= x+3 ∑∞0 (2n+m) / m+1
= 2n / m+1 einx e -y ex+3∑xt3/m+1
e x+3 ∑∞0 y m / ym+1
= e -ln(1-ex)
e x+3 (-ln(1-y))
Serie di Fourier
f(x) = x3
z0 = 1/π π∫ x3 dx - 1/π ∫π/-π [ x+4 / π ]π-π = 0
cn = ∫-ππ x3 cos (nx) dx = ∫ x3 sin (nx) / n - ∫ 3x x cos (nx) / n dx + 1/π =
-1/π [ x3 sin (nx) / n - 3x2 sin (nx) / n2 - ∫ -ππ 6x sin (nx) / n2 dx ] =
= -1/π [ x3 sin (nx) / n - 3x2 sin (nx) / n2 + ∫-ππ 6x sin (nx) / n2 dx ] =
= -1/π [ x3 sin (nx) / n - 3x2 sin (nx) / n2 + (6x sin (nx) / n3) - ∫-ππ 6 cos (nx) / n3 dx ] =
= -1/π [ x3 sin (nx) / n - 3x2 sin (nx) / n2 - 6x cos (nx) / n3 + ∫-ππ 6 cos (nx) / n3 dx ]
Serie di Fourier
f(x) = x3
z0 = 1/π ∫-ππ x3 dx = [π/π(x4/4)]-ππ = [π4/4 - π4/4] = 0
cn = 1/π ∫-ππ x3 cos(nx) dx = [x3 sin(nx)/n]-ππ - 3x2 ∫-ππ cos(nx)/n dx
= [-1/π { [x3 sin(nx)/n - 3x2 sin(nx)/n2}- ∫-ππ 6x sin(nx)/n2 dx]]
= [-1/π { [x3 sin(nx)/n - 3x2 sin(nx)/n2}-∫-ππ 6x sin(nx)/n2 dx]
= [-1/π [x3 sin(nx)/n - 3x2 sin(nx)/n2 + (6x cos(nx)/n3]-ππ + ∫-ππ 6 cos(nx)/n3 dx]
= [-1/π [x3 sin(nx)/n - 3x2 sin(nx)/n2 - 6x cos(nx)/n3 +∫-ππ 6 cos(nx)/n3 dx]
= 0
ϕ(t) = (t, cos(t), cos2(t))
Dϕ(t) = (1, -sin(t), -2 sin(t) )
∫02π ||Dϕ(t)|| dϕ = ∫02π √1+(-sin(t))2 + (-2 sin(t) )2 =
= ∫02π √1+ sin2(t) + 4 sin2(t) = ∫02π√1+1-cos2(t)+4-4cos2(t)
Curva
γ(t) = (5cos(t), 5sin(t), -sin(5t)) con 0 < t < 2π
Dγ(t) = (-5sin(t), 5cos(t), -5cos(5t))
|Dγ(t)| = ∫02π √25sin2(t) + 25cos2(t) + 25cos2(5t) dt =
= ∫02π √25 - 25cos2(t) + 25cos2(t) + 25cos2(5t) = ∫02π √25 + 25cos2(5t) ≈ 38,2
t x y z 0 5 0 0 π/6 4,33 2,5 0,5 π/3 2,5 4,33 0,86 π -5 0 0 2/3 π -2,5 4,33 0,86 5/6 π -4,33 2,5 0,5 4/3 π -2,5 -4,33 -0,86 5/3 π 2,5 -4,33 -0,86 11/6 π 4,33 -2,5 -0,5 2π 5 0 0∫τ ln (3x + y) dx dy
OA: y - 2 = x - 1 -> y = 2/3x - 2x = 0
2x - y = 0
OB: y - 1 = x - 2 -> -2y + 2x - x = 0
x - 2y = 0
∆ x = 4 - 1 = 3
1 - 4 = -3 -> -x + 2y -> 2x + 3y = 3
{u = 2x - y
v = -x + 2y
2x = u + y
y = (u + 2v)
-v + 2y = u + y
y = (u + 2v)/3
J = |1 2/3|
|2/3 1/3|
= 1/3
∫32 ∫3-v0 ln ((6u + 3v + u + 2v)/3) du dv -
∫30 ∫ln (7u + 5v) dx - ln (3) du dv
l'(x) = ln (7u + 5v)
g'(x) = 7
g(x) = 7u + 5v
∫(7u + 5v) ln (7u + 5v) - ∫(7u + 5v)/(7u + 5v) -
[∫(7u + 5v) ln (7u + 5v)]30 - 1
[ (7u + 5v) ln(7u + 5v) ]7-v - [U]7-v
[ (7u + 5v) ln(7u + 5v) - 5v ln(5v) ]3
[ (7 - 7v + 5v) ln(7 - 7v + 5v) ] - 5v ln(5v) ] - 3 + v
[ (7 - 2v) ln(7 - 2v) - 5v ln(5v) ] - 3 + v - 3 ln(3) + v ln(3)
g(x) ln(7 - 2v) g'(x) = x - 2 - 2v
f(x) ln(x) x-1 - 2x f(x) = ln(x) g'(x) = x
f'(x) = 1⁄x g8(x) = x⁄2
1⁄14 ∫127 x ln(x)
[ x ln(x) ]175 x dx
1/14 [ x ln(x) ]2127 x dx
[ x ln(x) ]2721 x dx
[ 27 ln(27) - 15 ln 75 ] - 27 x 75
1⁄14 ln(27) - 15 ln(75) - 27 + 5 = 1⁄24
1⁄28 [ x2 ln(x) ]122 x dx
1/28 [ 441 ln(27) - 725 ln(75) ] - 7471⁄2 2855⁄2 x 2 x 2
3/6 5v ln(5v) 5v = x
f(y) = ln(x) g'(x) = x
f'(x) = 1⁄x g'(x) = x⁄2
∫075 x2 ln(x) ∫075 x dx
-1/70 [225 ln (15)] - [x/2] 150 = -1/70[225 ln (15)] - [225 5/2]) = -7,09
-∫30 3 = - 3 []30 = -3 . 3 = -9
∫vdv = ∫30 v2/2 dv = [v2/2] 30 = 9/2
∫03 3 ln (3) dv = 3 ln (3) ∫03 v dv = 1/3[2 ln (3)
∫03 vln (3) = 9/2 ln (3)
92 - 7,09 - 9 + 9/2 - 9 ln (3) + 9/2 ln (3) = -546/3, 182
∫ ln (3x+4y) dx
T = {0, A(4, -1), B (3, 2)}
OA: y + 1 = x/4
→ 4y = x - 4
→ x + 4y = 0
OB: y - 2 = x - 3/3
→ 3y - 6 = 2x - 6
→ 2x - 3y = 0
x + 4y = 3 + 8 = 11 √
2x - 3y = 8 + 3 = 11 √
u = x + 4y → {x = u - 4y}
v = 2x - 3y → {x = v + 3y/2}
v + 3y = 2u - 8y
4y = 20 - v
{y = 2u - v}
{y = 2u - v/11}
(y = 2u - v/11 3 →) {x = u + 3v/2}
y = 2u - v/11
x = 4v + 3u/11
J = |2/11 - 1/11| |8/11 + 3/11 - 1/11|
|3/11 4 |
|11 |
∫ 011-v ∫ 011-u ln (3u + 12 v + 2u - v/11) dudv = 1/11 ∫ 011-u ln (14u + 11v) - ln (11) dudv
∫ 011-u ln (14u + 11v) dv
f(x) = ln(x)
g'(x) = 14
f'(x) = 1/14u + 11v
g*(x) = 14u + 11v
∫011-u [(11v + 11u)(ln (14u + 11v))]
∫011-u(14u + 11v)(ln (14u + 11v)) dv - ∫0∫v dv
- {|(121 - 33u + 33u)(ln(321 - 33u + 11v))|}
= {*|∫011 ∫0 2u ln (121) - 11 + v dv|}
∫ ln(t+1) du = -ln(t+1)∣011-v u du = -ln(t+1)(11-v) = -11ln(t+1) + vln(t+1)
∫011 11 ln(t+1) - 11 + v + 11 ln(t+1) + v ln(t+1) du
∫011 v du - ∫011 v2/2 = ∫011 v2/2 - ∫011 112/2
g'(x) = v
g(x) = v2/2
∫ 11 ln(t+1) dv v ln(t+1) dv
f(x) = ln(t+1)
f'(x) = 1/t+1
∫a11 [v2/2 ln(t+1)] - ∫011 -v2/2 dv = [112/2 ln(t+1)] - [-11/6 v2/2]110 =
-11/6 + 112/2 ln(t+1) - 11/2
∫ ln(3x+y) dx dy
OA:
OB:
x + 4y
3x + y = 0
2x - 3y = 0
- u = x + 4y
- u = 2x - 3y
J = 2/11 4/11
V + 3y = 2U - 8y
1/11 ∫ 111 ln(8u + 12v + 2u - v)/11
g'(x) = 1
l'(x) = 1/u + v
g(x) = u + v
[-x + v]
∫ 11[(0) - 17] ln(vt)]
- 12 ln(tt)
- = t 21 ln(x)
- - 17
t - 11
∫0v ln (v)
f'(x) = ln (v)
g'(x) = v
f(x) = 1/v
g(x) = v/2
[v2/2 ln(v)]v0 - ∫0v v/2 = v2/2 ln (v) - v2/2
1/10 [12 ln (v) - 12/2 ln (v) + 11/2 11 + 11/2 ] = 11 ln (v) - 11 ln (v+1)
= 11/2 ln (v-1) + 11/4 + 11/2 - v
∫14 ln(2x+3y)
T = { 0,A (1,3),B (2,2) }
OA y/3=x-1/x -y+3= -3x+3=3x-y=0 4√
OB y/2=x-2/2 -2y+x=2x+x=2x-4y=0 -2x+2y=0
4√
- U=-3x-y
- V=-2x+2y
- x=u+y/3
- x=u+y/3
x=-u+4y
2u+4y = 3v+6y
4y=3v-2u
y=-3v-2u/4
x=4u-3v-2u/12
2u-3v/12
- U=3x-y
- V=-2x+2y
- y=3x-u
- y=v+2x/2
x=v+2u
y=3v+2u/4
J =
| -2 4 | 1/4
| 3 4 | 6/16 = 4/16 = 1/4
∫10 ln(4u+2v+2u+3v/4)
= (1/6)∫04 6ln(6u+5v)-ln(x)
[ (6u+5v) ln(6u+5v) ]4-v-v - [
(24-6v+5v) ln(24-v) - ( 5v) ln(5v) -4+v]
(1/24)∫04 (2x-v) ln(2x-v) dv = ∫2024 f(x) ln(x) dx = -∫2420 (x) ln(x) dv
l(x)=ln (x)
l'(x) = 1/x
g⁻¹(x) = x
g⁻¹(x) = x²/2
[3/2 ln(x)]2024 - ∫2024 x/2 dx
576/2 ln(24) - 280 ln(20) - [x2/4]2024
576/2 ln(24) - 200 ln(20) - 576/4 + 200
228 ln(24) - 200 ln(20) - 200 + 100
∫05v ln(5v)
f(u) = ln(5v)
g"(u) = 5
g(x) = 5v2/2
∫05v/2 5u/2
(∫05v ln(5v))
∫04[40 ln(20) - 5/ln(v2/2)]4
-40 ln(20) - - 20
1/24 [228 ln(24) - 200 ln(20) - 4x - 40 ln(20) + 20 - 16 + 8 - 16 ln(x) + 8 ln(x)]
19/2 ln(x) - 85/3 ln(20) - 4/3 - 5/3 ln(20) - 7/3 ln(1) + 1/3 ln(2)
-1,56
ϕ(t) = (t cos(t), t sin(t))
t ∈ [0, 10π]
txy000π/60.50.26π/40.550.55π/30.520.9π/201.62/3 π-11.83π/4-1.61.65/6 π-2.31.3π-3.703/2 π0-4.7Dϕ(t) = (-tsin(t)+cos(t), tcos(t)+sin(t))
∫ ||Dϕ(t)|| = 010π ∫ √ ...
∫0∞ t2 + 1 dt ≈ 495
γ(t) = (t2cos(t), t2sin(t))
t ∈ ]0, 2π]
Dγ(t) = (2t cos(t) - t2sin(t) , 2t sin(t) + t2cos(t))
||Dγ(t)|| = ∫02π √ 4t2 cos2(t) + t4 sin2(t) * 2t3 sin(t) + 4t2 sin2(t) + t4 cos2(t) + t4= ∫02π √ 4t2 cos2(t) + t4 sin2(t) + 4t2 sin2(t) + t4 cos2(t)= ∫02π √ 4t2 + t4txy000π/60.240.14π/40.440.44π/30.550.95π/202.52π/3-2.23.83π/4-3.33.35π/6-5.33.43π-9.807π/6-11.6-6.75π/4-10.9-10.84π/3-8.7-15.23π/20-22.25π/313.7-23.77π/421.4-21.411π/628.7-16.62π19.701 ∫ ln (x - y) dx dy
OA: y = -1/2 x + 4: x = -6/6 → -6y + 8 = -x + 8 → x - 6y = 0 → x + 6y = 8
OB: y = − x/2 + 4 → -4y + 8 = -2x + 8 → 2x - 4y = 0 = 8
{u = -x + 6y {x = -u + 6y {x = -u + 6y
{v = 2x - 4y {x = v + 4y/2 {-2u + 12y = v + 4y
x = 40 + 6v/8
y = v + 20/8
J = | 4/8 6/8 |
| 2/8 1 |
= 4/64 + 12/64 - 8/64 = 1/8
1/8 ∫08-v ∫0 ln (4v + 6v - v + 2v/8) du dv - 1/8 ∫08-v ln (2u + 5v) -ln (8) du dv
1/2∫08-v z ln (2u + 5v) du
f (x) = ln (2u + 5v) f' (x) = 2/2u + 5v
g' (x) = 2
g (x) = 8u + 5v
{[(2u + 5v) ln (2u + 5v)]08-v -∫08-v v u du
{ [ (8 - 2u + 5v) ln (16 + 3v) ] 0 -∫08-v (5v) ln (5v)] - 8 + v-8 ln (8) + v ln (8)
{ (16 + 3v) ln (16 + 3v) dv = 1/36∫016 (x) ln (x) dx f (x) = ln (x) f ' (x) = 1/x
{ - ∫1640 ln (x)
{ 1/6 [1600 ln (40)-256 ln (16)] - 1/6 [x2/2]4016x2
[1600 ln (40) - 256 ln (8)] - 1600/12 + 256/12
∫08 5v ln (5v) dv = F(x) = ln (5v) F'(x) = 1/5v g'(x) = 5v g(x) = v2/2
5/2 [∫0v2/2 (ln (5v)v)8 dv = 160 ln (40) - 5/2 [∫0v2/2]8
160 ln (40) - 80
[1600/6 ln (40) - 256/6 ln (16) - 1600/12 + 256/12 = 260 ln (40) + 80 - 64 + 32 ln (8)]
+ 32 ln (8) ] 7/16 = 9,04
φ(t) = (5 cos(t), sin(3t), 5 sin(t) + cos(3t))
t ∈ [0, 2π]
DY(t) = (-5 sin(t), 3 cos(3t), 5 cos(t) - 3 sin(3t))
|DY(t)| = ∫02π √(25 sin²(t) + 9 cos²(3t) + 30 sin(t) cos(3t) + 25 cos²(t) + 9 - 36 cos(t) sin(3t)) dt
= ∫02π √(25 - 25 cos2(t) + 15 sin²(t) + 45 sin²(2t) - 9 - 9 - 25 cos²(t) - 15 sin²(4t)) dt
= ∫02π √(25 + 15 sin²(t) + 3 sin²(3t) - 9 - 15 sin²(t)) dt
= ∫02π √(34 - 30 sin²(t)) - √(36 = ∫02π √(1 - 30 sin²(t)) dt
= 34,31
t x y 0 5 ∞ ~ 1 π/3 3 5√3 π/4 2.8 2.8 π/2 2.5 3.3 π 1 5 2π/3 -2.5 5.33 3/4π 4.24 4.2 5/6π 5.3 2.5 π -5 -1 7/6π -3.33 -2.5-
Analisi matematica 3 - Esercizi
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Analisi matematica 3 - Esercizi
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Analisi Matematica 3 - Esercizi
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Formulario Analisi Matematica 3