In one line
A force acting on a rigid body can be slid anywhere along its own line of action without changing its external effect on the body.
Explained simply
Push a stalled car from the back, or pull it with a rope from the front along the same line: the car moves the same way. Where along the line you apply the force does not matter for the motion of the whole car.
Formally: the external effect of a force on a rigid body remains unchanged if the point of application is moved to any other point on its line of action, keeping magnitude and direction the same.
How it works
- A force has magnitude, direction, sense and line of action.
- Moving it along its own line keeps all four unchanged, so the net force on the body is the same.
- The perpendicular distance from any point to the line also stays the same, so its moment about every point is the same.
- Same net force and same moment about every point means the same external effect (motion or support reactions).
- This lets us slide a force to a convenient point, for example to where its components have easy moment arms.
Key formula
Moment about O before and after sliding: \( M_O = F \times d \), where \( F \) is the force (N) and \( d \) is the perpendicular distance (m) from O to the line of action. Since \( d \) does not change when the force slides along its line, \( M_O \) (N·m) is unchanged.
Quick example
A 100 N force acts on a beam at 30° to the horizontal. To find its moment about a support, slide it along its line until it meets the beam's axis; then only its vertical component \( 100 \sin 30^\circ = 50 \) N has a moment arm, which makes the calculation quicker.
Common mistakes
- Applying the principle to deformable bodies: internal stresses depend on where the force acts, so it is valid only for rigid bodies and external effects.
- Moving the force parallel to itself (to a different line); that changes its moment and needs an extra couple.
- Thinking the principle applies to internal forces of a structure; it does not.
How MU asks it
Asked as a 3-mark theory part in Q.1: 'State and explain the principle of transmissibility with a sketch'. Write the statement, show a body with force F at A and the same force at B on the same line, and add one line on its limitation (rigid bodies, external effect only). Sometimes it is clubbed with 'Explain the difference between transmissibility and moving a force to a parallel position'.