Earlier analogy note (December 2025)
Retained for the history of the proposal. The capacity and thermodynamic correspondences below are our extensions, not definitions from Werner's Quantity Theory of Credit. Claims about work bounds, entropy tendencies, and early-warning ceilings are unvalidated hypotheses, not results of the current measurement paper. The \(X_C\) sign comparison has been corrected for consistency with the displayed equation.
- Plain-English summary
- Overview
- Correspondence table
- Bank credit creation
- Free energy (F_C) & optional exergy (X_C)
- Maxwell-like relations
- Is it merely a rephrasing?
- What the analogy adds (insights & tests)
- Limitations & scope
- Minimal references
- Disclaimer & status
- App behavior
Plain-English summary (QTM vs QTC & the first/second laws)
What we compare. Two stories about money/credit: the classic Quantity Theory of Money (QTM) [3,4,6] and Werner’s Quantity Theory of Credit (QTC) [9].
- QTM — Quantity Theory of Money (money-first): more money → higher prices, if money moves fast enough.
- QTC — Quantity Theory of Credit (credit-first) [9]: banks create deposits when they lend; what credit is used for matters.
First law (bookkeeping idea).
- QTM: in the classic quantity-theory view [3, 4, 6], changes are explained via money stock, velocity, and policy shocks, without an explicit “capacity” state variable. Here we restate that as a split between (a) policy work and (b) extra mixing of money across uses.
- QTC: same split, but now we also track capacity/headroom on bank balance sheets. Using up headroom shows up like a pressure × volume term (work from constraints).
Second law (one-way tendency).
- Both: random mixing tends to raise our entropy-like index. To reverse it (make it more concentrated) you need structure—policy, rules, guidance.
- Only in QTC: tightening or relaxing capacity shifts the “pressure” of constraints, which changes how hard it is to concentrate or relax the system.
Why QTC adds value. QTC makes the hidden capacity/pressure channel explicit. That lets us distinguish “more random dispersion” from “intentional work by policy or rules” — which is exactly what you want for audit trails and early-warning dashboards.
Overview
The index we informally described above is made precise as follows.Definition. Monetary dispersion entropy (entropy-like, extensive):
\[
S_M \;=\; k\,M_{\mathrm{in}}\,H(q),\quad H(q)\equiv -\sum_i q_i\,\log q_i \tag{1}
\]
where M_in is the actual money-in-circulation over a chosen period/system and q are composition shares (MECE, stable).
Entropy form follows Shannon [12]. Economic applications of entropy/dispersion include Theil’s information-theoretic index [7]. We map ideal mixing \(\Delta S_{mix}=k_B N H(x)\) to money shares \(q\) and scale \(M_{in}\).
Correspondence table
Thermodynamics column is literal; QTM/QTC columns are analogy-level correspondences. Heat/Work entries are “-like” bookkeeping splits, not physical identities.
Notes are hidden behind the ⓘ icons; hover (or tap) to read.
| Variable | Thermodynamics | QTM (money-first) | QTC (credit-first) | Notes |
|---|---|---|---|---|
| Mixing entropy | \(\Delta S_{mix}=k_B N H(x)\) | \( S_M = k\,M_{in}\,H(q) \) | \( S_M = k\,M_{in}\,H(q) \) | |
| Temperature | \( T \) | \( T_L \) | \( T_L \) | |
| Internal energy | \( U \) | \( U_M(S_M) \) | \( U(S_M,V_C,\dots) \) | |
| Volume | \( V \) | — | \( V_C \) | |
| Pressure | \( p \) | — | \( p_C \equiv -\,(\partial U/\partial V_C)_{S_M} \) | |
| Heat (heat-like) | \( \delta Q_{\mathrm{rev}} = T\,dS \) | \( Q_M \sim T_0\,\Delta S_M \) | \( Q_C \sim \bar T_L\,\Delta S_M \) | |
| Work (work-like) | \( \delta W = p\,dV \) | \( W_M \equiv W_{\mathrm{policy}} \) | \( W_C \equiv -\,\bar p_C\,\Delta V_C \;+\; W_{\mathrm{policy}} \) | |
| First law | \( \Delta U \equiv T\,\Delta S + W \) | \( \Delta U_M = T_0\,\Delta S_M + W + \varepsilon \) | \( \Delta U = \bar T_L\,\Delta S_M + W + \varepsilon \) | |
| Second law (monotonicity) | \( \Delta S \ge 0 \) | \( \Delta S_M \ge 0 \) | \( \Delta S_M \ge 0 \) | |
| Helmholtz free energy | \( F \) | \( F_M \equiv U_M - T_0 S_M \) | \( F_C \equiv U - T_0 S_M \) | |
| Exergy / availability | \( X \) | \(X_M \approx U_M - T_0 S_M\) | \( X_C = \Delta U + p_0\Delta V_C - T_0 \Delta S_M \) |
- QTM: Bookkeeping potential \(U_M(S_M)\) so that a first‑law‑like split holds: \(\Delta U_M = T_0\,\Delta S_M + W_{policy} + \varepsilon\). Not a standard variable in classic QTM.
- QTC: Credit state potential \(U(S_M,V_C,\dots)\) with conjugates \(T_L=(\partial U/\partial S_M)_{V_C}\), \(p_C=-(\partial U/\partial V_C)_{S_M}\).
Bank credit creation (within this mapping)
Balance-sheet identity (loans create deposits)
When a bank grants a new loan, it books the loan as an asset and simultaneously creates a matching deposit as a liability. On the customer side, the new deposit is an asset and the loan is a liability. This standard identity is the only accounting ingredient we need.
\[ \Delta U \;\approx\; \bar T_L\,\Delta S_M \;- \; \bar p_C\,\Delta V_C \;+ \; W_{\mathrm{policy}} \;+ \; \varepsilon \tag{2} \]This expresses the credit‑creation energy balance — the “ΔU of credit creation,” decomposing changes into liquidity (T̄L ΔSM), capacity (−p̄C ΔVC), and policy work (Wpolicy).
- \( \Delta S_M \): with \( S_M = k\,M_{\mathrm{in}}\,H(q) \), credit creation typically raises \( M_{\mathrm{in}} \) (scale term) and, via allocation changes, may alter \( H(q) \), pushing \( S_M \) upward.
- \( \Delta V_C \): new lending uses headroom so \( \Delta V_C < 0 \) (capacity declines). Hence the term \( -\bar p_C\, \Delta V_C > 0 \) contributes positively.
- \( W_{\mathrm{policy}} \): includes structural work from regulation, capital injections, guarantees, purchases (QE/collateral ops), etc.
Creation vs repayment (sign conventions)
Notation: \(\Delta M_{\mathrm{in}}\) = change in money-in-circulation over the period. Arrows ↑/↓ denote increase/decrease.
| Variable | Credit creation (new lending > repayments) | Credit contraction (repayments > new lending) |
|---|---|---|
| \(\Delta M_{\mathrm{in}}\) | > 0 | < 0 |
| \(\Delta S_M\) | increase (scale ↑; dispersion may also rise) | decrease (scale ↓; if concentration increases, fall is larger) |
| \(\Delta V_C\) | \(< 0\) (headroom used) | \(> 0\) (headroom restored) |
| \(-\,\bar p_C\, \Delta V_C\) | > 0 | < 0 |
| \(\Delta F_C = \Delta(U - T_0 S_M)\) | sign depends on \(T_0\), dispersion changes, and \(p_C\) | same (case by case) |
Measurement proxies (practical)
- Credit flows/stocks: new loans, margin/credit for securities, corporate bonds/CP issuance (use stock series differences if needed).
- Shares \(q\): use a stable MECE partition by use/sector/instrument and update monthly.
- Capacity \(V_C\): CET1/RWA headroom, LCR/NSFR slack, HQLA-based lending capacity.
- Temperature \(T_L\): composite intensity index from spreads, turnover, and order-book depth (z-scored).
- Pressure \(p_C\): estimate via \(p_C \approx -\Delta U/\Delta V_C\) regressions or policy-shock differences.
Monthly algorithm (implementation steps)
- Aggregate credit flows/stocks \(f_i\); compute shares as \(q_i = f_i/\sum_i f_i\).
- Observe \(M_{\mathrm{in}}\) and compute \(S_M = k\,M_{\mathrm{in}}\,H(q)\).
- Build \(V_C\) from RWA, LCR/NSFR, and HQLA metrics.
- Compute \(T_L\) from market microstructure (spreads/turnover/depth).
- Evaluate \(\Delta U = \bar T_L \Delta S_M - \bar p_C \Delta V_C + W_{policy} + \varepsilon\).
- Detect events: label months with \(\Delta M_{\mathrm{in}}\) spikes (or net credit inflow if available) as credit-creation periods and decompose contributions.
Free energy \(F_C\) — and optional exergy \(X_C\)
Why this exists. We want a single scalar potential for the QTC side that (i) decreases as dispersion \(S_M\) increases under a fixed environment, and (ii) provides an upper bound on structured work over a cycle. A Helmholtz-style free energy plays exactly this role.
Definition. With a state potential \(U(S_M,V_C,\dots)\) and fixed environment \(T_0\): \[ F_C \equiv U - T_0 S_M,\qquad dF_C = -\,p_C\,dV_C + \delta W_{other} \tag{3} \]
It serves as an early-warning gauge: when \(\Delta F_C \to 0\), policy headroom for structured work dries up.
Exergy \(X_C\) (optional, environment-dependent)
When an ambient pressure-like term matters, use the exergy-like availability: \[ X_C = (U-U_0) + p_0\,(V_C - V_{C0}) - T_0\,(S_M - S_{M0}) \tag{4} \]
With fixed \(V_C\), it equals \(F_C-F_{C0}\), where \(F_C=U-T_0S_M\) and \(F_{C0}=U_0-T_0S_{M0}\). This is an algebraic comparison with the reference state, not a measured work bound. The value depends on the chosen environment \((T_0,p_0)\).
Gibbs free energy \(G_C\) (optional, fixed \(p_0\) environment)
When both temperature- and pressure-like environments are treated as fixed, the Gibbs free energy is convenient: \[ G_C \equiv U + p_0\,V_C - T_0\,S_M,\qquad dG_C = V_C\,dp_0 - S_M\,dT_0 + \delta W_{other} \] In practice, we use \(F_C\) for fixed-volume analyses and \(G_C\) when an ambient pressure-like \(p_0\) is the natural control.
Maxwell-like relations (integrability)
Given the state potential \(U(S_M,V_C,\dots)\) implied by the correspondence table and the \(F_C\) definition above, mixed partials must commute, giving a Maxwell-like condition:
\[ T_L = \left(\frac{\partial U}{\partial S_M}\right)_{V_C},\quad p_C = -\left(\frac{\partial U}{\partial V_C}\right)_{S_M} \;\Rightarrow\; \left(\frac{\partial T_L}{\partial V_C}\right)_{S_M} = -\left(\frac{\partial p_C}{\partial S_M}\right)_{V_C} \tag{5} \]Violations in data falsify the mapping (i.e., chosen variables are not state-like or proxies are inadequate).
Is this merely a rephrasing?
Mathematically it is a change of coordinates that isolates scale and dispersion. It becomes non-trivial because it yields: (i) falsifiable integrability constraints (Maxwell-like), (ii) a clean separation of policy work vs dispersion, and (iii) an exergy/free-energy lens for early-warning ceilings via \(X_C\) or \(F_C\).
What the analogy adds (insights & tests)
- Integrability test (Maxwell-like): Estimate \(T_L(S_M,V_C)\), \(p_C(S_M,V_C)\); check \((\partial T_L/\partial V_C)_{S_M} \approx - (\partial p_C/\partial S_M)_{V_C}\). Persistent failure ⇒ mapping/proxies are wrong.
- Work vs dispersion: Decompose \(\Delta U = \bar T_L\,\Delta S_M - \bar p_C\,\Delta V_C + W_{policy}\) to separate random mixing from structured/policy effects.
- Free-energy/exergy ceilings: Use \(F_C\) or \(X_C\) as early-warning gauges when they approach zero under chosen boundaries.
- Loop area (hysteresis): Non-zero loop area in \((p_C,V_C)\) over policy cycles measures dissipative stress.
Limitations & scope
- Category dependence: \(S_M\) depends on how uses/sectors are binned; require robustness checks.
- Proxy noise: \(T_L, V_C, p_C\) are noisy proxies; mis-measurement can break Maxwell-like relations.
- Quasi-static only: Fast crises and regime shifts violate the smooth state-variable picture.
- Non-physical: No microscopic “money particles” are assumed; this is structured bookkeeping, not physics.
- Identification: Policy and shocks move terms jointly; causal claims need proper empirical design.
- Scaling conventions: Parameters like \(k\) are conventional; report normalized, sensitivity-tested metrics.
- No guarantee of physical laws. Nothing here asserts or guarantees that macro-financial data obey the physical first or second laws; all mappings are analogy-level and subject only to empirical testing.
Minimal references (selected)
- [1] Kocherlakota, N. R. (1998). “Money is Memory.” Journal of Economic Theory 81(2): 232–251.
- [2] Kocherlakota, N. R. (2002). “Money is Memory.” Minneapolis Fed Quarterly Review 26(1): 2–10.
- [3] Fisher, I. (1911). The Purchasing Power of Money. Macmillan.
- [4] Friedman, M. (1956). “The Quantity Theory of Money—A Restatement.” In Studies in the Quantity Theory of Money (ed. Friedman). University of Chicago Press.
- [5] Friedman, M., & Schwartz, A. J. (1963). A Monetary History of the United States, 1867–1960. Princeton University Press.
- [6] Laidler, D. (1985, 3rd ed.). The Demand for Money: Theories, Evidence, and Problems. Harper & Row.
- [7] Theil, H. (1967). Economics and Information Theory. North-Holland.
- [8] Bank of England (McLeay, Radia, Thomas) (2014). “Money creation in the modern economy.” Quarterly Bulletin.
- [9] Werner, Richard A. (2011 keynote; 2012 journal; 2014 article). “Quantity Theory of Credit” program and bank money creation evidence. International Review of Financial Analysis.
- [10] Borio & White (2004). “Whither monetary and financial stability?” BIS Working Paper 147.
- [11] Fontana, G. (2004). “Rethinking endogenous money.” Metroeconomica.
- [12] Shannon, C. E. (1948). “A Mathematical Theory of Communication.” Bell System Technical Journal.
- [13] Jaynes, E. T. (1957). “Information Theory and Statistical Mechanics.” Physical Review.
- [14] Callen, H. B. (1985, 2nd ed.). Thermodynamics and an Introduction to Thermostatistics. Wiley.
- [15] Zemansky, M. W., & Dittman, R. H. (1997, 7th ed.). Heat and Thermodynamics. McGraw-Hill.
- [16] Foley, D. K. (1994). “A statistical equilibrium theory of markets.” Journal of Economic Theory.
- [17] Drăgulescu, A., & Yakovenko, V. M. (2000). “Statistical mechanics of money.” European Physical Journal B.
- [18] Wall, G. (1977). “Exergy—a useful concept.” Chalmers University preprint; later textbooks.
Disclaimer & status. This is ongoing independent research. It is provided as-is for information only, not as investment, legal, tax, policy, or regulated financial advice. Using this site does not create a client relationship. Findings may change as validation continues.
App behavior
- Monthly build computes \(S_M\), \(T_L\), loop_area (PLD), and \(X_C\) from public data.
- Interactive report (with PNG fallbacks): Open report
- Repository: GitHub repo