Singularity function

Singularity functions are a class of discontinuous functions that contain singularities, i.e., they are discontinuous at their singular points. Singularity functions have been heavily studied in the field of mathematics under the alternative names of generalized functions and distribution theory. The functions are notated with brackets, as \langle x-a\rangle ^n where n is an integer. The " \langle \rangle " are often referred to as singularity brackets. The functions are defined as: : }{dx^ }\delta(x-a)\, |- | -2 | \frac{d}{dx}\delta(x-a)\, |- | -1 | \delta(x-a)\, |- | 0 | H(x-a)\, |- | 1 | (x-a)H(x-a)\, |- | 2 | (x-a)^2H(x-a) |- | \ge 0 | (x-a)^nH(x-a) |} where: is the Dirac delta function, also called the unit impulse. The first derivative of is also called the unit doublet. The function H(x) is the Heaviside step function: for and for . The value of will depend upon the particular convention chosen for the Heaviside step function. Note that this will only be an issue for since the functions contain a multiplicative factor of for . \langle x-a\rangle^1 is also called the ramp function.

Singularity functions are a class of discontinuous functions that contain singularities, i.e., they are discontinuous at their singular points. Singularity functions have been heavily studied in the field of mathematics under the alternative names of generalized functions and distribution theory. The functions are notated with brackets, as \langle x-a\rangle ^n where n is an integer. The " \langle \rangle " are often referred to as singularity brackets. The functions are defined as: }{dx^ }\delta(x-a)\, |- | -2 | \frac{d}{dx}\delta(x-a)\, |- | -1 | \delta(x-a)\, |- | 0 | H(x-a)\, |- | 1 | (x-a)H(x-a)\, |- | 2 | (x-a)^2H(x-a) |- | \ge 0 | (x-a)^nH(x-a) |} where: is the Dirac delta function, also called the unit impulse. The first derivative of is also called the unit doublet. The function H(x) is the Heaviside step function: for and for . The value of will depend upon the particular convention chosen for the Heaviside step function. Note that this will only be an issue for since the functions contain a multiplicative factor of for . \langle x-a\rangle^1 is also called the ramp function. \int\langle x-a \rangle^n dx = \begin{cases} \langle x-a \rangle^{n+1}, & n w=-3\text{ N}\langle x-0 \rangle^{-1}\ +\ 6\text{ Nm}^{-1}\langle x-2\text{ m} \rangle^0\ -\ 9\text{ N}\langle x-4\text{ m}\rangle^{-1}\ -\ 6\text{ Nm}^{-1}\langle x-4\text{ m} \rangle^0\ Shear force: S=\int w\, dx S=-3\text{ N}\langle x-0\rangle^0\ +\ 6\text{ Nm}^{-1}\langle x-2\text{ m}\rangle^1\ -\ 9\text{ N}\langle x-4\text{ m}\rangle^0\ -\ 6\text{ Nm}^{-1}\langle x-4\text{ m}\rangle^1\, Bending moment: M = -\int S\, dx M=3\text{ N}\langle x-0\rangle^1\ -\ 3\text{ Nm}^{-1}\langle x-2\text{ m}\rangle^2\ +\ 9\text{ N}\langle x-4\text{ m} \rangle^1\ +\ 3\text{ Nm}^{-1}\langle x-4\text{ m}\rangle^2\, Slope: u'=\frac{1}{EI}\int M\, dx Because the slope is not zero at x  = 0, a constant of integration, c , is added u'=\frac{1}{EI}\left(\frac{3}{2}\text{ N}\langle x-0\rangle^2\ -\ 1\text{ Nm}^{-1}\langle x-2\text{ m}\rangle^3\ +\ \frac{9}{2}\text{ N}\langle x-4\text{ m}\rangle^2\ +\ 1\text{ Nm}^{-1}\langle x-4\text{ m}\rangle^3\ +\ c\right)\, Deflection: u=\int u'\, dx u=\frac{1}{EI}\left(\frac{1}{2}\text{ N}\langle x-0\rangle^3\ -\ \frac{1}{4}\text{ Nm}^{-1}\langle x-2\text{ m}\rangle^4\ +\ \frac{3}{2}\text{ N}\langle x-4\text{ m}\rangle^3\ +\ \frac{1}{4}\text{ Nm}^{-1}\langle x-4\text{ m}\rangle^4\ +\ cx\right)\, The boundary condition u  = 0 at x  = 4 m allows us to solve for c  = −7 Nm 2 ==See also== Macaulay brackets Macaulay's method ==References== ==External links== Singularity Functions (Tim Lahey) Singularity functions (J. Lubliner, Department of Civil and Environmental Engineering) Beams: Deformation by Singularity Functions (Dr. Ibrahim A. Assakkaf)

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