFlow Tutorial
- Recommendations for Neural Network Training
- Image Recognition using TensorFlow
- TensorFlow - Forming Graphs
- Gradient Descent Optimization
- TensorFlow - XOR Implementation
- TensorFlow - Optimizers
- Hidden Layers of Perceptron
- Multi-Layer Perceptron Learning
- TensorFlow - Exporting
- TensorFlow - Distributed Computing
- TensorFlow - Keras
- CNN and RNN Difference
- TFLearn and its installation
- TensorFlow - Linear Regression
- Single Layer Perceptron
- TensorFlow - Word Embedding
- TensorBoard Visualization
- Recurrent Neural Networks
- Convolutional Neural Networks
- TensorFlow - Basics
TensorFlow Useful Resources
Selected Reading
- Who is Who
- Computer Glossary
- HR Interview Questions
- Effective Resume Writing
- Questions and Answers
- UPSC IAS Exams Notes
TensorFlow - Forming Graphs
A partial differential equation (PDE) is a differential equation, which involves partial derivatives with unknown function of several independent variables. With reference to partial differential equations, we will focus on creating new graphs.
Let us assume there is a pond with dimension 500*500 square −
N = 500
Now, we will compute partial differential equation and form the respective graph using it. Consider the steps given below for computing graph.
Step 1 − Import pbraries for simulation.
import tensorflow as tf import numpy as np import matplotpb.pyplot as plt
Step 2 − Include functions for transformation of a 2D array into a convolution kernel and simppfied 2D convolution operation.
def make_kernel(a): a = np.asarray(a) a = a.reshape(pst(a.shape) + [1,1]) return tf.constant(a, dtype=1) def simple_conv(x, k): """A simppfied 2D convolution operation""" x = tf.expand_dims(tf.expand_dims(x, 0), -1) y = tf.nn.depthwise_conv2d(x, k, [1, 1, 1, 1], padding = SAME ) return y[0, :, :, 0] def laplace(x): """Compute the 2D laplacian of an array""" laplace_k = make_kernel([[0.5, 1.0, 0.5], [1.0, -6., 1.0], [0.5, 1.0, 0.5]]) return simple_conv(x, laplace_k) sess = tf.InteractiveSession()
Step 3 − Include the number of iterations and compute the graph to display the records accordingly.
N = 500 # Initial Conditions -- some rain drops hit a pond # Set everything to zero u_init = np.zeros([N, N], dtype = np.float32) ut_init = np.zeros([N, N], dtype = np.float32) # Some rain drops hit a pond at random points for n in range(100): a,b = np.random.randint(0, N, 2) u_init[a,b] = np.random.uniform() plt.imshow(u_init) plt.show() # Parameters: # eps -- time resolution # damping -- wave damping eps = tf.placeholder(tf.float32, shape = ()) damping = tf.placeholder(tf.float32, shape = ()) # Create variables for simulation state U = tf.Variable(u_init) Ut = tf.Variable(ut_init) # Discretized PDE update rules U_ = U + eps * Ut Ut_ = Ut + eps * (laplace(U) - damping * Ut) # Operation to update the state step = tf.group(U.assign(U_), Ut.assign(Ut_)) # Initiapze state to initial conditions tf.initiapze_all_variables().run() # Run 1000 steps of PDE for i in range(1000): # Step simulation step.run({eps: 0.03, damping: 0.04}) # Visuapze every 50 steps if i % 500 == 0: plt.imshow(U.eval()) plt.show()
The graphs are plotted as shown below −
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