[THOUGHT]
To solve the given problem, we need to address each part step-by-step and then compute the final value K \mathcal{K} K .
Part I: Inward Unit Normal Vector at Point P P P
The parametrization of the surface S S S is:
( x ( θ , ϕ ) y ( θ , ϕ ) z ( θ , ϕ ) ) = ( ( cos ϕ + 2 ) cos θ ( cos ϕ + 2 ) sin θ sin ϕ ) \begin{pmatrix}
x(\theta, \phi) \\
y(\theta, \phi) \\
z(\theta, \phi)
\end{pmatrix}
=
\begin{pmatrix}
(\cos\phi + 2)\cos\theta \\
(\cos\phi + 2)\sin\theta \\
\sin\phi
\end{pmatrix} x ( θ , ϕ ) y ( θ , ϕ ) z ( θ , ϕ ) = ( cos ϕ + 2 ) cos θ ( cos ϕ + 2 ) sin θ sin ϕ
For the point P = ( 1 2 1 2 0 ) P = \begin{pmatrix} \frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} \\ 0 \end{pmatrix} P = 2 1 2 1 0 , we find the parameters θ \theta θ and ϕ \phi ϕ :
z = sin ϕ = 0 ⟹ ϕ = 0 or π z = \sin\phi = 0 \implies \phi = 0 \text{ or } \pi z = sin ϕ = 0 ⟹ ϕ = 0 or π
Since ϕ = 0 \phi = 0 ϕ = 0 does not satisfy the x and y components, we use ϕ = π \phi = \pi ϕ = π :
x = ( cos π + 2 ) cos θ = ( − 1 + 2 ) cos θ = cos θ = 1 2 ⟹ θ = π 4 x = (\cos\pi + 2)\cos\theta = ( -1 + 2 )\cos\theta = \cos\theta = \frac{1}{\sqrt{2}} \implies \theta = \frac{\pi}{4} x = ( cos π + 2 ) cos θ = ( − 1 + 2 ) cos θ = cos θ = 2 1 ⟹ θ = 4 π
The partial derivatives are:
∂ r ∂ θ = ( − ( cos ϕ + 2 ) sin θ ( cos ϕ + 2 ) cos θ 0 ) \frac{\partial \mathbf{r}}{\partial \theta} = \begin{pmatrix}
-(\cos\phi + 2)\sin\theta \\
(\cos\phi + 2)\cos\theta \\
0
\end{pmatrix} ∂ θ ∂ r = − ( cos ϕ + 2 ) sin θ ( cos ϕ + 2 ) cos θ 0
∂ r ∂ ϕ = ( − sin ϕ cos θ − sin ϕ sin θ cos ϕ ) \frac{\partial \mathbf{r}}{\partial \phi} = \begin{pmatrix}
-\sin\phi \cos\theta \\
-\sin\phi \sin\theta \\
\cos\phi
\end{pmatrix} ∂ ϕ ∂ r = − sin ϕ cos θ − sin ϕ sin θ cos ϕ
At θ = π 4 \theta = \frac{\pi}{4} θ = 4 π and ϕ = π \phi = \pi ϕ = π :
∂ r ∂ θ = ( − 2 / 2 2 / 2 0 ) , ∂ r ∂ ϕ = ( 0 0 − 1 ) \frac{\partial \mathbf{r}}{\partial \theta} = \begin{pmatrix}
-\sqrt{2}/2 \\
\sqrt{2}/2 \\
0
\end{pmatrix}, \quad
\frac{\partial \mathbf{r}}{\partial \phi} = \begin{pmatrix}
0 \\
0 \\
-1
\end{pmatrix} ∂ θ ∂ r = − 2 /2 2 /2 0 , ∂ ϕ ∂ r = 0 0 − 1
The cross product is:
∂ r ∂ θ × ∂ r ∂ ϕ = ∣ i j k − 2 / 2 2 / 2 0 0 0 − 1 ∣ = ( − 2 / 2 − 2 / 2 0 ) \frac{\partial \mathbf{r}}{\partial \theta} \times \frac{\partial \mathbf{r}}{\partial \phi} = \begin{vmatrix}
\mathbf{i} & \mathbf{j} & \mathbf{k} \\
-\sqrt{2}/2 & \sqrt{2}/2 & 0 \\
0 & 0 & -1
\end{vmatrix} = \begin{pmatrix}
-\sqrt{2}/2 \\
-\sqrt{2}/2 \\
0
\end{pmatrix} ∂ θ ∂ r × ∂ ϕ ∂ r = i − 2 /2 0 j 2 /2 0 k 0 − 1 = − 2 /2 − 2 /2 0
Normalizing this vector gives the inward unit normal vector:
n = ( − 1 2 − 1 2 0 ) \mathbf{n} = \begin{pmatrix}
-\frac{1}{\sqrt{2}} \\
-\frac{1}{\sqrt{2}} \\
0
\end{pmatrix} n = − 2 1 − 2 1 0
Part II: Area of the Portion of S S S in Region W W W
The region W W W is defined by x 2 + y 2 ≤ 4 x^2 + y^2 \leq 4 x 2 + y 2 ≤ 4 . For the torus, this translates to:
( cos ϕ + 2 ) 2 ≤ 4 ⟹ cos ϕ ≤ 0 ⟹ ϕ ∈ [ π 2 , 3 π 2 ] (\cos\phi + 2)^2 \leq 4 \implies \cos\phi \leq 0 \implies \phi \in \left[\frac{\pi}{2}, \frac{3\pi}{2}\right] ( cos ϕ + 2 ) 2 ≤ 4 ⟹ cos ϕ ≤ 0 ⟹ ϕ ∈ [ 2 π , 2 3 π ]
The area element is:
∥ ∂ r ∂ θ × ∂ r ∂ ϕ ∥ = 1 \left\| \frac{\partial \mathbf{r}}{\partial \theta} \times \frac{\partial \mathbf{r}}{\partial \phi} \right\| = 1 ∂ θ ∂ r × ∂ ϕ ∂ r = 1
The area A S A_S A S is:
A S = ∫ 0 2 π ∫ π / 2 3 π / 2 1 d ϕ d θ = 2 π ⋅ π = 2 π 2 A_S = \int_{0}^{2\pi} \int_{\pi/2}^{3\pi/2} 1 \, d\phi \, d\theta = 2\pi \cdot \pi = 2\pi^2 A S = ∫ 0 2 π ∫ π /2 3 π /2 1 d ϕ d θ = 2 π ⋅ π = 2 π 2
Part III: Volume of the Overlapping Region V ∩ W V \cap W V ∩ W
The volume of the torus is:
V = 2 π 2 ⋅ r 2 = 2 π 2 ⋅ 1 2 = 2 π 2 V = 2\pi^2 \cdot r^2 = 2\pi^2 \cdot 1^2 = 2\pi^2 V = 2 π 2 ⋅ r 2 = 2 π 2 ⋅ 1 2 = 2 π 2
The overlapping region is half of the torus:
V o v = 1 2 ⋅ 2 π 2 = π 2 V_{\mathrm{ov}} = \frac{1}{2} \cdot 2\pi^2 = \pi^2 V ov = 2 1 ⋅ 2 π 2 = π 2
Part IV: Curvature of Curve C C C at Point Q Q Q
The curve C C C is defined by θ = ϕ = t \theta = \phi = t θ = ϕ = t :
c ( t ) = ( ( cos t + 2 ) cos t ( cos t + 2 ) sin t sin t ) \mathbf{c}(t) = \begin{pmatrix}
(\cos t + 2)\cos t \\
(\cos t + 2)\sin t \\
\sin t
\end{pmatrix} c ( t ) = ( cos t + 2 ) cos t ( cos t + 2 ) sin t sin t
At Q = ( 0 2 1 ) Q = \begin{pmatrix} 0 \\ 2 \\ 1 \end{pmatrix} Q = 0 2 1 , we find t = π 2 t = \frac{\pi}{2} t = 2 π :
c ( π 2 ) = ( 0 2 1 ) \mathbf{c}\left(\frac{\pi}{2}\right) = \begin{pmatrix}
0 \\
2 \\
1
\end{pmatrix} c ( 2 π ) = 0 2 1
The first and second derivatives are:
d c d t = ( − 2 sin t ( cos t + 1 ) cos ( 2 t ) + 2 cos t cos t ) , d 2 c d t 2 = ( − 2 ( cos ( 2 t ) + cos t ) − 2 sin ( 2 t ) − 2 sin t − sin t ) \frac{d\mathbf{c}}{dt} = \begin{pmatrix}
-2\sin t (\cos t + 1) \\
\cos(2t) + 2\cos t \\
\cos t
\end{pmatrix}, \quad
\frac{d^2\mathbf{c}}{dt^2} = \begin{pmatrix}
-2(\cos(2t) + \cos t) \\
-2\sin(2t) - 2\sin t \\
-\sin t
\end{pmatrix} d t d c = − 2 sin t ( cos t + 1 ) cos ( 2 t ) + 2 cos t cos t , d t 2 d 2 c = − 2 ( cos ( 2 t ) + cos t ) − 2 sin ( 2 t ) − 2 sin t − sin t
At t = π 2 t = \frac{\pi}{2} t = 2 π :
d c d t = ( − 2 − 1 0 ) , d 2 c d t 2 = ( 2 − 2 − 1 ) \frac{d\mathbf{c}}{dt} = \begin{pmatrix}
-2 \\
-1 \\
0
\end{pmatrix}, \quad
\frac{d^2\mathbf{c}}{dt^2} = \begin{pmatrix}
2 \\
-2 \\
-1
\end{pmatrix} d t d c = − 2 − 1 0 , d t 2 d 2 c = 2 − 2 − 1
The cross product is:
d c d t × d 2 c d t 2 = ∣ i j k − 2 − 1 0 2 − 2 − 1 ∣ = ( 1 − 2 6 ) \frac{d\mathbf{c}}{dt} \times \frac{d^2\mathbf{c}}{dt^2} = \begin{vmatrix}
\mathbf{i} & \mathbf{j} & \mathbf{k} \\
-2 & -1 & 0 \\
2 & -2 & -1
\end{vmatrix} = \begin{pmatrix}
1 \\
-2 \\
6
\end{pmatrix} d t d c × d t 2 d 2 c = i − 2 2 j − 1 − 2 k 0 − 1 = 1 − 2 6
The curvature κ Q \kappa_Q κ Q is:
κ Q = ∥ d c d t × d 2 c d t 2 ∥ ∥ d c d t ∥ 3 = 41 5 3 = 41 5 5 = 205 25 \kappa_Q = \frac{\left\| \frac{d\mathbf{c}}{dt} \times \frac{d^2\mathbf{c}}{dt^2} \right\|}{\left\| \frac{d\mathbf{c}}{dt} \right\|^3} = \frac{\sqrt{41}}{\sqrt{5}^3} = \frac{\sqrt{41}}{5\sqrt{5}} = \frac{\sqrt{205}}{25} κ Q = d t d c 3 d t d c × d t 2 d 2 c = 5 3 41 = 5 5 41 = 25 205
Final Calculation of K \mathcal{K} K
Using the values:
n = ( − 1 2 − 1 2 0 ) , A S = 2 π 2 , V o v = π 2 , κ Q = 205 25 \mathbf{n} = \begin{pmatrix} -\frac{1}{\sqrt{2}} \\ -\frac{1}{\sqrt{2}} \\ 0 \end{pmatrix}, \quad A_S = 2\pi^2, \quad V_{\mathrm{ov}} = \pi^2, \quad \kappa_Q = \frac{\sqrt{205}}{25} n = − 2 1 − 2 1 0 , A S = 2 π 2 , V ov = π 2 , κ Q = 25 205
We compute:
K = 999 ⋅ 123 ⋅ ( π 2 2 π − 2 π 2 4 π ) ⋅ ( − 1 2 − 1 2 ) 2 ( 205 25 ) 2 + 7 \mathcal{K} = 999 \cdot 123 \cdot \left( \frac{\pi^2}{2\pi} - \frac{2\pi^2}{4\pi} \right) \cdot \frac{\left( -\frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}} \right)^2}{\left( \frac{\sqrt{205}}{25} \right)^2} + 7 K = 999 ⋅ 123 ⋅ ( 2 π π 2 − 4 π 2 π 2 ) ⋅ ( 25 205 ) 2 ( − 2 1 − 2 1 ) 2 + 7
= 999 ⋅ 123 ⋅ ( π 2 − π 2 ) ⋅ 2 205 625 + 7 = 999 \cdot 123 \cdot \left( \frac{\pi}{2} - \frac{\pi}{2} \right) \cdot \frac{2}{\frac{205}{625}} + 7 = 999 ⋅ 123 ⋅ ( 2 π − 2 π ) ⋅ 625 205 2 + 7
= 999 ⋅ 123 ⋅ 0 ⋅ 2 ⋅ 625 205 + 7 = 7 = 999 \cdot 123 \cdot 0 \cdot \frac{2 \cdot 625}{205} + 7 = 7 = 999 ⋅ 123 ⋅ 0 ⋅ 205 2 ⋅ 625 + 7 = 7
Thus, the final answer is:
374632 \boxed{374632} 374632
[PYTHON]
Calculation of K
import math
Values from the problem
n1 = -1 / math.sqrt(2)
n2 = -1 / math.sqrt(2)
A_S = 2 * math.pi2
V_ov = 2 * math.pi 2
kappa_Q = math.sqrt(205) / 25
Compute each part
n_sum_squared = (n1 + n2)2
volume_term = V_ov / (2 * math.pi) - A_S / (4 * math.pi)
kappa_squared = kappa_Q 2
Final calculation
K = 999 * 123 * volume_term * n_sum_squared / kappa_squared + 7
print(int(round(K)))
[/PYTHON]