
Measuring Intermetallic Phase Growth in Lead Free Solder Joints
Accurate intermetallic phase growth measurement requires bevel-free metallographic polishing, etching chemical selection, and kinetic modeling to set supplier liability limits.
Solid state diffusion processes at the copper tin interface create a distinct intermetallic phase that influences the mechanical properties and electrical conductivity of a soldered joint. This Cu3Sn planar layer, also known as the epsilon phase, forms between the base copper substrate and the thicker Cu6Sn5 layer during the soldering process and subsequent thermal aging. It is characterized by a high copper content and a relatively thin, uniform thickness compared to the scalloped morphology of the neighboring tin-rich phase.
The growth of this layer is driven by the diffusion of copper atoms into the tin-rich region, a process that continues throughout the life of the electronic assembly. While a thin layer is necessary for a strong metallurgical bond, excessive growth can lead to the formation of defects and a reduction in the overall ductility of the interconnect. The presence of this phase is a standard feature of most copper-solder interfaces, but its management is critical for high reliability applications in the automotive and aerospace sectors.
Growth of the intermetallic phase occurs primarily through the diffusion of copper atoms into the tin lattice and the subsequent reaction to form a stable crystalline structure. The Cu3Sn planar layer starts as a very thin film immediately after the reflow soldering process, where the temperature is high enough to melt the solder. As the joint cools and ages, the layer thickens through a solid state reaction that is highly sensitive to temperature.
The rate of growth follows a parabolic law, meaning the thickness increases with the square root of time. Higher operating temperatures significantly accelerate this process, leading to a more prominent layer over the life of the product. This phase is less stable than the Cu6Sn5 phase and acts as a transition zone between the bulk copper and the solder.
The crystal structure is orthorhombic, which differs from the hexagonal structure of the tin-rich phase. This difference in crystal symmetry contributes to the mechanical stresses that develop at the interface.
Long term exposure to elevated temperatures in the field causes the Cu3Sn planar layer to expand at the expense of both the copper substrate and the Cu6Sn5 layer. This growth is a common failure precursor in electronics subjected to continuous heat, such as power supplies or engine control units. As the layer thickens, it consumes the available copper, which can be problematic for thin copper traces on printed circuit boards.
The growth rate is also influenced by the composition of the solder alloy, with certain additives like nickel or cobalt used to suppress the diffusion of copper. In lead free soldering, the higher reflow temperatures often result in a thicker initial layer compared to traditional leaded processes. Thermal aging tests at 150 degrees Celsius are frequently used by manufacturers to simulate the effects of years of service and to monitor the stability of the interface.
A thick epsilon phase is generally associated with a higher risk of brittle fracture under mechanical load.
Brittleness in the solder joint often stems from the mechanical properties of the epsilon phase and its tendency to host microscopic defects. The Cu3Sn planar layer is significantly harder and less ductile than the bulk solder, making it a site for crack initiation during vibration or thermal cycling. A specific phenomenon known as Kirkendall voiding often occurs within this layer, where the unequal diffusion rates of copper and tin leave behind microscopic gaps.
These voids can coalesce into a continuous line of weakness, leading to a complete separation of the solder joint from the copper pad. This type of failure is particularly dangerous because it can occur suddenly without prior signs of electrical degradation. Quality control laboratories use metallographic cross sectioning and high resolution microscopy to measure the thickness of the layer and check for the presence of voids.
Maintaining a thickness below a few micrometers is often cited as a target for ensuring the long term reliability of the interconnect.

Accurate intermetallic phase growth measurement requires bevel-free metallographic polishing, etching chemical selection, and kinetic modeling to set supplier liability limits.
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