Related Experiment Video
Updated: Apr 15, 2026

06:43
Effective Analysis of Human Exposure Conditions with Body-worn Dosimeters in the 2.4 GHz Band
Published on: May 2, 2018
7.5K
Experimental Path Loss Models for In-Body Communications Within 2.36-2.5 GHz
IEEE Journal of Biomedical and Health Informatics
|April 4, 2015
Summary
This study investigates radio propagation for in-body sensors above 1 GHz, offering new path loss formulas for higher data rates. This research supports advanced biomedical telemetry and chronic disease management.
Area of Science:
- Biomedical Engineering
- Wireless Communications
- Radio Frequency Engineering
Background:
- Biomedical implantable sensors are crucial for chronic disease management, typically operating below 1 GHz.
- Lower frequencies offer reduced propagation loss but limited data rates due to narrow bandwidths.
- Advanced sensors and actuators require higher data rate communication, necessitating exploration of higher frequencies.
Purpose of the Study:
- To evaluate radio propagation characteristics for in-body sensors in frequency bands above 1 GHz.
- To investigate the feasibility of using the 2360-2400 MHz and 2400-2483.5 MHz bands for in-body communication.
- To develop empirical path loss models for various in-body communication scenarios.
Main Methods:
- Utilized a phantom-based approach to simulate radio propagation through biological tissues.
- Conducted propagation measurements for three scenarios: in-body to in-body, in-body to on-body, and in-body to off-body.
- Analyzed data to derive path loss formulas for the studied frequency bands.
Main Results:
- Presented novel path loss formulas for in-body communication in the 2.36-2.48 GHz range.
- Quantified radio propagation losses for different communication links (in-body to in-body, on-body, off-body).
- Demonstrated the potential of higher frequency bands for increased data rates in medical sensing.
Conclusions:
- The study provides essential data for designing next-generation high-data-rate wireless in-body sensors.
- The developed path loss models can guide the optimization of antenna design and system performance.
- Findings support the consideration of spectrum above 1 GHz for advanced wearable and implantable medical devices.
Related Concept Videos
Propagation Speed of Electromagnetic Waves
5.0K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
5.0K
Boundary Conditions: Lossless Lines
462
Consider a single-phase, two-wire, lossless transmission line terminated by an impedance at the receiving end and a source with Thevenin voltage and impedance at the sending end. The line, with length, has a surge impedance and wave velocity determined by the line's inductance and capacitance.
At the receiving end, the boundary condition states that the voltage equals the product of the receiving-end impedance and current. This relationship is expressed as a function of the incident and...
At the receiving end, the boundary condition states that the voltage equals the product of the receiving-end impedance and current. This relationship is expressed as a function of the incident and...
462
Transmission Line Design Considerations
771
Aluminum has become the material of choice for overhead transmission lines, surpassing copper due to its abundance and cost-effectiveness. The most prevalent type is the aluminum conductor, steel-reinforced (ACSR), which combines aluminum strands around a steel core. Other variants include all-aluminum conductors (AAC), all-aluminum alloy conductors (AAAC), aluminum conductor alloy-reinforced (ACAR), and aluminum-clad steel conductors. Advanced designs, such as aluminum conductors with steel...
771
Lossless Lines
658
In electrical engineering, a lossless transmission line is characterized by a purely imaginary propagation constant and a resistive characteristic impedance. The ABCD parameters, which describe the relationship between the input and output voltages and currents, indicate an equivalent π circuit with an imaginary series impedance and a shunt admittance. This results in a transmission line that, when the product of the phase constant (beta) and the length of the line is less than pi,...
658
Plane Electromagnetic Waves I
5.4K
The existence of combined electric and magnetic fields that propagate through space as electromagnetic (EM) waves is the most significant prediction of Maxwell's equations. As Maxwell's equations hold in free space, the predicted electromagnetic waves do not require a medium for their propagation. An EM wave comprises an electric field, defined as the force per charge on a stationary charge, and a magnetic field, which is the force per charge on a moving charge.
The EM field is assumed to be a...
The EM field is assumed to be a...
5.4K
Traveling Waves: Lossless Lines
538
The provided content explores the behavior of traveling waves on single-phase lossless transmission lines. It begins with a single-phase two-wire lossless transmission line of length Δx, characterized by a loop inductance LH/m and a line-to-line capacitance C F/m. These parameters result in a series inductance LΔx and a shunt capacitance CΔx.
538

