Wednesday, February 19, 2025

x̄ - > 3D visualization of entropy




3D visualization of entropy 

  • Physics/Thermodynamics: A 3D representation of particles dispersing over time.
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Shannon Entropy Proof

Shannon Entropy Proof

Definition of Entropy

Entropy is defined as:

\[ H(X) = - \sum_{i=1}^{n} P(x_i) \log_b P(x_i) \]

Entropy of Equally Likely Outcomes

For a uniform distribution where each outcome has probability \( P(x_i) = \frac{1}{n} \):

\[ H(X) = - \sum_{i=1}^{n} \frac{1}{n} \log_b \frac{1}{n} \]

Simplifying:

\[ H(X) = - n \cdot \frac{1}{n} \cdot \log_b \frac{1}{n} = \log_b n \]

Entropy of Independent Random Variables

If \( X \) and \( Y \) are independent, then their joint probability distribution satisfies:

\[ P(x_i, y_j) = P(x_i) P(y_j) \]

Thus, the entropy of their joint distribution is:

\[ H(X, Y) = - \sum_{i,j} P(x_i, y_j) \log_b P(x_i, y_j) \]

Expanding using independence:

\[ H(X, Y) = - \sum_{i,j} P(x_i) P(y_j) \log_b (P(x_i) P(y_j)) \]

Using the logarithm property \( \log_b(ab) = \log_b a + \log_b b \):

\[ H(X, Y) = - \sum_{i,j} P(x_i) P(y_j) (\log_b P(x_i) + \log_b P(y_j)) \]

Separating the sums:

\[ H(X, Y) = - \sum_{i} P(x_i) \log_b P(x_i) \sum_{j} P(y_j) - \sum_{j} P(y_j) \log_b P(y_j) \sum_{i} P(x_i) \]

Since probabilities sum to 1:

\[ H(X, Y) = H(X) + H(Y) \]

Thus, entropy is additive for independent random variables.

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