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Fig.4. Experimental setup for reflection measurements (left) and a block diagram of the instrumentation for the microwave X and K- band. SO:
sweeper oscillator, VM: vector-volt-meter, r/t port: adapter for reflection/transmitting measurements, ref: reference signal, bus:IEEE bus, TH:
transmitting horn antenna, RH: receiving horn antenna, r: reflected signal.
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The dielectric function of snow with different stages of
metamorphism, and different amounts of liquid water has
been measured in the frequency rangefrom 20 MHz up to
16 GHz. Capacitive flat-plate sensors have been used in
the radio-frequency range of 20-40 MHz, the mono-pole
sensor has been appliedin the rangefrom 100 MHz up to 3
GHz, and in the X/K-bands reflection measurements of
electromagnetic waves on a smoothed snow surface have
been made using the free-space technique. Measurements
have beendoneinsitu on anatural snowcover in theStubai

Alps ([!]3000 m a.s.l.) and at the Hafelekar ([!]1900 m a.s.l.)
near Inns-bruck, Austria. Snowwetnesshas beenmeasured
by freezing calorimetry; and snow density has been
measured simply by weighing a known volume of snow.
Snow porosity has been calculated from the volumetric
liquid water content Wand snow density. The experimen-
tally found relation between snow mission.
Incremental permittivity E (real part), snow liquid wa-
ter content W (volume basis), and frequency of sensor op-
eration is shown in Fig.5 as a 3-D wetness calibration plot
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on a logarithmic frequency scale. E, the incremental per-
mittivity, is defined as:
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E =e ' (wet) e'(dry)
e'(wet) is the(measured)dielectric functionof wet snow,
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e'(dry) is the (calculated) dielectric function of snow with
the same porosity F:
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e' (dry) = 1 + 1.76 (1-F ) + 0.37 (1- F )2
For practicalreasons - and acceptinga slightly reduced
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accuracy in determining snow wetness - the very weak
effect of water geometry on the snow dielectric function
has been neglected, and it results a simple quadratic rela-
tion between snow wetness W (in % by volume) and in-
cremental permittivity: E = a W + ßW2 , whereby the pa-
rameters a and ß depend on the actual frequency f' of
sensor operation:
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