PPT-Isostasy: static equilibrium in pressure of a fluid at some

The height of the top of the block iceberg continental crust would be h m h c Response of the crust to a addition of a load sediment accumulating or a large volcano the crust floats downward to reestablish isostatic equilibrium and the elevation of the crust changes less that the thickness of the material added . Universal gravitational constant G667 x 10 11 Nm kg 2 2 EPS 122 Lecture 14 Gravity and isostasy Theory of gravity Gravitational potential Definition The gravitational potential V due to a point mass m at a distance r from m is the work done by th Chapter 9. Isostasy: The Concept of Floating Blocks. Isostasy = the concept that large topographic features effectively float on the asthenosphere. Iso. = same – stasis = standstill. Involves a state of constant pressure at any point. Examples. Lecture . 20: . Static Equilibrium. Conditions for static equilibrium.  . No linear acceleration:.  . No . angular . acceleration:. Two-dimensional problems.  .  . All forces act in one plane, the . Too much of a good thing. Intravenous fluid boluses are used liberally in medicine to achieve a variety of goals.. In critical care we use them most often to improve cardiovascular parameters and replace known losses. and Uncertainty Assessment Methodology. H. . Elshiekh. , H. Yoon, M. . Muste. , F. Stern. Acknowledgements: S. . Ghosh. , M. Marquardt, S. Cook. Table of Contents. What is EFD. EFD philosophy. EFD Process. 2. Objectives. . Students must be able to. Utilize theory of dry friction. Describe . theory of dry friction. . Describe . physical meanings. of frictional effects. Describe and differentiate between . Examples. Lecture . 22: . Static Equilibrium. Conditions for static equilibrium.  . No linear acceleration:.  . No . angular . acceleration:. Two-dimensional problems.  .  . All forces act in one plane, the . Back in Time: General gas law . PV=. nRT. <=> P= . nRT. /V. Pressure is directly proportional to number of moles and temperature, and is inversely proportional to the volume occupied by the gas . © 2016 Pearson Education, Inc.. Goals for Chapter 13. To study density and pressure in a fluid . with. Pascal’s. . Law. To apply . Archimedes principle . of buoyancy.. © 2016 Pearson Education, Inc.. E-mail: . benzene4president@gmail.com. Web-site: http://clas.sa.ucsb.edu/staff/terri/. Chemical Equilibrium – Ch. 6. 1. Consider the following reaction: . N. 2. (g) 3 . H. 2. (g) . ⇌ . Department of Chemistry. University of Utah. Saturday, September 19, 2015. What is equilibrium?. Equilibrium is a . state of balance between opposing forces or actions that is either . static. (as in a body acted on by forces whose resultant is zero) or . . Students must be able to. Utilize theory of dry friction. Describe . theory of dry friction. . Describe . physical meanings. of frictional effects. Describe and differentiate between . static and kinetic coefficients of friction. Problems of Gas phase equilibria 1) Consider the following reaction:CO(g) Cl2(g) COCl2(g)The initial partial pressures are (CO) 2 atm and (Cl) 2 atm. When the reaction reaches equilibrium t ’ level is the mid-axillary line. (do NOT use the . phlebostatic. axis or the symphysis pubis . as these underestimate the true pressure. ). IV fluid in pressure bag at 300 mmHg. 60 mL Syringe. 50.