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Linear approximation Differential notation Parametric derivatives Arc length parametric Applications to physics
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3
( )
dy ( 3x^ 5 ) dx
2
2
3
2 2
2
3 x 1
2dx dy 3 x 1
6 x 2 6 x dy
3 x 1
3 x 1 2 2 x 3
3 x 1
2 x dy d
−
− ⇒∴ =
−
−
−
=
multiply itby dx.
oftherightmemberoftheequationand
Note:Inpractice,wesimplygetthederivative
_3
( )
( ) ( )
( )
( )
60
1 less that 27 3 ; therefore 26. 55 3
60
1 which implies that 26. 55 willbe approximately
1
100
45
27
1
1 Hence, dy
Because x isdecreasing from 27 to26.55, then x dx 0.
dx 3 x
1 x dx 3
1 dy
dy f' x dx f x x
x 27. Thedifferentialdy is
value of x that is aperfect cube andisrelatively closeto26.55,namely
Because the function youare applyingisf x x, choose a convenient
3
3 3
3
3
2
3
2
3
2
3
1
3
≈ ≈
= ≈ −
= ⋅ − = ⋅− =− =−
∆ = =−
= =
= → =
=
=
−
3
2
of x dx 0.01 to an originalvalueof x 2.
considering 2.01 as the result of applying an increment
y dy. Note that if we write 2.01 2 0.01,then we are
to find the approximate value,then we shall solve for
The exact value is y y but since we are simply asked
( )
y dy 13 0. 20 13. 20
therefore,the required approximation is
dy 12 8 0. 01 0. 20
and when x 2 and dx 0. 01 , then
when x 2 , then y 8 8 3 13
then dy 3 x 4 x dx
Since y x 2 x 3
2
3 2
= + =
= =
= = + − =
= +
= + −
2
2 3 2
dx
d y
2 3 t
2 t 1
dt
dx
dt
dy
dx
dy + = =
( ) 2 5
2
4 2
2
2
2
2 2
2
9 t
2 t 1
dx
d y
3 t
1
9 t
3 t 2 2 t 1 6 t
dx
d y
dx
dt
3 t
2 t 1
dt
d
dx
d y
− + ∴ =
2
2
dx
d y
= θ θ
θ
θ = 2 tan 2 cos
4 sin
d
dx
d
dy
dx
dy
( )
∴ = θ
= θ• θ
θ
= θ•
θ θ θ
=
3 2
2
2 2
2
2 2
2
2
2
sec dx
d y
sec sec dx
d y
2 cos
1 2 sec dx
d y
dx
d 2 tan d
d
dx
d y