By Snieder R.

Not like conventional textbooks for college kids and pros within the actual sciences, this e-book provides its fabric within the type of difficulties. the second one version includes new chapters on dimensional research, variational calculus, and the asymptotic assessment of integrals. The booklet can be utilized by way of undergraduates and lower-level graduate scholars. it may possibly function a stand-alone textual content, or as a resource of difficulties and examples to counterpoint different textbooks. First version Hb (2001): 0-521-78241-4 First variation Pb (2001): 0-521-78751-3

**Read or Download A Guided Tour of Mathematical Methods: For the Physical Sciences, Edition: 2ed. PDF**

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**Extra info for A Guided Tour of Mathematical Methods: For the Physical Sciences, Edition: 2ed.**

**Example text**

And a perturbation δr in the position vector along a contour line. f f = const. r Fig. 3 Contour lines deﬁned by the condition f = const. and a perturbation δr in the position vector in an arbitrary direction. perpendicular to the surface f = const. Now that we know this, the gradient can still point in two directions because one can move in two directions perpendicular to a surface. 3 where we consider a step δr in an arbitrary direction. 10) where θ is the angle between ∇ f and δr. The change δ f is largest when the vectors ∇ f and δr point in the same direction because in that case cos θ is equal to its maximum value of 1, that is when θ = 0.

Paradoxically, Berry and Klein [15] showed in their analysis of “transparent mirrors” that for the special case of a large stack of layers with random transmission coefﬁcient the total transmission coefﬁcient is the product of the transmission coefﬁcients of the individual layers, despite the fact that multiple reﬂections play a crucial role in this process. 4 Spherical and cylindrical coordinates Many problems in mathematical physics exhibit a spherical or cylindrical symmetry. For example, the gravity ﬁeld of the Earth is to ﬁrst order spherically symmetric.

Note that the last two equations immediately give T and R once A and B are known. The ﬁrst two equations give A and B. Problem b Show that TL , (1 − R L R R ) TL R R . 38) This is a puzzling result, the right-going wave A between the layers not only contains the transmission coefﬁcient of the left layer TL but also an additional term 1/(1 − R L R R ). Problem c Make a series expansion of 1/(1 − R L R R ) in the quantity R L R R and show that this term accounts for the waves that bounce back and forth between the two stacks.