Direct current injection is required. Can be difficult to get current into the ground so that little or no current reaches the zone of interest and hence its resistivity has little effect on the apparent resistivity measured by the resistivity meter. Labor intensive and time consuming- DRAWBACKS The resistivity method is generally more versatile than the terrain conductivity survey. There are fewer restrictions on electrode spacing The ability to employ a great number of electrode spacings in a sounding, for example, provides a much more comprehensive data base of measurements from which to infer the distribution of subsurface resistivity variation. ASSETS

By convention the direction of current flow is considered to be the direction in which positive charges move. Hence if you are following the progress of an electron in a wire, current flow is opposite the direction of the electron movement.

We also associate certain vector orientations with positive and negative charges. + The force or electric field intensity arrows emerge from the positive charges. Thus as you might have guessed our reference charge is positive (likes repel). - Conversely, by convention, the field lines associated with a negative charge point toward it.

+ - SourceSink Source Sink + - Direction of positive charge flow

Current i = current q = charge t = time Cross sectional area A Drift Velocity v A charge will move through a conductor at some average or root-mean-square velocty Charge q

The quantitative aspects of resistivity methods that we will deal with all stem directly from Ohm’s law. Because resistance is so dependant upon the geometry of the conductor, we deal with resistivity rather than resistance. The form of Ohm’s law we will use is where  is the resistivity.

Next let’s consider how apparent ground resistivity is measured given the typical setup of current and potential electrodes. To do this we have to compute the potential difference between the terminals of the voltmeter. But first consider the following diagram and ask what is the potential at point A? + - A d1d1 d2d2

Recall that the potential + -A d1d1 Medium with resistivity  In this diagram l is d 1. What is A? Consider first, what is the potential at A due to the positive current electrode located a distance d 1 away? - i.e. Ohm’s law.

+ - A d1d1 A will be the area over which the current i spreads out through the subsurface. That area will be the area of a hemisphere with radius d 1 or just 2  d 1 2. Thus -

Obviously the potential at point A will be the sum of two potentials - one with respect to the positive electrode, V + and the other with respect to the negative electrode, V -. By a similar line of reasoning - Note that we include the negative sign associated with the negative charge of the sink electrode.

Hence, the potential at point A associated with the contributions from both the positive and negative electrodes will be the sum of these two potentials, or just or just

Through a similar line of reasoning - A + - V B d1d1 d4d4 d2d2 d3d3 the potential difference measured by the voltmeter between potential electrodes located at points A and B on the surface will be V A - V B.

M + - V N d1d1 d4d4 d2d2 d3d3 AB

Given that The potential difference

and we generally just write the potential difference as or

This equation is easily solved for the resistivity The term Is referred to as a geometrical factor and the apparent resistivity  a is often written as

Where G is We can see that the geometrical factor contains information about the positioning of the current and potential electrodes in the survey - and as you have probably guessed there are several ways to arrange the potential and current electrodes.

One of the most commonly used electrode configurations is known as the Wenner array. In this setup a constant spacing is maintained between the electrodes in the array. That spacing is usually referred to as a. + - V d 1 =ad 4 =a d 2 =2a d 3 =2a a WENNER ARRAY

Determining the geometrical factor for the Wenner array

Thus computation of the apparent resistivity  a from the measured potential difference V is simply -

Consider the Schlumberger array.

From the preceding discussions and the above diagram it should be clear that d 1 = l-b d 2 = l+b d 3 = l+b d 4 = l-b Take a few minutes and determine the geometrical factor for the Schlumberger array.

Hint

and finally -

The third and fourth terms simplify in the same way so that you end up with or just

Note that when conducting a sounding using the Wenner array all 4 electrodes must be moved as the spacing is increased and maintained constant. The location of the center point of the array remains constant (despite appearances above).

Conducting a sounding using the Schlumberger array is less labor intensive. Only the outer two current electrodes need to be moved as the spacing is adjusted to achieve greater penetration depth. Periodically the potential electrodes have to be moved when the current electrodes are so far apart that potential differences are hard to measure - but much less often that for the Wenner survey

There are many types of arrays as shown at left. You should have general familiarity with the method of computing the geometrical factors at least for the Wenner and Schlumberger arrays. The resistivity lab you will be undertaking models Schlumberger data and many of the surveys conducted by Dr. Rauch and his students usually employ the Wenner array.

Consider the following problem. 1. Assume a homogeneous medium of resistivity 120 ohm-m. Using a Wenner electrode system with a 60m spacing, Assume a current of amperes. A. What is the measured potential difference? B. What will be the potential difference if we place the sink (negative-current electrode) at infinity? A + - B d1d1 d4d4 d2d2 d3d3 V

We know in general that For the Wenner array the geometrical factor G is 2  a and the general relationship of apparent resistivity to measured potential difference is In this problem we are interested in determining the potential difference when the subsurface resistivity distribution is given.

In part A) we solve for V as follows A + - V B d1d1 d4d4 d2d2 d3d3 and In part B) what happens to d 2 and d 4 ?

… d 2 and d 4 go to . We really can’t think of this as a simple Wenner array any longer. We have to return to the starting equation from which these “array-specific” generalizations are made. What happens when d 2 and d 4 go to  ? Part B)

A + - V B d1d1 d4d4 d2d2 d3d3 d 1 = 60 m and d 3 = 120 m. V is now only 0.1 volts. 

1B

Due Dates Hand in Terrain Conductivity paper summaries this Thursday Finish up Terrain Conductivity Lab and have in my mailbox next Wednesday Write up the answers to in-class problem 1 and hand in next period this Thursday Consider the current refraction problem (in-class problem 2). We will go over this problem in class this Thursday. Continue your readings from Chapter 5 of the text.