A Brief Overview of Thermal Stress in Resin 3D Printing

Thermal Stress Basic Concepts

Thermal stresses are stresses that arise when the thermal deformation of an object caused by a change in temperature is restrained. However, a change in temperature alone does not necessarily produce stresses within the object, but only when the expansion or contraction caused by the change in temperature is restrained, will produce stresses within the object. This kind of no external force but due to the temperature change caused by thermal deformation is constrained and produced by the stress, known as thermal stress or temperature stress.

With more simple words to describe that is, under normal circumstances the material is subjected to temperature changes. Most of them will undergo some deformation due to thermal expansion and contraction and other principles. And if this deformation process is constrained, thermal stresses will be generated.

Let's consider a metal rod with a diameter of dd and length of ll at the initial temperature of t0t_0. If we heat it evenly to a temperature of t1t_1, the rod will expand to:

Length change: Δl=α(t1t0)l\Delta l = \alpha (t_1 - t_0)l

Length strain: ϵl=Δll=α(t1t0)\epsilon_l = \frac{\Delta l}{l} = \alpha (t_1 - t_0)

Diameter change: Δd=α(t1t0)d\Delta d = \alpha (t_1 - t_0)d

Diameter strain: ϵd=Δdd=α(t1t0)\epsilon_d = \frac{\Delta d}{d} = \alpha (t_1 - t_0)

That is, if the temperature of the rod is increased from t0t_0 to t1t_1, the strain of the rod will be:

ϵ=α(t1t0)=αΔt\epsilon = \alpha (t_1 - t_0) = \alpha \Delta t

Where α\alpha is the coefficient of thermal expansion of a certain material, it varies with the material and temperature, if the temperature is constant, α\alpha is a constant.

For an isotropic cube, uniform heating or cooling produces free expansion or contraction, with the same degree of elongation or contraction in the three directions of length, width and height, but no shear deformation, only longitudinal deformation.

If a metal bar expands freely and is not constrained, then no thermal stresses are generated. And put it between two rigid body wall, fixed ends, then in the rod heat task rises to t1t_1, because by the rigid body wall to prevent, it can not expand, and will produce compression thermal stress. Thus although there is no external force acting, the thermal deformation is externally constrained and stresses are also generated within the object.

In addition, within the same object, if the temperature is not uniformly distributed, although the object is not subject to external constraints, but because of the different temperatures in each place, each part can not be free to expand and contract due to the influence of neighboring parts with different temperatures, will also produce thermal stresses within.

Also, a component consists of a number of parts made of different materials that are combined, even if subjected to the same heating or cooling, but due to the various parts of the expansion coefficient is different, or the expansion of different ways, resulting in the parts of each other constraints, can not be free to expansion and contraction, thus generating different thermal stress.

Thus, to summarize, the stresses arising from a change in the temperature of an object due to mutual constraints between it and other objects that are not free to expand or contract, or between the internal parts of an object, become thermal stresses. This is a non-external force caused by the stress, the root cause is the temperature change and constraint. Constraints can be summarized in three forms:

Thermal stresses lead to an uneven distribution of stresses inside and on the surface of an object, which may cause deformation or damage. The magnitude and direction of thermal stresses depend on factors such as the material, shape and size of the object, the degree and rate of temperature change, and the manner in which it is cooled or heated.

The Basic Equations Of Thermal Elasticity

Take a tiny parallel hexahedron with sides parallel to the coordinate axis and side lengths of dx,dy,dzd_x, d_y, d_z , as shown in the figure:

The stress component acting on the microelement surface:

σxx,σyy,σzz,τxy,τxz,τyx,τzx,τzy,τzz\sigma_{xx}, \sigma_{yy}, \sigma_{zz}, \tau_{xy}, \tau_{xz}, \tau_{yx}, \tau_{zx}, \tau_{zy}, \tau_{zz}

By the shear stress reciprocity theorem:

τxy=τyz,τyz=τzy,τxz=τzx\tau_{xy} = \tau_{yz}, \tau_{yz} = \tau_{zy}, \tau_{xz} = \tau_{zx}

Stresses and strains generated by external forces are calculated using the principles of mechanics of materials and elasticity. Thermal stresses and strains thermal strains generated by temperature changes are calculated using the principles of thermoelastic mechanics, and the two are superimposed.

Thermal Stress in SLA 3D Printing

With the rapid development of industrial technology, the problem of thermal stress and deformation caused by uneven temperature or inconsistent coefficient of thermal expansion has become a major problem in certain projects, which is mainly manifested in:

In the light-curing 3D printing process, the liquid photosensitive resin is excited by ultraviolet light and cured to a solid by a cross-linking reaction. However, this UV-induced chemical reaction is also accompanied by the release of energy, which can lead to the warming of localized areas of the material. The uneven distribution of temperature changes generated during the curing process causes internal deformation constraints in the printed part, in which case the material shrinks or expands, which in turn generates thermal stresses. The process of generating thermal stress is as follows:

Reducing the Effects of Thermal Stress

This generation of thermal stresses may lead to problems such as deformation, cracking and damage to the print. In life thermal deformations and thermal stresses may adversely affect the system and in general there are several measures in principle:

In order to reduce the impact of thermal stress in light-curing 3D printing, the following methods can be taken: