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Position of maximum sag, unequal supports
Short answer
The lowest point is at x1 = L/2 - (Th)/(wL) from the lower support and x2 = L/2 + (Th)/(wL) from the higher. If h > wL^2/(2T), x1 becomes negative, the parabola's minimum lies outside the span, and the sag to that imaginary point is virtual sag; the conductor then exerts uplift on the lower tower.
Determine the position of maximum sag from either supporting towers of equal height at a different elevation from a common reference. Also, explain the condition of virtual sag.
When the two supports are at different heights, the lowest point of the conductor is not at mid-span. It shifts towards the lower support. Its position is found from the parabolic approximation.
Derivation
Let:
- = span (horizontal distance between supports A and B)
- = difference in level between the supports (B higher than A)
- = weight of conductor per unit length, and = horizontal tension
- , = horizontal distances of the lowest point O from A (lower) and B (higher), so
B
/|
S2 / |
A / | h
|\ / |
S1 | \_____ O _____/ .......|
|<- x1 ->|<----- x2 ---->|
Taking O as the origin, the conductor is the parabola . So:
Solving with :
The lowest point (point of maximum sag) is at from the lower tower and from the higher tower. The sags are below A and below B. Under wind and ice, is replaced by the resultant loading .
If the supports are at equal height (), and .
Virtual sag
- If , then becomes negative. The lowest point O of the parabola then lies outside the span, beyond the lower support.
- The conductor rises all the way from A to B and has no real lowest point inside the span. The sag measured to the imaginary point O is called the virtual sag.
- This happens on steep hill slopes, which are common in Nepal. The conductor pulls upward on the lower tower (uplift). That tower must be designed as a tension tower, or guyed, and the string must be a tension string, because a suspension string would be pulled up.
✓ Answer checked by Claude Opus 5.5 (high effort)
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