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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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1.3 COORDINATE GEOMETRYwith K <strong>and</strong> φ as given above. Notice that the inverse sine yields two values in the range 0to 2π <strong>and</strong> that there is no real solution to the original equation if |k| > |K| =(a 2 +b 2 ) 1/2 . ◭1.3 Coordinate geometryWe have already mentioned the st<strong>and</strong>ard <strong>for</strong>m <strong>for</strong> a straight-line graph, namelyy = mx + c, (1.35)representing a linear relationship between the independent variable x <strong>and</strong> thedependent variable y. Theslopem is equal to the tangent of the angle the linemakes with the x-axis whilst c is the intercept on the y-axis.An alternative <strong>for</strong>m <strong>for</strong> the equation of a straight line isto which (1.35) is clearly connected byax + by + k =0, (1.36)m = − a b<strong>and</strong> c = − k b .This <strong>for</strong>m treats x <strong>and</strong> y on a more symmetrical basis, the intercepts on the twoaxes being −k/a <strong>and</strong> −k/b respectively.A power relationship between two variables, i.e. one of the <strong>for</strong>m y = Ax n ,canalso be cast into straight-line <strong>for</strong>m by taking the logarithms of both sides. Whilstit is normal in mathematical work to use natural logarithms (to base e, writtenln x), <strong>for</strong> practical investigations logarithms to base 10 are often employed. Ineither case the <strong>for</strong>m is the same, but it needs to be remembered which has beenused when recovering the value of A from fitted data. In the mathematical (basee) <strong>for</strong>m, the power relationship becomesln y = n ln x +lnA. (1.37)Now the slope gives the power n, whilst the intercept on the ln y axis is ln A,which yields A, either by exponentiation or by taking antilogarithms.The other st<strong>and</strong>ard coordinate <strong>for</strong>ms of two-dimensional curves that studentsshould know <strong>and</strong> recognise are those concerned with the conic sections – so calledbecause they can all be obtained by taking suitable sections across a (double)cone. Because the conic sections can take many different orientations <strong>and</strong> scalingstheir general <strong>for</strong>m is complex,Ax 2 + By 2 + Cxy + Dx + Ey + F =0, (1.38)but each can be represented by one of four generic <strong>for</strong>ms, an ellipse, a parabola, ahyperbola or, the degenerate <strong>for</strong>m, a pair of straight lines. If they are reduced totheir st<strong>and</strong>ard representations, in which axes of symmetry are made to coincide15

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