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Mathematics Reference by Prof Miller
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Mathematics reference David Miller
Quantum Mechanics for Scientists and Engineers On-Line Course 1
Elementary mathematical expressions Quadratic equations
2 2a b a b a b (1) The solutions to the general quadratic equation
2 0ax bx c (2) are
2 4
2b b acx
a (3)
Taylor and Maclaurin series (power-series expansion) The Taylor series
2 2
21! 2! !
n n
na a a
x a x a x adf d f d ff x f adx dx n dx
(4)
gives a useful way of approximating a function near to some specific point x a , giving a power-series expansion in nx a for the function near that point. The Maclaurin series
2 2 20 0 0
01! 2! !
n n
nx df x d f x d ff x fdx dx n dx
(5)
is a special case of the Taylor series where we are expanding around the point 0x . Power-series expansions of common functions
For small a, the Maclaurin expansions of various common functions are, to first order
1 1 / 2a a (6) 1 1
1a
a (7)
sin a a (8) tan a a (9)
2
cos 12aa (10)
exp 1a a (11)
Mathematics reference David Miller
Quantum Mechanics for Scientists and Engineers On-Line Course 2
Sine and cosine addition and product formulae
2 2sin cos 1 (12) sin sin cos cos sin (13) sin 2sin cos (14) cos cos cos sin sin (15) 2 2 2 2cos 2 cos sin 2cos 1 1 2sin (16) 2 1cos 1 cos 2
2 (17)
2 1sin 1 cos 22
(18)
1cos cos cos cos2
(19)
1sin sin cos cos2
(20)
1sin cos sin sin2
(21)
cos cos 2cos cos2 2
(22)
sin sin 2sin cos2 2
(23)
cos cos 2sin sin2 2
(24)
sin sin 2cos sin2 2
(25)
Mathematics reference David Miller
Quantum Mechanics for Scientists and Engineers On-Line Course 3
Differential calculus Product rule
d dv duuv u vdx dx dx
(26) Quotient rule
2
du dvv ud u dx dxdx v v
(27)
Chain rule
d df dgf g xdx dg fx
(28)
Derivatives of elementary functions
1n nd x nxdx
(29)
exp expd ax a axdx
(30)
1lnd xdx x
(31)
sin cosd x xdx
(32)
cos sind x xdx
(33)
1
2
sin 11
d xdx x
(34)
1
2
tan 11
d xdx x
(35)
Mathematics reference David Miller
Quantum Mechanics for Scientists and Engineers On-Line Course 4
Integral calculus Integration by parts
( )b bba
a a
dg x df xf x dx f x g x g x dx
dx dx (36)
where we use the common notation
ba
h x h b h a (37) and, specifically, here
ba
f x g x f b g b f a g a (38) Some definite integrals
20
sin2
nx dx (39)
2 20
4/ 2 sin sin , for odd
0 , for even
nmx nx mx dx n mn m n m
n m
(40)
0
sin cos 2 2 / 3d
(41)
0
sin 2 cos 4 / 3d
(42) 3
0
4sin3
d (43)
1/20
exp2
t t dt
(44) sin x dx
x
(45)
2sin x dx
x
(46) 2exp x dx
(47)
21
1dx
x
(48)