Significantly reduced c-axis thermal diffusivity of graphene-based papers.
Meng Han1, Yangsu Xie2, Jing Liu3
1Department of Mechanical Engineering, 2010 Black Engineering Building, Iowa State University, Ames, IA 50011, United States of America.
Nanotechnology
|April 6, 2018
Summary
This study investigates the thermal properties of graphene-based papers, finding that defects limit heat transfer. Optimizing graphene nanostructures is key for effective thermal management materials.
Area of Science:
- Materials Science
- Nanotechnology
- Thermal Engineering
Background:
- Graphene-based films/papers offer high thermal conductivity and surface-to-volume ratio.
- They are considered for lightweight thermal interface materials and lateral heat spreaders.
- Understanding their cross-plane thermal properties is crucial for material optimization.
Purpose of the Study:
- To investigate the cross-plane thermal conductivity (k_c) and diffusivity (α_c) of partially reduced graphene paper (PRGP) and graphene oxide paper (GOP).
- To compare the thermal properties of PRGP and GOP with highly-reduced graphene paper and graphite.
- To elucidate the factors influencing thermal transport in these graphene-based materials.
Main Methods:
- Experimental determination of cross-plane thermal diffusivity (α_c) for PRGP and GOP across a temperature range (12-295 K).
- Analysis of material structure, including grain size and defect density, to correlate with thermal transport.
- Comparative analysis with other graphene-based materials and graphite.
Main Results:
- PRGP exhibited low α_c attributed to phonon scattering from grain boundaries and defects.
- GOP showed limited cross-plane thermal transport due to functional groups hindering direct energy coupling between layers.
- Thermal transport in GOP is described as occurring through "weak thermal transport tunnels".
Conclusions:
- Defects and functional groups significantly impact the thermal performance of graphene-based papers.
- PRGP and GOP demonstrate limitations in cross-plane thermal transport compared to highly-reduced graphene.
- This research provides insights for tailoring graphene nanostructures to achieve desired thermal properties for advanced applications.
More Related Videos
Related Concept Videos
Diffusion
221.8K
Diffusion is the passive movement of substances down their concentration gradients—requiring no expenditure of cellular energy. Substances, such as molecules or ions, diffuse from an area of high concentration to an area of low concentration in the cytosol or across membranes. Eventually, the concentration will even out, with the substance moving randomly but causing no net change in concentration. Such a state is called dynamic equilibrium, which is essential for maintaining overall...
221.8K
Diffusion
6.5K
Diffusion is a type of passive transport. In passive transport, a substance tends to move from an area of high concentration to an area of low concentration until the concentration is equal across the space. For example, take the diffusion of substances through the air. When someone opens a perfume bottle in a room filled with people, the perfume is at its highest concentration in the bottle and is at its lowest at the edges of the room. The perfume vapor will diffuse, or spread away, from the...
6.5K
Hypothalamic-Pituitary Axis
66.5K
The response to stress—be it physical or psychological, acute or chronic—involves activation of the Hypothalamic-Pituitary-Adrenal (HPA) axis. The HPA axis is part of the neuroendocrine system because it involves both neuronal and hormonal communication. Its function is to regulate homeostatic systems—metabolic, cardiovascular, and immune—providing the necessary means to respond to a stressor.
66.5K
Perpendicular-Axis Theorem
4.6K
The perpendicular-axis theorem states that the moment of inertia of a planar object about an axis perpendicular to its plane is equal to the sum of the moments of inertia about two mutually perpendicular concurrent axes lying in the plane of the body.
Consider a circular disc of mass M and radius R lying along an x-y plane. The origin lies at the center of the disc, and the z-axis is perpendicular to the disc's plane. All three axes coincide at the disc's center. The moment of inertia of this...
Consider a circular disc of mass M and radius R lying along an x-y plane. The origin lies at the center of the disc, and the z-axis is perpendicular to the disc's plane. All three axes coincide at the disc's center. The moment of inertia of this...
4.6K
Parallel-axis Theorem
8.3K
The parallel-axis theorem provides a convenient and quick method of finding the moment of inertia of an object about an axis parallel to the axis passing through its center of mass. Consider a thin rod as an example. There is a striking similarity between the process of finding the moment of inertia of a thin rod about an axis through its middle, where the center of mass lies, and about an axis through its end using the conventional method. In the conventional method, the concept of linear mass...
8.3K
Thermal expansion and Thermal stress: Problem Solving
2.2K
San Francisco's Golden Gate Bridge is exposed to temperatures ranging from -15 °C to 40 °C. At its coldest, the main span of the bridge is 1275 m long. Assuming that the bridge is made entirely of steel, what is the change in its length between these temperatures?
To solve the problem, first, identify the known and unknown quantities. The initial length (L) of the bridge is 1275 m, the coefficient of linear expansion (α) for steel is 12 x 10-6/°C, and the change in temperature (ΔT) is 55...
To solve the problem, first, identify the known and unknown quantities. The initial length (L) of the bridge is 1275 m, the coefficient of linear expansion (α) for steel is 12 x 10-6/°C, and the change in temperature (ΔT) is 55...
2.2K


