A
review of whole-plant water use studies in trees: Wullschleger Stan et al. 1998
The
article described reviewed fifty two studies previously conducted on
whole-plant water use, detailing the different techniques used in doing
so. The techniques vary from modern
energy-balance and heat dissipation methods to older techniques such as weighing
lysimeters, large-tree photometers, ventilated chambers, and
radioisotopes. The accuracy of water-use
measurements between these techniques varies a great deal, and as such, the
variation in trees studied ranged from 10 kg day-1 to 1,180 kg day-1,
with the majority of measurements falling between 10-200 kg day-1. The merits and drawbacks of each category of
technique was evaluated. Weighing
lysimeters are sensitive to small changes, but they are very expensive to
maintain. Large-tree photometers can
often change the amount of water that the tree originally would have used. Radioactive tracers like tritium are being
phased out due to environmental and regulatory concerns. Heat-pulse and heat-dissipation techniques
are gaining widespread acceptance because of their relative
inexpensiveness. Drawbacks of the
heat-pulse and heat-dissipation techniques include empirical calibration
inaccuracies, and variation in flux through the depth of the sapwood, but many of
these concerns are being addressed through new methods of applying the said
techniques. The article recommends the
continued use of heat-pulse and heat-dissipation methods in the future to
estimate whole-tree water use.
Physiological
impacts: There are five main places the article elaborates on in terms of
physiological impacts of measuring whole-tree water use.
Stomatal
and boundary layer control of whole-tree water use:
Measuring
whole-tree water use gives several benefits in evaluating the role of the
stomata in controlling transpiration.
Having quantitative values allows scientists to make meaningful
hypotheses about several factors. In
fact, Jarvis et al. (1986) elaborates by introducing a dimensionless decoupling
coefficient (Ω) which measures the relative amount that the stomata affects the
whole-tree transpiration rate. The
closer Ω is to zero, the more control the stomata has on the rate of
transpiration of the whole tree.
Conversely, the closer Ω is to one, the less control the stomata has on
the rate of transpiration. For a tree
with large leaves (Tectona grandis
has a leaf size of 700 cm2), Ω approaches one and the stomata
conductance is so high that it cannot influence the rate of transpiration in
the tree.
Whole-tree
estimates of hydraulic conductance:
Hydraulic
conductance is the measure of water flow from the soil to the trunk via the
roots of the tree. With the advent of
easily measurable whole-tree water use, hydraulic conductance is measurable
simply by a conversion described by
, where
is hydraulic conductance,
is an estimate of current transpiration, and
is the difference between maximum and current
leaf water potential. Estimating
hydraulic conductance is important physiologically because it allows
researchers to evaluate the benefits of certain designs of tree growth. For example, scientists can assess the
trade-offs between
and vulnerability to xylem cavitation –
something that would be controlled through evolution.
Coordinated
control of stomatal and hydraulic conductance:
Quantitative
measurements of whole-tree water use can help scientists assess the correlation
between stomatal and hydraulic conductance in trees. There is substancial evidence that stomatal
and hydralulic conductance are positively correlated – when
increases, stomatal conductance and leaf
transpiration also sharply increase.
This shows that stomata respond quickly and sharply to changes in water
transport efficiency.
Sapwood
water storage:
In
large trees such as oak, there is a considerable lag between changes in
transpiration and changes in water flux at the base of the tree. This lag shows that there is a significant
storage of water inside the tree. By
measuring at both ends of the tree, it is possible to quantitatively determine
the quantity of stored water inside the tree.
This measurement can help scientists measure the drought-resistance of
certain trees.
Granier’s
Thermal Dissipation Probe (TDP) Method for Measuring Sap Flow in Trees: Theory
and Practice: Ping Lu, Laurent Urban, Ping Zhao, et al.
This
article thoroughly reviews the thermal dissipation method first described in
Granier 1987. This method is one of the
most popular ones to determine whole-tree water use in modern day. This is because of the Granier method’s
simplicity, high degree of accuracy, and relatively low cost. A comprehensive review of the technique will
help refine future methods of measurement using the TDP method. Several practical issues such as the
determination of non-flow values, natural gradient, wounding effect, reversed
sap flow, and flux scaling are discussed.
The
original Granier method was published by Andre Granier in French. Therefore, there have been many
misunderstandings on the technique and misuse of the methods. The purpose of the article is to clarify many
of these misunderstandings and give a clear overview of the technique,
including how to scale measurements from a point to cross section, and then to
the tree level.
The
theory behind the technique is as follows: the equilibrium of the system will
be changed as the sap flux rate changes.
This changes the convection between the two sensors and changes the
difference in voltage between the two.
Practically, the system consists of a pair of sensors embedded in the
trunk of a tree. One probe is heated
while one is not. The heated probe is
embedded 10-15cm above the reference probe.
The reference (unheated) probe has two wires inside creating a
thermocouple. The two wires are made out
of copper and constantan. The heater
probe has four wires consisting of a thermocouple and a heater. The thermocouple is a copper-constantan pair,
while the heater is a constantan-constantan pair. The two thermocouples are joined together
through the constantan wire, and linked to the data logger through the copper
wires. The two heater wires are routed
to a 12v power supply where they will receive a constant 0.2 watts of
power. Now the circuit is complete, and
by measuring the difference in voltage between the two probes, one can see the
sap flux rate. The conversion formula is
. The length and diameter of the probe is
important in this empirical formula – any changes to the shape of the probe
will most likely change the formula.
However, Granier calculated that a change in the tree should not change
the formula that is applied. Also,
unlike the heat-pulse method, there is no real harm in varying the distance
between the heater and reference probe, as long as the reference probe is not
affected by the heat propagated by the heater probe. An optimal distance, as shown in literature,
is between 10-15 cm.
Determination
of
:
The
parameter
is defined as the maximum difference in
temperature between the two probes when the rate of sap flux is zero. In the past, scientists assumed that the
value of sap flux at night was zero, and simply calibrated the value of
each and every night. We now know through different studies that
the sap flux at night time is not
zero. This poses a problem – what is the
true value of
every night?
The answer to this problem is not incredibly simple, but it is possible
to estimate the true value of
at any given time. Determining nights when the sap flux rates
will be closest to zero can be done by looking at different variable such as
Vapor Pressure Deficit (VPD) and Photosynthetically Active Radiation
(PAR). When a baseline is determined,
scientists can then estimate the value of
through a linear regression. Granier proposed in his 1987 paper to
calculate the local maxima of
over a 10 day period, and then average the
values to calculate a value – this has been used with some limited
success. Linear regression is the
preferred method to calculate this.
Calculation
of whole-tree sap flow from a point-value:
Scaling
is a known issue with the Granier Thermal Dissipation Probe method. Measurements by the probes can only determine
the exact rate of flux at a specific location.
Scaling to the cross sectional level, the tree level, and the stand
level relies on several calculations.
The current method to determine this is to find the centroid of the sap
flux curve from the outer edge of the xylem to the sapwood, and then integrate
this over the entire area of the cross section of the tree. This can be further integrated to obtain the
complete water use of the tree.
Additionally, one can take the curve of the sap flow for different
depths all the way to the heartwood, and use calculus methods to rotate this
curve around the center axis of the tree to get a rotated solid that will have
the total calculated volume of water flow.
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