The Limits of Science: Science, Scientism and a Theistic Universe [Sermon]
- Anush A. John

- Jun 23
- 10 min read
Updated: Jul 20
June 2026, Krabi, Thailand
Science is a rigorous method of empirical investigation grounded in observation, experimentation, and the testing of falsifiable hypotheses. It relies on systematic evidence-gathering and peer review to build knowledge about the natural world.
Science vs Theology on Authority
Science vs Scientism
Scientism is the view that natural sciences are the only legitimate way of obtaining knowledge of reality. It claims that if something cannot be tested through the scientific method, it is not genuine knowledge.
The Limitations of Science (What Science Cannot Explain)
I. FOUNDATIONS OF KNOWLEDGE & RATIONALITY
1. The Epistemological Foundation of Science
Why the scientific method assumes uniformity of nature, logical inference, and reliable reason
2. The Basis for Rationality and Truth
Why mind-world correspondence exists; why truth exists at all
3. The Reliability of Human Reasoning About Non-Empirical Matters
How we have justified confidence in reasoning about metaphysics, mathematics, and logic
4. The Origin and Intelligibility of Mathematical Truth
Why abstract mathematics so precisely describes physical reality
II. METAPHYSICS & EXISTENCE
5. The Cosmological Question: Why Anything Exists
What explains the existence of contingent reality and the laws of physics
6. Fine-Tuning of Physical Constants
Why universal constants are calibrated to permit life
7. The Origin of Biological Information
How specified, complex information arises in genetic systems
III. CONSCIOUSNESS & AGENCY
8. The Problem of Consciousness
Why subjective experience cannot be fully reduced to physical processes
9. Free Will and Moral Responsibility
How genuine human agency coexists with physical determinism
IV. ETHICS & VALUES
10. The Origin of Objective Moral Values
What grounds objective morality independent of evolution or preference
11. Human Dignity and Rights
What grounds intrinsic human worth and universal rights
12. Guilt, Redemption, and Moral Restoration
Why humans experience guilt and whether genuine restoration is possible
13. Conscience and Moral Obligation
The inner compulsion toward right action and binding moral duties
V. MEANING & TRANSCENDENCE
14. Meaning and Purpose in Human Existence
Why human life has significance and direction in a random universe
15. The Universality of Religious Experience
Why humans across all cultures seek transcendence
16. Beauty and Aesthetic Experience
Why beauty has non-utilitarian power and inspires transcendence
VI. HISTORICAL & THEOLOGICAL
The best explanation for disciples' transformation and early Christianity's growth
How to reconcile evil with an omnipotent, good God
The Origin of the Universe
1. An Eternal Universe
2. The Evidence for a Temporal Beginning
a. The Expansion of the Universe
Einstein's relativity (1915): Space and time are linked and dynamic.
Lemaître (1927): predicted that the universe is expanding.
Hubble (1929): Observed that distant galaxies are moving away from us, and farther ones move faster.
b. Cosmic Microwave Background Radiation (CMB)
3. The Big Bang (Temporal Beginning)
a. Mathematical Frameworks For The Big Bang
Framework /Equation | Originator(s) | Year | Purpose | Key Equation(s) | Role in Big Bang |
|---|---|---|---|---|---|
General Relativity (Field Equations) | Albert Einstein | 1915 | Describes gravity as curvature of spacetime; foundation for all cosmological models | Gμν + Λgμν = (8πG/c⁴)Tμν | Foundational: Shows spacetime can expand/contract; enables dynamic universe solutions |
Schwarzschild Metric | Karl Schwarzschild | 1916 | Describes spacetime around a spherical mass; earliest exact solution to Einstein equations | ds² = -(1-2GM/c²r)c²dt² + (1-2GM/c²r)⁻¹dr² + r²(dθ² + sin²θdφ²) | Foundation for understanding gravitational physics; precursor to cosmological metrics |
Friedmann Equations | Alexander Friedmann | 1922 | Describe expansion/contraction rate of universe; relate expansion to density | (da/dt)²/a² = (8πGρ/3) - k/a² + Λ/3 and d²a/dt² = -(4πG/3)(ρ + 3p/c²)a + (Λ/3)a | Core equations for Big Bang cosmology - govern how universe expands from initial singularity |
Friedmann-Lemaître-Robertson-Walker (FLRW) Metric | Friedmann, Lemaître, Robertson, Walker | 1922-1936 | Describes geometry of homogeneous, isotropic expanding universe | ds² = -c²dt² + a(t)²[dr²/(1-kr²) + r²(dθ² + sin²θdφ²)] | Describes the spacetime of expanding universe - mathematical foundation for all Big Bang models |
Lemaitre's Primeval Atom Solution | Georges Lemaître | 1927-1931 | Applied Friedmann equations to predict universe began from single point | Solution to Friedmann equations with finite initial radius → 0 | Theoretical foundation of Big Bang concept - shows universe must have had a beginning |
Hubble's Law (Observational) | Edwin Hubble | 1929 | Empirical relationship between distance and recession velocity | v = H₀d (where H₀ ≈ 70 km/s/Mpc) | Observational confirmation - proves Friedmann/Lemaître predictions correct |
Cosmological Constant (Λ) | Einstein, Friedmann, others | 1915-1920s | Term in Einstein equations representing vacuum energy density | Λgμν term in Einstein field equations | Becomes critical in modern Big Bang: explains accelerating expansion (dark energy) |
Equation of State for Matter | Various | 1920s+ | Relates pressure to density for different substances | p = wρc² (where w varies: w=0 for matter, w=1/3 for radiation) | Determines how universe expands in different eras: radiation-dominated, matter-dominated |
Conservation Laws in Expanding Universe | Friedmann, others | 1920s | Energy and momentum conservation in expanding spacetime | dρ/da + 3(ρ+p/c²)/a = 0 | Describes how density changes as the universe expands |
Big Bang Nucleosynthesis (BBN) Equations | Alpher, Gamow, Herman | 1948 | Describes nuclear reactions in early hot universe | Boltzmann equations for nuclear reaction rates: dn/dt = ... | Predicts light element abundances (H, He, Li) from first 3 minutes |
Thermal History of Universe | Gamow, others | 1948 | Evolution of temperature/energy as universe expands | T(t) ∝ 1/√t for radiation-dominated era | Shows how temperature drops as universe expands from initial hot state |
Boltzmann Equation (Cosmological) | Boltzmann; applied by Gamow | 1920s-1948 | Describes distribution of particles and radiation in early universe | ∂f/∂t + v·∇f + F·∇v f = C[f] (collision term) | Governs particle behavior in extreme early universe conditions |
Radiative Transfer Equations | Various | 1950s+ | Describes photon propagation through expanding universe | dI/ds = -κI + (emissivity) | Used to model CMB formation and propagation |
Inflation Theory (Scalar Field) | Alan Guth, Andrei Linde | 1980-1986 | Describes exponential expansion in first fraction of second | φ̈ + 3H φ̇ + dV/dφ = 0 (scalar field equation) | Solves flatness, horizon, and monopole problems; explains universe's initial conditions |
Scalar Potential (Inflation) | Guth, Linde, others | 1980+ | Energy density driving inflation | V(φ) - various potentials (chaotic, new, hybrid inflation) | Determines exact inflationary dynamics and perturbations |
Perturbation Theory (Linear) | Lifshitz, Bardeen, others | 1946-1980 | Describes small density fluctuations in expanding universe | δk̈ + 2H δk̇ + (k²/a² + d²V/dφ²) δk = 0 | Explains how small quantum fluctuations grew into galaxies |
Power Spectrum of Perturbations | Mukhanov, Chibisov, Guth, others | 1981-1985 | Distribution of fluctuation amplitudes across scales | P(k) ∝ k^n (where n ≈ 1 for scale-invariant spectrum) | Predicts pattern of density fluctuations observed in CMB and galaxy distribution |
Einstein-de Sitter Model | Einstein, de Sitter | 1917-1932 | Simple cosmological model: flat, matter-dominated, no dark energy | a(t) ∝ t^(2/3) | Historically important; approximation for universe before dark energy discovered |
Λ-CDM Model (Standard Cosmological Model) | Many contributors (Perlmutter, Riess, et al.) | 1998+ | Current best-fit model: Λ (dark energy) + Cold Dark Matter + baryons | Friedmann equations with Λ, Ωm ≈ 0.3, ΩΛ ≈ 0.7, Ωk ≈ 0 | Modern Big Bang framework - describes 13.8 billion year cosmic evolution |
Quantum Field Theory (QFT) in Curved Spacetime | Hawking, DeWitt, others | 1970s+ | Describes quantum fields in expanding spacetime | [φ(x),π(x')] = iℏδ(x-x') (field commutation relations in curved space) | Explains particle creation in early universe; basis for inflation quantum fluctuations |
Quantum Gravity (Loop Quantum Cosmology) | Ashtekar, Bojowald | 2000s+ | Attempts to quantize spacetime geometry itself | Difference equations replacing differential equations at Planck scale | Addresses singularity problem: suggests bounce instead of infinite density at t=0 |
Inflationary Perturbation Spectrum | Mukhanov, others | 1985+ | Quantum fluctuations during inflation become classical perturbations | δφk(η) = (H/√2k³ω)[ηk aₖ + ηk† aₖ†] | Explains origin of seed fluctuations for all structure in universe |
Recombination Physics | Peebles, Zeldovich, others | 1960s-1990s | Describes when electrons bind to nuclei; universe becomes transparent | Saha equation for ionization balance; radiative transfer | Explains formation of CMB; describes era 380,000 years after Big Bang |
Dark Energy Equation of State | Observational cosmology | 1998+ | Characterizes mysterious accelerating expansion component | w = p/ρc² ≈ -1 for dark energy (or possibly varying) | Essential for modern Big Bang: universe's fate depends on dark energy properties |
Distance Measures in Expanding Universe | Hogg, others | 1990s+ | Different distance definitions in curved, expanding spacetime | Comoving distance, luminosity distance, angular diameter distance | Allows precise comparison of observations at different redshifts |
Redshift-Distance Relation | Lemaitre, Hubble; formalized later | 1920s-1950s | Converts observed redshift to distance and lookback time | z = a₀/a - 1 (redshift-scale factor relation) | Allows us to see back in time; fundamental observational tool |
Age of Universe from Hubble Constant | Hubble, Lemaître, Gamow | 1929+ | Calculate cosmic age from current expansion rate | t₀ ≈ 1/H₀ (simplified; more complex with dark energy) | Determines that Big Bang occurred ~13.8 billion years ago |
Baryon Acoustic Oscillations (BAO) | Peebles, others; observed by SDSS | 1970s-2005 | Sound waves in early plasma leave imprint in galaxy distribution | Characteristic scale ~150 Mpc (comoving) from primordial sound speed | Provides "standard ruler" to measure cosmic expansion history |
b. Confirmation of the Big Bang
Prediction | Predicted By | Year | Observation/Finding | Observed By | Year | Match? |
|---|---|---|---|---|---|---|
Universe is expanding | Lemaître | 1927 | Galaxies receding with distance-velocity relationship (v = H₀d) | Hubble, others | 1929–present | ✓ Confirmed |
Universe had a beginning (primeval atom) | Lemaître | 1927–1931 | Backward extrapolation shows all matter compressed to single point ~13.8 billion years ago | Cosmological calculations | 1960s–present | ✓ Confirmed |
Cosmic Microwave Background (CMB) exists | Gamow, Alpher, Herman | 1948 | Isotropic microwave radiation detected from all directions in space | Penzias & Wilson, others | 1964–present | ✓ Confirmed |
CMB temperature ~5 Kelvin | Alpher & Herman | 1948 | CMB temperature measured at 2.7 Kelvin (−270.5°C) | Penzias & Wilson, Planck satellite | 1964–2018 | ~ Close |
Helium abundance ~25% of primordial matter | Alpher & Gamow (BBN) | 1948 | Measured He abundance in old stars and gas clouds: 23–25% by mass | Spectroscopy, Hubble observations | 1960s–present | ✓ Confirmed |
Deuterium abundance (heavy hydrogen) in specific ratio | BBN (Alpher, Gamow, Herman) | 1948 | Deuterium-to-hydrogen ratio matches BBN predictions within 10% | Spectrography, radio telescopes | 1970s–present | ✓ Confirmed |
Lithium-7 abundance in primordial abundance | BBN (Alpher, Gamow) | 1948 | Observed Li-7 abundance in oldest stars; subtle discrepancy with theory (lithium problem) | Stellar spectroscopy | 1990s–present | ~ Tension |
CMB should be almost perfectly isotropic (uniform) | Friedmann, Lemaître (FLRW) | 1922–1927 | CMB isotropy confirmed to 1 part in 100,000; tiny anisotropies detected | COBE, WMAP, Planck | 1992–2018 | ✓ Confirmed |
CMB temperature varies slightly with direction (dipole) | Cosmological models | 1970s | Dipole anisotropy detected: one direction ~3K, opposite ~2.4K (Earth's motion relative to CMB) | COBE, WMAP | 1977–1990s | ✓ Confirmed |
CMB anisotropies have specific power spectrum (acoustic peaks) | Inflation theory (Mukhanov, others) | 1985 | Three acoustic peaks observed in CMB power spectrum at predicted scales (150 Mpc) | BOOMERANG, WMAP, Planck | 2000–2018 | ✓ Confirmed |
Age of universe calculable from Hubble constant | Hubble, cosmology | 1929 | Universe age calculated: 13.8 ± 0.02 billion years (from H₀ and Λ-CDM model) | Planck, other surveys | 2013–present | ✓ Confirmed |
Universe is spatially flat (Ωk ≈ 0) | Inflation theory (Guth, Linde) | 1980–1986 | Spatial curvature measured: |Ωk| < 0.005 (essentially flat) | WMAP, Planck, BAO | 2003–2018 | ✓ Confirmed |
Inflation smooths out inhomogeneities and produces flatness | Guth, Linde, others | 1980–1986 | Universe observed to be remarkably homogeneous and flat on large scales | Galaxy surveys, CMB observations | 1990s–present | ✓ Confirmed |
Quantum fluctuations during inflation seed density perturbations | Inflationary cosmology | 1985 | CMB anisotropies match predicted power spectrum from inflation-generated perturbations | WMAP, Planck | 2003–2018 | ✓ Confirmed |
Primordial perturbation spectrum should be nearly scale-invariant | Inflationary theory | 1985 | Power spectrum exponent measured: ns = 0.961 ± 0.013 (nearly 1 = scale-invariant) | Planck | 2018 | ✓ Confirmed |
Galaxy distribution traces matter density fluctuations | Perturbation theory | 1946+ | Large-scale galaxy distribution matches predicted density power spectrum from CMB anisotropies | SDSS, 2dF, others | 2000s–present | ✓ Confirmed |
Baryon Acoustic Oscillations (BAO) at ~150 Mpc scale | Peebles, others | 1970s (predicted); 2005 (observed) | Sound wave imprint in galaxy distribution confirmed at 147.7 ± 3.8 Mpc | SDSS, DES, others | 2005–present | ✓ Confirmed |
Small-scale density perturbations grow into galaxies and clusters | Structure formation theory | 1970s+ | Simulations match observed galaxy distributions; first galaxies form ~200 million years after Big Bang | N-body simulations, JWST | 1990s–present | ✓ Confirmed |
Distant galaxies are younger/different from nearby ones | BBT predictions | 1990s | Distant (old) galaxies look morphologically different, more chaotic, still assembling | Hubble Deep Field, JWST | 1995–present | ✓ Confirmed |
Expansion accelerating due to dark energy (Λ) | Einstein (1917), rediscovered cosmology | 1998 | Type Ia supernovae dimmer than expected; expansion rate increasing | Perlmutter, Riess, Schmidt | 1998–present | ✓ Confirmed |
Dark energy comprises ~68% of universe's energy density | Λ-CDM model | 1998 | Multiple probes (SNe, CMB, BAO) converge: ΩΛ ≈ 0.683 ± 0.005 | Planck, Pantheon survey | 2018 | ✓ Confirmed |
Dark matter comprises ~27% of universe's energy density | Structure formation theory; Vera Rubin | 1970s–1998 | Galaxy rotation curves, gravitational lensing, CMB anisotropies all require dark matter | Multiple observations | 1978–present | ✓ Confirmed |
Radiation-dominated era in early universe | BBN, Friedmann equations | 1948 | Big Bang Nucleosynthesis predictions consistent with era when radiation dominated | Theoretical consistency | 1960s+ | ✓ Consistent |
Matter-dominated era follows radiation era | Friedmann equations | 1922+ | Transition occurred ~60,000 years after Big Bang; current universe matter-dominated | Cosmological models | Calculated from theory | ✓ Consistent |
Recombination occurs ~380,000 years after Big Bang | Peebles, Zeldovich | 1965–1970s | CMB last-scattering surface at redshift z ≈ 1,089; occurs at calculated epoch | WMAP, Planck | 2003–2018 | ✓ Confirmed |
Universe opaque before recombination, transparent after | Recombination physics | 1960s+ | Cannot see beyond CMB (z > 1,089); universe fully ionized before z ≈ 1,089 | Direct observation limit | Observed fact | ✓ Confirmed |
Gravitational lensing distorts distant galaxy images | General Relativity (Einstein, 1916) | 1916 | Massive structures bend light from distant objects; observed extensively | HST, Planck, galaxy surveys | 1990s–present | ✓ Confirmed |
Gravitational waves from early universe imprinted on CMB | Inflation theory | 1985 | Search ongoing for primordial B-mode polarization; tight limits from Planck | Planck, future experiments | 2018–ongoing | ~ Pending |
CMB polarization consistent with Thomson scattering | Cosmological models | 1990s | E-mode polarization detected; pattern matches predictions | WMAP, Planck | 2006–2018 | ✓ Confirmed |
Hubble tension: H₀ discrepancy between early and late universe | Observed discrepancy | 2019+ | CMB predicts H₀ ≈ 67 km/s/Mpc; supernovae measure ≈ 73 km/s/Mpc (5σ tension) | Planck, local measurements | 2019–present | ✗ Tension |
Matter density Ωm ≈ 0.315 (baryons + dark matter) | Λ-CDM model fitting | 1998 | Multiple probes converge: Ωm ≈ 0.315 ± 0.007 | Planck, galaxy surveys | 2018 | ✓ Confirmed |
Baryon density Ωb ≈ 0.049 (ordinary matter) | BBN predictions, Λ-CDM | 1948 (BBN); 1998 (Λ-CDM) | Baryon density constrained by BBN and CMB: Ωb ≈ 0.0493 ± 0.0008 | Planck | 2018 | ✓ Confirmed |
4. The Cosmological Argument
Everything that begins to exist has a cause.
The universe began to exist.
Therefore, the universe has a cause.
Must be uncaused (or infinite regress occurs)
Must be timeless or eternal
Must be necessary rather than contingent
Must possess sufficient power to create the universe
The Argument from Beauty
Beauty is the quality of being pleasing, attractive, or aesthetically satisfying to the senses or mind.
Different kinds of Beauty
Physical Beauty
Artistic Beauty
Intellectual Beauty
Natural Beauty
Character Beauty
How can we explain beauty?
1. The Explanatory Gap in Aesthetic Neuroscience
2. The Problem of Excessive Beauty
3. The Meaning-Bestowing Function of Beauty
The books or the music in which we thought the beauty was located will betray us if we trust to them; it was not in them, it only came through them, and what came through them was longing. These things—the beauty, the memory of our own past—are good images of what we really desire; but if they are mistaken for the thing itself, they turn into dumb idols, breaking the hearts of their worshippers. For they are not the thing itself; they are only the scent of a flower we have not found, the echo of a tune we have not heard, news from a country we have never yet visited. C. S. Lewis, The Weight of Glory.

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