Cable Sag Calculator Back
Structural Analysis Tool

Cable Sag Calculator

Enter span, unit weight, and sag to visualize the exact catenary curve alongside the parabolic approximation. Instantly compute horizontal tension H, maximum tension T_max, and cable length S.

Input Parameters
Span L
m
Sag d
m
Unit weight w
N/m
⚠️ Sag ratio d/L > 1/8 — parabolic approximation accuracy degrades. Use catenary values.
Results
Results
Horiz. tension H (N)
Max tension T_max (N)
Cable length S (m)
Sag ratio d/L

Blue: catenary (exact) / Orange dashed: parabolic approximation

Sag d vs span L for constant horizontal tension H (w = current value)

Theory & Key Formulas

Horizontal tension (parabolic):

$$H = \frac{wL^2}{8d}$$

Maximum tension at supports:

$$T_{max}= \sqrt{H^2 + \left(\frac{wS}{2}\right)^2}$$

Exact catenary shape:

$$y = \frac{H}{w}\left(\cosh\frac{wx}{H}-1\right)$$

Cable length (catenary):

$$S = \frac{2H}{w}\sinh\frac{wL}{2H}$$

What is Cable Sag?

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What exactly is "sag" in a cable, and why do engineers need to calculate it?
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Basically, sag is the vertical distance the cable dips down from a straight line between its two supports. It's not a flaw—it's essential! Without sag, the tension in the cable would be astronomically high. In practice, engineers calculate it to design safe and efficient structures like power lines and suspension bridges. Try moving the "Sag (d)" slider in the simulator above. You'll see how a tiny change dramatically alters the cable's curve and the forces involved.
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Wait, really? So more sag is better because it lowers tension? But then, why not just have a ton of sag?
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Good question! It's a trade-off. A common case is a power line over a road. Yes, more sag (a larger `d`) lowers the horizontal tension `H`, which is good for the towers. But too much sag means the cable hangs too low and could be a safety hazard or not meet clearance regulations. That's why this simulator has three key parameters: Span `L`, Sag `d`, and unit weight `w`. You have to balance them all.
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I see the simulator shows a "catenary" and a "parabolic approximation". What's the difference, and which one should I trust?
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The exact shape a hanging cable forms is called a catenary. For shallow sags (when `d/L` is small, say less than 1/8), a parabola is a very close and much simpler approximation that engineers use daily. For instance, in most power line design, the parabolic formula works fine. But if you increase the sag-to-span ratio in the simulator, you'll see the two curves start to diverge. For deep sags, like in some decorative cables, you must use the exact catenary math to avoid significant error.

Physical Model & Key Equations

The primary equation used for design is the parabolic approximation for horizontal tension. It comes from balancing moments and is remarkably accurate for small sags.

$$H = \frac{w L^2}{8d}$$

Where:
H = Horizontal tension in the cable (N)
w = Unit weight of the cable (N/m)
L d = Sag at the midpoint (m)

The maximum tension doesn't occur at the lowest point, but at the supports where the cable is steepest. This tension is found by combining the horizontal pull with the vertical component from half the cable's weight.

$$T_{max}= \sqrt{H^2 + \left(\frac{w S}{2}\right)^2}$$

Where:
T_max = Maximum tension at the supports (N)
S = Total cable length (m)
The term $(wS/2)$ is the vertical reaction at each support. This is the tension that the support towers and cable anchors must withstand.

Frequently Asked Questions

If the sag d is approximately d/L ≤ 1/8 relative to the span L, parabolic approximation provides sufficient accuracy and is easier to calculate. For larger sags or when more precise shape and tension are required, use the catenary curve. This tool displays both overlapped, allowing you to visually confirm the differences.
The unit weight w is the cable's self-weight per meter. Multiply the linear density (kg/m) from the cable manufacturer's specification by the gravitational acceleration of 9.8 m/s² to convert to N/m. For example, if the linear density is 1.0 kg/m, then w = 9.8 N/m. If including the weight of accessories or ice/snow, add that weight accordingly.
Horizontal tension H indicates the horizontal force acting on supports and is used in the strength design of towers or bridge piers. Maximum tension is the maximum tensile force on the cable itself and must be confirmed to be below the cable's allowable tensile strength. Especially with the catenary curve, tension is highest at the ends, so determine the design value considering a safety factor.
The longer the span and the smaller the sag, the more sharply the horizontal tension H increases (H ∝ L²/d). As a result, excessive tension is applied to the cable and supports, posing risks of breakage or structural deformation. During design, always verify that the calculated tension does not exceed the allowable values of the cable and the strength of the supports.

Real-World Applications

Overhead Power Lines: This is the most common use. Engineers use these exact calculations to ensure cables have enough tension to avoid excessive sway in the wind, but enough sag to keep tension forces on the utility poles within safe limits. The unit weight `w` includes the cable plus any ice loading.

Suspension Bridge Cables: The main cables of bridges like the Golden Gate are giant catenaries. The sag calculation is critical for determining the required cable strength and the height of the supporting towers. The dead load of the bridge deck is the primary "unit weight" `w`.

Telecommunication & Cable Car Lines: Fiber optic or coaxial cables strung between poles, and the cables for ski lifts or gondolas, all rely on sag-tension analysis. For cable cars, the sag must be minimized for passenger comfort and safety, leading to very high tensions.

Architectural & Stage Design: Decorative cable nets for facades, or cables suspending lights and sound equipment in theaters, use these principles. Here, the desired aesthetic shape (a specific catenary curve) often drives the calculation to find the required tension and anchor points.

Common Misconceptions and Points to Note

First, understand that "sag is not just about appearance." For example, reducing the sag from 1m to 0.5m on a 100m span causes the tension to jump to approximately four times the original value (from the parabolic approximation formula $H = w L^2 / (8d)$). What might seem like "just a little tightening up" can easily exceed the allowable stress of the cable or supports, making it a dangerous operation. Next, pay close attention to the units of your input parameters. The "unit weight w" is particularly easy to get wrong. Cable catalogs often list "linear density [kg/m]". When calculating, remember to convert it to [N/m] using $w = mass \times gravitational acceleration$ (e.g., 1.5 kg/m → approx. 14.7 N/m). Finally, beware of confusing the "initial state" with the "loaded state". This tool calculates the basic state with only the cable's self-weight acting on it—a "no wind, no ice/snow" condition. In practice, you must separately verify the sag and tension for the "loaded state" when wind pressure or snow/ice loads are applied. If there's no margin in the initial state's tension, the loaded state could become dangerous. Always be conscious of "which condition you are assuming" in your calculations.