Assignment title: Information
1
Mid-term exam in FYS-2008, autumn 2016
Department of Physics and Technology
University of Tromsø
NB! Deadline for handing in: Monday 31st October 23:59 in Fronter
This exam paper consists of four pages.
Problem 1: Heavy suitcase
Setting: You are ready to go to Silicon Valley to make a fortune. However, as you
drag your suitcase out to the car, you start thinking about the maximum weight
allowed on this flight: 23 kg. As you are broke, an overweight fee will stop your
plans. You decide to take the bathroom scales out to the car and measure the
weight. These are state-of-the-art bathroom scales with specified maximum
error 0.2% of FSD for standard conditions (temperature 20°C, battery voltage
3.0V, range 0-120kg). Ready to measure the suitcase next to the car, the display
on the scales says -10°C and the display is flickering due to low battery voltage:
2.5 V (also indicated). With the suitcase on, the scales show 22.8 kg.
Note: It is advised to make some plots, e.g. of calibration curves, non-linearity,
equations found and deviations from the equations.
Table 1
Calibration of bathroom scales. The displayed value Wout is given with certified
weights Win on the scales. Standard conditions: 20°C and 3V. To find interfering
and modifying inputs, the scales have been calibrated versus temperature and
voltage for two input weights: 0 kg and 120 kg, marked as W0 and W120 in the
table. For this, a certified temperature chamber and voltage source was used.
Std. conditions Temperature Voltage
Win (kg) Wout (kg) T (°C) W0 (kg) W120 (kg) V (V) W0 (kg) W120 (kg)
0.00 -0.02 10 -0.25 119.73 2.6 0.02 119.54
15.00 15.08 15 -0.14 119.81 2.8 -0.03 119.78
30.00 30.17 20 0.03 119.96 3.0 -0.04 120.00
45.00 45.17 25 0.15 120.12 3.2 0.05 120.26
60.00 60.22 30 0.29 120.29
75.00 75.22
90.00 90.13
105.00 105.05
120.00 119.982
a) Calibration
Being a meticulous and trained measurement specialist, you have previously
calibrated the scales, see table 1. Find the ideal equation for the scales for
standard conditions (20°C and 3.0V).
b) Non-linearity and error
What is the maximum non-linearity and error of the scales for standard
conditions? Does it comply with the specified maximum error of 0.2% of FSD?
Find an expression for the non-linearity.
c) Interfering and modifying inputs
Are temperature or battery voltage interfering or modifying inputs? Find the
relevant coefficients (KI and KM).
d) Calibrated expression
Put together the answers in a) to c) to give a complete expression for the
displayed weight (Wout) as a function of the weight put onto the scales (Win),
taking into account any non-linearity, interfering and modifying inputs.
e) True value for 22.8 kg displayed
Returning to the suitcase, what is the estimated true weight of the suitcase? I.e.
for displayed weight 22.8 kg, temperature -10°C and battery voltage 2.5V.
Problem 2: Capacitive sensor
In this problem we will study two methods for measuring capacitance induced
by a capacitive type of sensor.
a) Step input
Let us first consider the experimental setup shown in Fig.1. Here a signal
generator is modeled as a potential source V in series with a resistor RS. The
signal generator is then connected to a capacitive sensor yielding a capacitance
CS and an output voltage U with respect to ground (GND) is measured by a high
impedance oscilloscope.
Figure 1 Signal generator and sensor.
Problem 1
In this problem we will study some methods for measuring capacitance induced by a capacitive
type of sensor.
a) Let us first consider the experimental setup shown in Fig.1. Here a signal generator is
modelled as a potential source ܸ in series with a resistor ܴ௦. The signal generator is then
connected to a capacitive sensor yielding a capacitance ܥ௦ and an output voltage ܷ with
respect to ground (GND) is measured by a high impedance oscilloscope.
Fig. 1
In order to estimate the sensor capacitance, we program the signal generator to give the
following step potential:
ܸ = 0 for t < 0
ܸ = ܸ = ܿ ݐݏ݊for t >= 03
In order to estimate the sensor capacitance, we program the signal generator to
give the following step potential:
V = 0, for t < 0
V = V0 = const for t > 0
Obtain the transfer function for the system in Fig. 1 and find the solution for U as
a function of time with initial condition U(t = 0) = 0.
Illustrate how this solution can be used to estimate Cs if we assume the
resistance RS in Fig. 1 to be known.
b) Dynamic error
Consider the system given in a). What is the dynamic error of the system? Plot
the dynamic error for voltage V0 = 5V, resistance RS = 1kΩ and sensor
capacitance CS in the range 20-100 nF. Use a few values of the sensor capacitance
to illustrate how the error evolves.
c) Bridge
A second option for measuring CS is shown in Fig. 2. Here the capacitance sensor
is inserted in a bridge circuit together with a constant capacitor C0 and two
constant resistors that both have a resistivity value R. An AC potential V acts as
the potential source as shown in Fig. 2, while the potential difference Ub - Ua is
measured by a high impedance voltage probe assumed to put no load on the
circuit.
Figure 2 Capacitance sensor in bridge
Further on, we assume that the sensor gives a linear capacitance
CS = C0(1-αΔd)
where α is a sensor constant.
Write down the potential relation for the suggested bridge and show that the
output potential can approximated by
Ub - Ua ≈ ¼VαΔd
assuming |αΔd|≪1.
d) A third option for measuring ܥ௦ is shown in Fig. 3. Here the capacitance sensor is inserted a
bridge circuit together with a constant capacitor ܥand two constant resistor that both have a
resistivity value ܴ. An AC potential ܸ acts as the potential source as shown in Fig. 3, while
the potential difference ܷ െ ܷ is measured by a high impedance voltage probe assumed to
put no load on the circuit.
Fig. 3
Further on, we assume that the capacitive sensor gives a linear
ܥ௦
= (ܥ1 െ ߙȟ݀)
where ߙis a sensor constant.
Write down the potential relation for the suggested bridge and show that the output potential
can approximated by
ܷ ܷ െ
ܸ 4
݀ȟߙ
assuming |ߙȟ݀| ا1.
e) In the last point we will look at the quantization error and other uncertainties involved in the
bridge measurement. We will assume that the potential difference ܷ െ ܷ is amplified and
then digitized by an AD-converter. The output from the AD-converter is assumed to be within4
Problem 3 Accelerometer
According to Wikipedia:
An accelerometer is a device that measures proper acceleration; proper
acceleration is not the same as coordinate acceleration (rate of change of
velocity). For example, an accelerometer at rest on the surface of the
Earth will measure an acceleration due to Earth's gravity, straight
upwards (by definition) of g ≈ 9.81 m/s2. By contrast, accelerometers in
free fall (falling toward the center of the Earth at a rate of about 9.81
m/s2) will measure zero.
Find three types of accelerometers and for each of them, describe:
- Measurement principle
- Typical specifications, e.g.: Range, noise/resolution, frequency range,
size, etc.
- Typical applications
- 'Killer application': One example where this accelerometer is better
suited than the other listed.
Hints:
Types: The three types should be based on different measurement principles.
References: Write where you found the information, e.g. link to web-pages.
Figures: You can copy figures from internet, books, etc. But remember to tell
where you found it => reference.
Tables: It is nice to include tables, e.g. with specifications. But do not include all
values! Make a critical selection and include e.g. typical, minimum and maximum
values.