
 
measurements in vitro. Additionally, 12 channels are 
available for communication, allowing multiple 
instrumented animals to be housed in close 
proximity. 
Power is provided wirelessly to the implant using 
inductively coupled power transfer (Budgett, Hu et 
al. 2007).  This has allowed high power devices 
(relatively speaking) such as A/D converters, 
microcontrollers and digital transmission systems to 
be used. During use, the implant can be charged by 
placing a coil under the animal’s home cage through 
which high frequency AC current is passed. Power is 
received at the implant by a ferrite pickup which is 
magnetically coupled to the charging coil.  
Information about the charge state of the battery and 
power received are embedded in the BP/SNA data 
packets and transmitted to the wireless power 
supply. The magnetic field can then be controlled 
such that only the required amount of power is 
delivered to the implant. This reduces the 
temperature rise during charging to approximately 
5°C. 
 
Figure 3: Block diagram of the telemeter. 
Between charging, a 70 mAH lithium ion coin 
cell provides power. Consumption is 6 mA during 
continuous operation which results in a battery life 
of 12 h.  In vivo charging takes between 2 and 4 
hours and is dependent on how active the animal is 
and how close the implant’s orientation is to the 
optimum for charging. During charging SNA 
recording is not possible as the nerve signal is 
swamped by noise generated by the 200 kHz 
charging field. 
2.2  Blood Pressure Measurements 
Blood pressure measurements are performed using a 
10cm fluid filled polyurethane catheter, which acts 
as an interface between the measurement site (for 
instance the aorta) and the piezo resistive pressure 
transducer in the telemeter. Pressure waveforms are 
transmitted along the catheter using low viscosity 
biocompatible fluid. No obvious reference pressure 
is available internally to make measurements 
against. Therefore, an absolute pressure sensor (one 
with an internal vacuum reference) is used. 
Physiologically, the pressure of interest is the 
difference between the blood pressure and the 
ambient or atmospheric pressure.  This pressure is 
derived by measuring the atmospheric pressure 
using a second absolute transducer and subtracting it 
from the internal pressure. 
2.2.1  Frequency Response 
Accurate measurements of systolic and diastolic 
pressure require the use of a wide bandwidth 
measurement system.  One historical rule of thumb 
is that the bandwidth should be greater than 10 times 
the heart rate (Gabe 1972).  For a rat, the maximum 
heart rate that can be reasonably expected is 500 
beats per minute. This requires a bandwidth of 
greater than 80 Hz. 
 
Figure 4: Frequency Response Measurement System. 
In order to characterise the telemeters pressure 
measurement bandwidth, the rig represented by 
Figure 4 was constructed. A fluid filled chamber acts 
as a pressure source for frequency response 
measurements. Pressure waveforms are generated by 
a voice coil actuator which exerts force on the fluid 
through a thin brass diaphragm. The catheter of the 
device under test (DUT) is inserted into the chamber 
using a luer lock adaptor. A second high bandwidth 
transducer provides a reference pressure for 
calculations. Provided compliance of the chamber is 
minimized, the system’s measurement bandwidth 
can be high. Bandwidths of 5 kHz (-3 dB) have been 
attained with usable signals present until approx 
15 kHz. 
Tests are preformed using the swept sine 
technique where sinusoidal perturbations are applied 
to the DUT.  The LabVIEW Sound and Vibration 
Analysis Toolbox (www.labview.com) 
automatically calculates the magnitude transfer 
function from reference pressure (P
ref
) to telemeter 
output (P
T
) as defined by equation 1. 
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