Beam Q, M & N Diagrams

Internal force diagrams (**shear Q**, **bending moment M**, **axial force N**) are the standard way to read how a **straight beam** carries loads to supports. This page uses a **simply supported** beam (pin at A, roller at B) of fixed span **L = 6 m** with a **downward point load** at a user-chosen position and a **uniformly distributed load (UDL)** over the full span. Reactions follow from **static equilibrium**; **Q(x)** is built from vertical forces to the left of a cut (with a **step** at the point load); **M(x)** integrates the shear pattern—**parabolic** under UDL, kinked under a point force—with **sagging moment taken positive**. **N** is modeled as a **uniform** axial term you set separately: vertical loads alone do not induce axial force in a horizontal beam, but the flat **N** diagram illustrates **superposition** when axial effects from columns or temperature are added in a larger model. The sketch is **schematic** (no deflection shape, shear deformation, or beam width).

Who it's for: Introductory statics and strength-of-materials students learning to sketch SFD/BMD and to separate flexural and axial resultants.

Key terms

  • Shear force diagram
  • Bending moment diagram
  • Axial force
  • Simply supported beam
  • Point load
  • Uniformly distributed load (UDL)
  • Static equilibrium
  • Sagging moment sign

How it works

For a **straight beam**, internal **shear Q** (here V), **bending moment M**, and **axial force N** describe section resultants. This page uses a **simply supported** span with a **point load** at a chosen position and a **uniform distributed load** over the whole span. **Q** jumps down at the point force; under UDL it **slopes linearly**. **M** is **parabolic** under UDL and piecewise between kinks; we take **sagging M > 0**. **N** is independent of vertical loads in this model and appears as a **flat line** for a uniform axial term (useful when superposing with a truss or column action).

Key equations

ΣF_y = 0, ΣM_A = 0 → R_A, R_B
Q(x) from vertical forces to the left of the cut
dM/dx = Q (with sign convention used here)

Frequently asked questions

Why does Q jump at the point load?
Across an **infinitesimal** segment carrying a **concentrated downward** force, equilibrium of the left segment requires the internal shear to **drop by P** so vertical forces still balance.
Why is M a parabola under UDL?
With **w** constant, **Q** decreases **linearly** along the span. Since **dM/dx = Q** in this sign convention, integrating gives **M** as a **quadratic** (parabola).
Does changing axial N affect Q or M here?
**No.** For a **straight horizontal** beam with **vertical** loads only, flexural resultants decouple from a **uniform axial** term in this linear model. The axial slider is for **conceptual** practice stacking effects.
Why might my textbook use opposite signs for M or V?
**Sign conventions differ** by country and author. Here **sagging M** is **positive** and **Q** is chosen to match that derivative relation. Always state your convention when comparing numbers.