A Statistical View of Entropy — Question 10

Section 20-7 · Physics pages 3370–3371

Question 10 Resetting biased memory has a probability-dependent thermodynamic bound A memory bit is initially 0 with probability .900 and 1 with probability .100. It is reset to 0 while coupled to a 300 K bath. Use Sbit = −kB ∑p ln p and kB = 1.381 × 10−23 J/K. Assume energetically degenerate logical states, zero net internal-energy change, no initial correlations, and a controller returned to its initial state. Positive Qb is heat delivered to the bath. memory reset 300 K bath Qb Win Schematic; labels, not drawing lengths, specify the data. (a) Use the total entropy balance and energy conservation to find the lower bounds on bath heat and work input per reset. (b) Evaluate the bounds for 109 independent bits, and compare the single-bit result with a fair bit. State the total entropy generation in the ideal reversible limit.
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Question 10 - Solution Resetting biased memory has a probability-dependent thermodynamic bound memory reset 300 K bath Qb Win (a) Method and calculation h = −.9 ln .9 −.1 ln .1 ≈.325083, ∆Sbit = −kBh. Sgen = Qb/T −kBh ≥0 ⇒Qb ≥kBTh, Win = Qb. (b) Interpretation and further calculation Wmin = Qb,min ≈1.34682 × 10−21 J per bit. Wmin(109 bits) ≈1.34682 × 10−12 J, Wmin,fair = kBT ln 2 ≈2.87171 × 10−21 J. Sgen,min = 0. In the ideal reversible limit, the bath entropy increase exactly balances the memory entropy decrease. Positive heat rejection does not imply strictly positive total entropy generation. Physical check This bound concerns the stated reset operation and assumptions, not an energy cost for every computational step.

Question 10

Resetting biased memory has a probability-dependent thermodynamic bound

A memory bit is initially 0 with probability .900 and 1 with probability .100. It is reset to 0 while coupled to a 300 K bath. Use Sbit=−kB∑pln⁡pS_{\mathrm{bit}}=-k_B\sum p\ln p and kB=1.381×10−23k_B=1.381\times10^{-23} J/K. Assume energetically degenerate logical states, zero net internal-energy change, no initial correlations, and a controller returned to its initial state. Positive QbQ_b is heat delivered to the bath.

Diagram shown in the original SVG worksheet.

  1. Use the total entropy balance and energy conservation to find the lower bounds on bath heat and work input per reset.

  2. Evaluate the bounds for 10910^9 independent bits, and compare the single-bit result with a fair bit. State the total entropy generation in the ideal reversible limit.

Question 10 - Solution

Resetting biased memory has a probability-dependent thermodynamic bound

Diagram shown in the original SVG worksheet.

(a) Method and calculation

h=−.9ln⁡.9−.1ln⁡.1≈.325083,ΔSbit=−kBh.h=-.9\ln.9-.1\ln.1\approx.325083,\quad\Delta S_{\mathrm{bit}}=-k_Bh.Sgen=Qb/T−kBh≥0⇒Qb≥kBTh,Win=Qb.S_{\mathrm{gen}}=Q_b/T-k_Bh\ge0\Rightarrow Q_b\ge k_BTh,\quad W_{\mathrm{in}}=Q_b.

(b) Interpretation and further calculation

Wmin=Qb,min≈1.34682×10−21Jper bit.W_{\min}=Q_{b,\min}\approx1.34682\times10^{-21}\,\mathrm J\ \text{per bit}.Wmin(109 bits)≈1.34682×10−12J,Wmin⁡,fair=kBTln⁡2≈2.87171×10−21J.W_{\min}(10^9\text{ bits})\approx1.34682\times10^{-12}\,\mathrm J,\quad W_{\min,\mathrm{fair}}=k_BT\ln2\approx2.87171\times10^{-21}\,\mathrm J.Sgen,min=0.S_{\mathrm{gen,min}}=0.In the ideal reversible limit, the bath entropy increase exactly balances the memory entropy decrease. Positive heat rejection does not imply strictly positive total entropy generation.

Physical check

This bound concerns the stated reset operation and assumptions, not an energy cost for every computational step.