Problem Statement
A structural steel cable follows path x = 2 + t , y = β 1 + 2 t , z = 3 β 2 t x = 2 + t, y = -1 + 2t, z = 3 - 2t x = 2 + t , y = β 1 + 2 t , z = 3 β 2 t (meters). An electrical line passes near point M ( 5 , 5 , 2 ) M(5, 5, 2) M ( 5 , 5 , 2 ) .
Step-by-Step Mathematical Solution
1. Extract Cable Line Data
Reference point on cable (at t = 0 t=0 t = 0 ): P = ( 2 , β 1 , 3 ) P = (2, -1, 3) P = ( 2 , β 1 , 3 )
Direction vector of cable: v β = β¨ 1 , 2 , β 2 β© \vec{v} = \langle 1, 2, -2 \rangle v = β¨ 1 , 2 , β 2 β©
2. Construct Displacement Vector P M β \vec{PM} P M
P M β = β¨ 5 β 2 , 5 β ( β 1 ) , 2 β 3 β© = β¨ 3 , 6 , β 1 β© Β m \vec{PM} = \langle 5 - 2, 5 - (-1), 2 - 3 \rangle = \langle 3, 6, -1 \rangle\text{ m} P M = β¨ 5 β 2 , 5 β ( β 1 ) , 2 β 3 β© = β¨ 3 , 6 , β 1 β© Β m
3. Compute Cross Product P M β Γ v β \vec{PM} \times \vec{v} P M Γ v
P M β Γ v β = β£ i ^ j ^ k ^ 3 6 β 1 1 2 β 2 β£ \vec{PM} \times \vec{v} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 3 & 6 & -1 \\ 1 & 2 & -2 \end{vmatrix} P M Γ v = β i ^ 3 1 β j ^ β 6 2 β k ^ β 1 β 2 β β
P M β Γ v β = i ^ ( 6 ( β 2 ) β ( β 1 ) ( 2 ) ) β j ^ ( 3 ( β 2 ) β ( β 1 ) ( 1 ) ) + k ^ ( 3 ( 2 ) β 6 ( 1 ) ) \vec{PM} \times \vec{v} = \hat{i}(6(-2) - (-1)(2)) - \hat{j}(3(-2) - (-1)(1)) + \hat{k}(3(2) - 6(1)) P M Γ v = i ^ ( 6 ( β 2 ) β ( β 1 ) ( 2 )) β j ^ β ( 3 ( β 2 ) β ( β 1 ) ( 1 )) + k ^ ( 3 ( 2 ) β 6 ( 1 ))
P M β Γ v β = i ^ ( β 12 + 2 ) β j ^ ( β 6 + 1 ) + k ^ ( 6 β 6 ) = β 10 i ^ + 5 j ^ + 0 k ^ = β¨ β 10 , 5 , 0 β© \vec{PM} \times \vec{v} = \hat{i}(-12 + 2) - \hat{j}(-6 + 1) + \hat{k}(6 - 6) = -10\hat{i} + 5\hat{j} + 0\hat{k} = \langle -10, 5, 0 \rangle P M Γ v = i ^ ( β 12 + 2 ) β j ^ β ( β 6 + 1 ) + k ^ ( 6 β 6 ) = β 10 i ^ + 5 j ^ β + 0 k ^ = β¨ β 10 , 5 , 0 β©
4. Calculate Vector Magnitudes
Magnitude of cross product:
β₯ P M β Γ v β β₯ = ( β 10 ) 2 + 5 2 + 0 2 = 100 + 25 = 125 = 5 5 Β m 2 \|\vec{PM} \times \vec{v}\| = \sqrt{(-10)^2 + 5^2 + 0^2} = \sqrt{100 + 25} = \sqrt{125} = 5\sqrt{5}\text{ m}^2 β₯ P M Γ v β₯ = ( β 10 ) 2 + 5 2 + 0 2 β = 100 + 25 β = 125 β = 5 5 β Β m 2
Magnitude of direction vector v β \vec{v} v :
β₯ v β β₯ = 1 2 + 2 2 + ( β 2 ) 2 = 1 + 4 + 4 = 9 = 3 Β m \|\vec{v}\| = \sqrt{1^2 + 2^2 + (-2)^2} = \sqrt{1 + 4 + 4} = \sqrt{9} = 3\text{ m} β₯ v β₯ = 1 2 + 2 2 + ( β 2 ) 2 β = 1 + 4 + 4 β = 9 β = 3 Β m
5. Calculate Shortest Clearance Distance d d d
d = β₯ P M β Γ v β β₯ β₯ v β β₯ = 5 5 3 β 3.73 Β meters d = \frac{\|\vec{PM} \times \vec{v}\|}{\|\vec{v}\|} = \frac{5\sqrt{5}}{3} \approx 3.73\text{ meters} d = β₯ v β₯ β₯ P M Γ v β₯ β = 3 5 5 β β β 3.73 Β meters
Real-Life Engineering Meaning & Application
Physical Interpretation: The calculated distance of 3.73 Β m 3.73\text{ m} 3.73 Β m is the absolute minimum geometric air gap between the electrical conductor and the grounded steel structural cable.
Engineering Application: National Electrical Safety Code (NESC) and OSHA standards specify minimum flashover clearance distances around high-voltage transmission lines (typically β₯ 3.0 Β m \ge 3.0\text{ m} β₯ 3.0 Β m for medium voltage) to prevent electrical arcing under high humidity or windy cable sway conditions. A verified distance of 3.73 Β m 3.73\text{ m} 3.73 Β m confirms compliance, allowing structural engineers to issue formal building certification.