Abstract
Chapter 1 is a condensed overview of a raft of techniques which are used in applied mathematics in studying natural phenomena. The chapter focusses on phenomena which occur in continuous systems, modelled by differential equations. Non-dimensionalisation and scaling are treated. For ordinary differential equations, oscillations, hysteresis and resonance are discussed; for partial differential equations, topics covered are waves, nonlinear diffusion, blow-up and reaction–diffusion equations.
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Notes
- 1.
We can understand why T follows the equilibrium curve as follows. We can write (1.26) in terms of suitable dimensionless variables as \(\dot{\Delta}=T_{0}-g(\Delta)\), where g(Δ) is a cubic-like curve similar to the function T 0(Δ) depicted in Fig. 1.9. if T 0 is slowly varying, then T 0=T 0(δt) where δ≪1, and putting τ=δt, we have δdΔ/dτ=T 0(τ)−g(Δ); thus on the slow time scale τ, Δ will tend rapidly to a (quasi-equilibrium) zero of the right hand side.
- 2.
- 3.
- 4.
Geomorphologists would call this surface convex; see Chap. 6.
- 5.
Ice sheets and their marginal movement are discussed further in Chap. 10.
- 6.
We use the summation convention, which implies summation over repeated suffixes.
- 7.
- 8.
See Watson (1944, pp. 199 f.) for these results.
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Fowler, A. (2011). Mathematical Modelling. In: Mathematical Geoscience. Interdisciplinary Applied Mathematics, vol 36. Springer, London. https://doi.org/10.1007/978-0-85729-721-1_1
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