hms112formulasheets_sem2
TRANSCRIPT
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HMS 112 FORMULA SHEETS 2
(i) the surface has a local maximum at P if
2z
x2< 0
and
2z
x22z
y2(
2z
xy)2 > 0
;
(ii) the surface has a local minimum at P if
2z
x2> 0
and
2z
x22z
y2(
2z
xy)2 > 0
;
(iii) the surface has a saddle point at P if
2z
x22z
y2(
2z
xy)2 < 0
CHAIN RULES:
(i) ifz = f(x,y) and x = x(t) and y = y(t) thendz
dt=z
x
dx
dt+z
y
dy
dt
(ii) ifz = f(x,t) and x = x(t) then
dz
dt =
z
x
dx
dt +
z
t
(iii) if z = f(x,y) and y = y(x) then
dz
dx=z
x+z
y
dy
dx
(iv) if z = f(x,y) and x = x(u,v) and y = y(u,v) thenz
u=z
x
x
u+z
y
y
u and
z
v=z
x
x
v+z
y
y
v
COMPLEX IMPEDANCE IN RLC CIRCUITS
= 2f
Z
VI
cisZZ
CLjRZ
tII
tVV
00
0
0
)1
(
)sin(
)sin(
=
=
+=
=
+=
LINEAR HOMOGENEOUS 2ND ORDER DIFFERENTIAL EQUATIONS WITHCONSTANT COEFFICIENTS
i.e.ad2y
dx2+ b
dy
dx+ cy = 0
(1)
IF THE ROOTS OF THECHARACTERISTIC (AUXILIARY)
EQUATION am2 + bm + c = 0 ARE
THEN THE SOLUTIONOF (1) IS
2 real and different roots m1 and m2 y = Aem1x + Be
m2x
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HMS 112 FORMULA SHEETS 3
2 real and equal roots ( i.e. m = m1 = m2 )(also called a double root)
y = em1x A +Bx( )
2 conjugate complex roots m1 and m2 ,
where m1 = + j and m2 = j
(where1=
j )
y = ex
(A cosx + Bsinx)
LINEAR NONHOMOGENEOUS 2ND ORDER DIFFERENTIAL EQUATIONSWITH CONSTANT COEFFICIENTS
i.e.ad2y
dx2+ b
dy
dx+ cy = f(x)
, where f(x) 0 (2)
The solution of (2) is phyyy +=
, where)( ch yy (the COMPLEMENTARY
FUNCTION or C.F.) is the GENERAL SOLUTION (i.e. it contains 2 arbitraryconstants) of the corresponding homogeneous equation, i.e.
ad2y
dx2+ b
dy
dx+ cy = 0
andyp , the PARTICULAR INTEGRAL, can be found by the table below:
IF f(x) HAS A TERM ACONSTANTMULTIPLE OF
AND IF THENy
p IS
epx p N.R.A.E (i.e. p not a
root of auxiliaryequation)
Cepx
p S.R.A.E (i.e. p a singleroot of the auxiliaryequation)
Cxepx
p D.R.A.E (i.e. p adouble root of theauxiliaryequation)
Cx2epx
sinqx orcosqx jq N.R.A.E (where1=j )
Ccosqx + Dsin qx
jq S.R.A.E x(Ccos qx + Dsin qx)
a0 + a1x + .... + anxn 0 N.R.A.E. b0 + b1x + .... + bnx n
0 S.R.A.E. x(b0 + b1x + .... + bnxn)
0 D.R.A.E. x2(b0 + b1x + .... + bnx
n)
Note: the constants inyp can always be found.
Derivatives
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HMS 112 FORMULA SHEETS 4
FUNCTION DERIVATIVE
sin1 x
1
1 x2
cos1 x 21
1
x
tan1 x
1
1+ x2
sinh1x
1
1 + x2
cosh1x
1
x2
1
tanh1x
1
1 x2
Integrals
FUNCTION INTEGRAL1
a2
x2
ca
x+
1sin
1
x2 + a2c
a
x
a+
1tan1
sinh kx cosh kx
k+ c
cosh kx sinhkx
k + csech
2kx tanh kx
k+ c
1
a2
+ x2
sinh1 x
a+ c
orln( x + x2 + a2 )+ c
1
x2
a2
cosh1 x
a+ c
or caxx ++ )ln(22
1
a2 x21
atanh
1 x
a+ c
orc
xa
xa
a+
+ln
2
1
1
x2 a2 cax
a+
1coth
1
orc
ax
ax
a ++
ln2
1
xe x sin xex cos
c
xxe x
+
+
)cossin(22
xe x cos
)sincos(22
xxe x
++
+c
INTEGRATION BY PARTS: u
dv
dx dx = uv vdu
dx dx
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HMS 112 FORMULA SHEETS 5
SUBSTITUTION RULE:f(u)
du
dxdx = f(u) du
orf(x)dx = f(x)
dx
d d
RULES OF BOOLEAN ALGEBRA:
p + p = p (1)pp = p (2)p + 0 = p (3)p +1= 1 (4)p1=p (5)p0 = 0 (6)p +p =1 (7)pp = 0 (8)
p =p (9)p + qr= (p + q)(p + r) (10)p + pr= p (11)