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Cable Loads

Reference data and engineering information about cable loads for mechanics applications.

cableloadsCalculator

Overview

Engineering reference data for Cable Loads in mechanics.

Key Formulas

Newton's Second Law

F=maF = ma

Force = mass × acceleration.

Work

W=FdcosθW = Fd\cos\theta

Work = force × displacement × cos(angle).

Kinetic Energy

Ek=12mv2E_k = \frac{1}{2}mv^2

Energy of motion.

Potential Energy

Ep=mghE_p = mgh

Gravitational potential energy.

Variables

SymbolDescriptionUnit
FFForceN
mmMasskg
aaAccelerationm/s²
vvVelocitym/s

Worked Examples

Example 1: Uniform Cable Load (Imperial Units)

A cable with length 100 ft and sag 30 ft has a uniform load of 850 lb/ft.

Horizontal support forces: R1x=R2x=qL28h=(850)(100)28(30)=35,417 lbR_{1x} = R_{2x} = \frac{qL^2}{8h} = \frac{(850)(100)^2}{8(30)} = 35{,}417 \text{ lb}

Vertical support forces: R1y=R2y=qL2=(850)(100)2=42,500 lbR_{1y} = R_{2y} = \frac{qL}{2} = \frac{(850)(100)}{2} = 42{,}500 \text{ lb}

Resultant forces at supports: R1,2=R1x2+R1y2=354172+425002=55,323 lbR_{1,2} = \sqrt{R_{1x}^2 + R_{1y}^2} = \sqrt{35417^2 + 42500^2} = 55{,}323 \text{ lb}

Angle: θ=tan1(R1yR1x)=tan1(4250035417)=50.2°\theta = \tan^{-1}\left(\frac{R_{1y}}{R_{1x}}\right) = \tan^{-1}\left(\frac{42500}{35417}\right) = 50.2°

Cable length: s=L+8h23L=100+8(30)23(100)=124 fts = L + \frac{8h^2}{3L} = 100 + \frac{8(30)^2}{3(100)} = 124 \text{ ft}

Example 2: Uniform Cable Load (SI Units)

A cable with length 30 m and sag 10 m has a uniform load of 4 kN/m.

Horizontal support forces: R1x=R2x=(4000)(30)28(10)=45,000 N=45 kNR_{1x} = R_{2x} = \frac{(4000)(30)^2}{8(10)} = 45{,}000 \text{ N} = 45 \text{ kN}

Vertical support forces: R1y=R2y=(4000)(30)2=60,000 N=60 kNR_{1y} = R_{2y} = \frac{(4000)(30)}{2} = 60{,}000 \text{ N} = 60 \text{ kN}

Resultant forces: R1,2=452+602=75 kNR_{1,2} = \sqrt{45^2 + 60^2} = 75 \text{ kN}

Angle: θ=tan1(60/45)=53.1°\theta = \tan^{-1}(60/45) = 53.1°

Cable length: s=30+8(10)23(30)=38.9 ms = 30 + \frac{8(10)^2}{3(30)} = 38.9 \text{ m}

Example 3: Known Tension at Supports — Calculate Sag and Length

A 30 m cable with uniform load 4 kN/m has resultant tension at supports of 100 kN.

Vertical forces: R1y=R2y=(4)(30)/2=60 kNR_{1y} = R_{2y} = (4)(30)/2 = 60 \text{ kN}

Horizontal forces: R1x=R2x=1002602=80 kNR_{1x} = R_{2x} = \sqrt{100^2 - 60^2} = 80 \text{ kN}

Angle: θ=tan1(60/80)=36.9°\theta = \tan^{-1}(60/80) = 36.9°

Sag: h=qL28R1x=(4)(30)28(80)=5.6 mh = \frac{qL^2}{8R_{1x}} = \frac{(4)(30)^2}{8(80)} = 5.6 \text{ m}

Cable length: s=30+8(5.6)23(30)=32.8 ms = 30 + \frac{8(5.6)^2}{3(30)} = 32.8 \text{ m}

Inclined Cable Formulas

For cables spanning between supports at different heights with uniform horizontal load qq, the horizontal support forces are equal:

R1x=R2x=qa22h1=qb22h2R_{1x} = R_{2x} = \frac{qa^2}{2h_1} = \frac{qb^2}{2h_2}

When b>ab > a, the maximum resultant forces are:

R2=R2x2+(qb)2R1=R1x2+(qa)2R_2 = \sqrt{R_{2x}^2 + (qb)^2} \qquad R_1 = \sqrt{R_{1x}^2 + (qa)^2}

The angles between horizontal and resultant forces:

θ2=cos1(R2xR2)θ1=cos1(R1xR1)\theta_2 = \cos^{-1}\left(\frac{R_{2x}}{R_2}\right) \qquad \theta_1 = \cos^{-1}\left(\frac{R_{1x}}{R_1}\right)

Cable segment lengths:

sb=b(1+23(h2b)2)sa=a(1+23(h1a)2)s_b = b\left(1 + \frac{2}{3}\left(\frac{h_2}{b}\right)^2\right) \qquad s_a = a\left(1 + \frac{2}{3}\left(\frac{h_1}{a}\right)^2\right)

s=sa+sbs = s_a + s_b

Important Notes

  • The parabolic cable equations are valid when the sag-to-span ratio h/L<0.1h/L < 0.1. For larger ratios, use catenary equations instead.
  • The cable length approximation (Eq. 1d) is not valid when h>L/4h > L/4.
  • For cables loaded only with self-weight, these parabolic approximations apply provided the sag ratio condition is met.
  • Unit conversions: 1 kip=1000 lb1 \text{ kip} = 1000 \text{ lb} and 1 klf=1 kip/ft1 \text{ klf} = 1 \text{ kip/ft}.
  • The inclined chord equations use an iterative algorithm to fit the parabolic shape to the specified span LL and heights h1h_1, h2h_2.

Calculator Implementation Notes

The inclined cable calculator uses an iterative algorithm to adapt a parabola-shaped cable to the specified span L and heights h1 and h2. The resulting parabolic equation can be exported for use in spreadsheets or CAD systems.

Sag-to-Span Ratio Validity

The parabolic cable equations have two important validity constraints:

ConditionValidity
h/L < 0.1Equations apply to cables loaded only with self-weight
h/L < 0.25Cable length approximation s ≈ L + 8h²/(3L) is valid

Unit Definitions

For imperial calculations:

SymbolDefinition
kip1,000 lb
klfkip per linear foot

Inclined Cable Parabolic Equation

For inclined cables with supports at different heights, the cable shape follows:

y=ax2y = ax^2

where the coefficient aa is determined iteratively to satisfy the boundary conditions for span LL and heights h1h_1, h2h_2.

The total cable length is approximated by summing the segments:

s=sa+sbs = s_a + s_b

sa=a(1+23(h1a)2)s_a = a\left(1 + \frac{2}{3}\left(\frac{h_1}{a}\right)^2\right)

sb=b(1+23(h2b)2)s_b = b\left(1 + \frac{2}{3}\left(\frac{h_2}{b}\right)^2\right)

Inclined Cable Formulas (Continued)

For inclined cables with uniformly distributed horizontal loads, the relationship between the parameters defines the parabolic shape. The following derived equations are useful for analysis:

The lengths of each cable segment from the lowest point to the supports can be approximated as:

sb=b(1+23(h2b)2)s_b = b \left(1 + \frac{2}{3} \left(\frac{h_2}{b}\right)^2\right)

sa=a(1+23(h1a)2)s_a = a \left(1 + \frac{2}{3} \left(\frac{h_1}{a}\right)^2\right)

The total length of the sagged cable is the sum of these segments:

s=sa+sbs = s_a + s_b

The maximum cable forces occur at the supports. For the support at the lower point of the incline (Support 1), the resultant force is:

R1=R1x2+(qa)2R_1 = \sqrt{R_{1x}^2 + (q a)^2}

And for the higher support (Support 2):

R2=R2x2+(qb)2R_2 = \sqrt{R_{2x}^2 + (q b)^2}

The vertical components of the support forces are:

R1y=R12R1x2=qaR_{1y} = \sqrt{R_1^2 - R_{1x}^2} = q a

R2y=R22R2x2=qbR_{2y} = \sqrt{R_2^2 - R_{2x}^2} = q b

The angles the resultant forces make with the horizontal are:

θ1=cos1(R1xR1)\theta_1 = \cos^{-1}\left(\frac{R_{1x}}{R_1}\right)

θ2=cos1(R2xR2)\theta_2 = \cos^{-1}\left(\frac{R_{2x}}{R_2}\right)

Worked Examples (Continued)

Example: Known Support Tension - Calculate Sag and Length (SI Units)

For a 30 m long cable with a uniform load of 4 kN/m, the resultant tension at the supports is measured as 100 kN.

  1. Vertical Forces: Since the load is uniform and horizontal, the vertical forces at the supports are equal to the load carried on that segment. R1y=R2y=qL2=4 kN/m30 m2=60 kNR_{1y} = R_{2y} = \frac{q \cdot L}{2} = \frac{4 \text{ kN/m} \cdot 30 \text{ m}}{2} = 60 \text{ kN}

  2. Horizontal Forces: Using the Pythagorean theorem with the known resultant tension and calculated vertical force. R1x=R2x=Rsupport2R1y2=(100 kN)2(60 kN)2=80 kNR_{1x} = R_{2x} = \sqrt{R_{\text{support}}^2 - R_{1y}^2} = \sqrt{(100 \text{ kN})^2 - (60 \text{ kN})^2} = 80 \text{ kN}

  3. Sagging: Rearrange the horizontal force formula to solve for sag. h=qL28R1x=4 kN/m(30 m)2880 kN=5.625 mh = \frac{q \cdot L^2}{8 \cdot R_{1x}} = \frac{4 \text{ kN/m} \cdot (30 \text{ m})^2}{8 \cdot 80 \text{ kN}} = 5.625 \text{ m}

  4. Cable Length: Estimate the sagged cable length using the approximate formula. s=L+8h23L=30 m+8(5.625 m)2330 m32.81 ms = L + \frac{8h^2}{3L} = 30 \text{ m} + \frac{8 \cdot (5.625 \text{ m})^2}{3 \cdot 30 \text{ m}} \approx 32.81 \text{ m}

Inclined Cable Example Parameters

9 rows
Example parameters for an inclined cable with uniform horizontal load.
Parameter
Value
Span (L)30 m
Segment Length (a)7.21 m
Segment Length (b)22.8 m
Sag at Support 1 (h₁)1 m
Sag at Support 2 (h₂)10 m
Uniform Load (q)4 kN/m
Segment Length (sₐ)7.37 m
Segment Length (s_b)25.5 m
Total Cable Length (s)32.9 m

Source: engineeringtoolbox.com

References