2.1.2 Deflections under the vertical (normal) force component

2.1.2 Deflections under the vertical (normal) force component

Let us determine the magnitude and direction of the deformation arising from the vertical force . Solution to this problem will allow to find components of the third column of tensor (see (2) in chapter 2.1.1).




Deformation that we call here the vertical bending of z-type is shown in Fig. 1.

Fig. 1. Vertical deflection of the z-type.

Next, let's examine a section of the beam. We will cut the beam and consider the deformation of the beam element having length between the two cross sections (Fig. 2). Since this element is bent, the material at the outer edge is stretched in tension while at the inner edge it is compressed. Hence, there is a neutral plane of zero stress between the two surfaces. For calculations simplification we assume that the beam cross-sections remain planar and normal to their centroidal axis (pure bending of the uniform cross-section beam). This assumption is valid if [1] which is true in our case.

Fig. 2a.  Section of the bent beam.

Fig. 2b.  Beam cross-section.

At the pure bending the neutral plane passes through the centroid of the beam cross-sectional area [2], i.e. in our case the parallepiped long axis belongs to the neutral plane. The material longitudinal extension is proportional to the distance z from the neutral plane: (Fig. 2). According to the Hooke's law, the force acting on a unit area in a small strip near z with square is equal to , where – Young's modulus, – beam curvature radius. If any cross-section is considered, the forces are acting in one direction over the neutral surface and in the other direction below it. This makes a couple of forces producing the bending moment , which is a moment of forces with respect to the neutral axis:


The quantity , is called the axial moment of inertia of the beam section about the axis that passes through its centroid. For the beam with rectangular cross-section it is given by:


By we denote the deflection of the beam point at the distance y from the fixed end in the z-direction. The curvature of the curve at small bends ( ) is given by . Then, taking into account expression (5), the bending moment can be expressed as


On the other hand, is a moment of forces with respect to point y due to the action of force – and the beam own weight – . Thus, we derive an equation:


Integration of (7) having for boundary conditions and , gives:


The beam end deflection (Fig. 1) is:


The second summand is the deflection under own weight. For a typical cantilever, it is of the fraction of the angstrom and can be neglected because in AFM experiments the first term is hundreds of time more. Relation (9) is nothing but expression (3) in which we should suppose:


The beam deflection angle calculated without the second term in (9) is as follows:


The coefficient of inverse stiffness is the largest among the tensor components. In (11) this parameter is specially denoted as " " without indexes. In particular, magnitude of characterizes the cantilever stiffness and is one of its major parameters. Below, for the purpose of obviousness, we will take outside as a common multiplier of all the matrix (see (2) in chapter 2.1.1) components. For a cantilever with rectangular cross-section, (11) can be rewritten as


From formula (10) and diagram for the beam vertical bending of z-type (Fig. 1) it is easy to derive the tip deflection induced by the force application:


From (13) and (1), (2), (3) it is clear that


Taking into consideration that , we get


Finally, we calculate the components of the matrix (3) from chapter 2.1.1 third column. From expressions (9–12) it follows that


Because under the influence of the force the top cantilever surface does not bend in the direction, then



  • The z-type deflection is a result of the vertical bending force action.
  • To find the components of the inverse stiffness tensor corresponding to the z-type deflection, one should solve the problem of the beam static deflection which is reduced to the ordinary differential equation of the second order.
  • The vertical force results in the tip deflection in vertical and longitudinal directions and in the deflection angle appearance.
  • Besides the supporting force from the sample, the cantilever is influenced in vertical direction by its own gravity. Under this load the cantilever free end is deflected but such a deformation is small compared to minimal detected displacement.


  1. Feynman R., Leighton R., Sands M. The Feynman Lectures on Physics, volume 7. – MIR, 1966. – 292 p. (in Russian)
  2. Gorshkov A.G., Troshin V.N., Shalashilin V.I. Strength of Materials. – FIZMATLIT, 2002. – 544 p. (in Russian)