Answers for Tutorial 2
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Answers for Tutorial 2
[M283 - Field theory and PDEs]
Thursday 18th October
1. The gradients of the following functions:
(a) T (x, y, z) = x2 + xy + 3z 3
(b) T (x, y, z) = x2 y 3 + z 4
(c) T (x, y, z) = ez sin x + ln(y)
are respectively
(a) ∇T = (2x + y, x, 9z 2 )
(b) ∇T = (2xy 3 , 3x2 y 2 , 4z 3 )
(c) ∇T = (ez cos x, 1/y, ez sin x).
2. The unit inward pointing normal to the sphere defined by the equation T (x, y, z) =
x2 + y 2 + z 2 = 1 at a general point (x, y, z) is (note the minus sign)
∇T (2x, 2y, 2z) (x, y, z)
ˆ
n=− = −√ 2 2 + 4z 2
= −√ 2 .
| ∇T | 4x + 4y x + y2 + z2
At point a = (1, 0, 0) it can be recast as:
ˆ
n = −(1, 0, 0) .
Hence, the cartesian equation for the tangent plane which touches the sphere at that
point is given by
ˆ
(r − a) · n = 0
(r − (1, 0, 0)) · (1, 0, 0) = 0
(x − 1, y, z) · (1, 0, 0) = 0 .
Or
x=1.
3. The unit outward pointing normal to the ellipsoid T (x, y, z) = x2 + 2y 2 + 3z 2 = 6 at a
general point (x, y, z) is (note that the sign is now positive)
∇T (2x, 4y, 6z) (x, 2y, 3z)
ˆ
n= =√ 2 2 + 36z 2
=√ 2 .
| ∇T | 4x + 16y x + 4y 2 + 9z 2
At point a = (1, 1, 1) it can be recast as:
(1, 2, 3)
ˆ
n= √ .
14
1
Hence, the cartesian equation for the tangent plane which touches the ellipsoid at that
point is given by
ˆ
(r − a) · n = 0
(1, 2, 3)
(r − (1, 1, 1)) · √ =0
14
(x − 1) + 2(y − 1) + 3(z − 1) = 0
Or
x + 2y + 3z = 6 .
4. The directional derivative of the function
1
φ(x, y, z) = x2 + y 2 +
z
at a general point (x, y, z) in the direction given by the vector b = (−1, −1, 1) writes
as
b (−1, −1, 1)
Db Φ = ∇Φ · = (2x, 2y, −1/z 2 ) · √ .
|b| 3
At the point a = (1, 0, 1), it reduces to
b (−1, −1, 1) −2 − 1 √
Db Φ(a) = ∇Φ(a) · = (2, 0, −1) · √ = √ =− 3.
|b| 3 3
5. Given that r = (x, y, z), r = |r|, and that r = r/|r|, we see that
(a) ∇(r 2 ) = (∂/∂x, ∂/∂y, ∂/∂z)(x2 + y 2 + z 2 ) = (2x, 2y, 2z).
This can be further simplified as
(x, y, z) r
∇(r 2 ) = 2 x2 + y 2 + z 2 √ = 2| r | = 2r r
x2 + y 2 + z 2 |r|
(b) ∇ r12 = (∂/∂x, ∂/∂y, ∂/∂z)(x2 + y 2 + z 2 )−1 = − (x(2x,2y,2z))2 .
2 +y 2 +z 2
This can be further simplified as
√ 2
1 x + y2 + z2 (x, y, z) r 2
∇ 2 = −2 √ 2 2 + z2 √ 2
= −2| r | 5 = − 3r
r x +y x +y 2 + z24 |r| r
6. The divergence and curl of the function
v = (2xy, −yz, 3zx) .
are respectively
∇ · v = (∂/∂x, ∂/∂y, ∂/∂z) · (2xy, −yz, 3zx) = 2y − z − 3x ,
2
(which is a scalar field) and
∇ × v = (∂/∂x, ∂/∂y, ∂/∂z) × (2xy, −yz, 3zx)
∂ ∂ ∂ ∂
= ˆ
i (3zx) − (−yz) − ˆ j (3zx) − (2xy)
∂y ∂z ∂x ∂z
ˆ ∂ (−yz) − ∂ (2xy)
+ k
∂x ∂y
= yˆ − 3zˆ − 2xk
i j ˆ (1)
which is a vector field.
7. The vector field
j ˆ
F1 = (14x + 3y)ˆ + 3xˆ + k ,
i
has a curl given by
∇ × F1 = (∂/∂x, ∂/∂y, ∂/∂z) × (14x + 3y, 3x, 1)
∂ ∂ ∂ ∂
= ˆ
i (1) − (3x) − ˆ j (1) − (14x + 3y)
∂y ∂z ∂x ∂z
ˆ ∂ (3x) − ∂ (14x + 3y)
+ k
∂x ∂y
ˆ
= 0ˆ − 0ˆ − (3 − 3)k = 0 .
i j (2)
It can thus be expressed as the gradient of a scalar field since for any scalar field f
∇ × ∇f = 0 This scalar field is f (x, y, z) = 7x2 + 3yx + z. Indeed, we check that
∇f = (∂/∂x, ∂/∂y, ∂/∂z)(7x2 + 3xy + z) = (14x + 3y, 3x, 1) = F1 .
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