Skip to main content

Soil Resistivity

  • Chapter
  • First Online:
Power Systems Grounding

Part of the book series: Power Systems ((POWSYS))

Abstract

Soil is defined as the top layer of the earth’s crust. It covers most of the land on the earth. It is made up of minerals (rock, sand, clay and silt), air, water and organic materials. The organic materials are formed from the dead plants and animals. There are many properties of soil. Although varying soil properties of different kinds can be observed small area, the electric power utility companies are interested in the electrical properties of the soil, especially the specific resistance or resistivity. Soil resistivity is one of the important factors which plays a vital role in the design and analysis of ground resistance. The dry soil with small particles acts as nonconductor of current. Sands, rocks and loams are some examples of nonconductors. The resistivity of soils drops down when the water content in the soil is more. In this chapter, different types and characteristics of soil, and size of earth electrode and different ground resistance measurement methods will be discussed.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

eBook
USD 16.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 99.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 109.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

References

  1. J.N. Cernica, Geotechnical Engineering: Soil Mechanics. (Wiley, USA, 1995)

    Google Scholar 

  2. B.M. Das, Principles of Geotechnical Engineering. (PWS-KENT Publishing Company, USA, 1985)

    Google Scholar 

  3. D.K. Cheng, Fundamentals of Engineering Electromagnetics, 1st edn. (Prentice-Hall Inc., Upper Saddle River, New Jersey, USA, 1993)

    Google Scholar 

  4. M.A. Salam, Electromagnetic Field Theories for Engineering, 1st edn. (Springer Publishers, 2014), pp. 1–311

    Google Scholar 

  5. P.P. Silvester, R.L. Ferrari, Finite Elements for Electrical Engineers, 3rd edn. (Cambridge University Press, UK, 1996)

    Google Scholar 

  6. C.R. Paul, S.A. Nasar, Introduction to Electromagnetic Fields, 1st edn. (McGraw-Hill Inc., USA, 1982)

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Md. Abdus Salam .

Exercise Problems

Exercise Problems

  1. 5.1

    The expression of electric potential in Cartesian coordinates is \(V(x,y,z) = x^{2} y - z^{2} + 8\). Determine the (i) numerical value of the voltage at point \(P(1, - 1,2)\), (ii) electric field, and (iii) verify the Laplace equation.

  2. 5.2

    The electric potential in Cartesian coordinates is given by \(V(x,y,z) = {\text{e}}^{x} - {\text{e}}^{ - y} + z^{2}\). Determine the (i) numerical value of the voltage at point \(P(1,1, - 2)\), (ii) electric field at the point \(P(1,1, - 2)\), and (iii) verify the Laplace equation.

  3. 5.3

    The expression of electric potential in cylindrical coordinates is given as \(V(\rho ,\phi ,z) = \rho^{2} z\cos \phi\). Determine the (i) numerical value of the voltage at point \(P(\rho = - 1,\phi = 45^{ \circ } ,z = 5)\), (ii) electric field at the point \(P(\rho = - 1,\phi = 45^{ \circ } ,z = 5)\), and (iii) verify the Laplace equation.

  4. 5.4

    The electric potential in spherical coordinates is given by \(V(r,\theta ,\phi ) = 5r^{2} \sin \theta \cos \phi\). Determine the (i) numerical value of the voltage at point \(P(r = 1,\theta = 40^{ \circ } ,\phi = 120^{ \circ } )\), (ii) electric field at the point \(P(r = 1,\theta = 40^{ \circ } ,\phi = 120^{ \circ } )\), and (iii) verify the Laplace equation.

  5. 5.5

    In Cartesian coordinates, the volume charge density is \(\rho_{v} = - 1.6 \times 10^{ - 11} \varepsilon_{0} x\;{\text{C/m}}^{3}\) in the free space. Consider \(V = 0\) at \(x = 0\) and \(V = 4\,{\text{V}}\) at \(x = 2\;{\text{m}}\). Determine the electric potential and field at \(x = 5\;{\text{m}} .\)

  6. 5.6

    The charge density in cylindrical coordinates is \(\rho_{v} = \frac{25}{\rho }\,{\text{pC/m}}^{ 3}\). Consider \(V = 0\) at \(\rho = 2\,{\text{m}}\) and \(V = 120\,{\text{V}}\) at \(\rho = 5\,{\text{m}}\). Calculate the electric potential and field at \(\rho = 6\,{\text{m}}\).

  7. 5.7

    Two concentric spherical shells with radius of \(r = 1\,{\text{m}}\) and \(r = 2\,{\text{m}}\) contain the potentials of \(V = 0\) and \(V = 80\,{\text{V}}\) respectively. Find the potential and electric field.

  8. 5.8

    Determine the potential of a rectangular object of infinite length. Consider \(a = b = 1\,{\text{m}}\), \(V_{0} = 50\,{\text{V}}\), \(x = \frac{3a}{2}\) and \(y = \frac{b}{2}\).

Rights and permissions

Reprints and permissions

Copyright information

© 2016 Springer Science+Business Media Singapore

About this chapter

Cite this chapter

Salam, M.A., Rahman, Q.M. (2016). Soil Resistivity. In: Power Systems Grounding. Power Systems. Springer, Singapore. https://doi.org/10.1007/978-981-10-0446-9_5

Download citation

  • DOI: https://doi.org/10.1007/978-981-10-0446-9_5

  • Published:

  • Publisher Name: Springer, Singapore

  • Print ISBN: 978-981-10-0444-5

  • Online ISBN: 978-981-10-0446-9

  • eBook Packages: EnergyEnergy (R0)

Publish with us

Policies and ethics