Geophysics Lecture 14: Rotation Poles and Tectonic Plate Motion, Study notes of Physics

An overview of plate motions on a spherical earth, describing how they can be uniquely and completely described by rotation about an axis passing through the earth's center. The concept of euler poles or instantaneous rotation poles, the relative motion of plates, and the application of the equation for speed and angular velocity about a rotation pole. Students are encouraged to study problems related to spherical geometry and rotation poles for well-known plate boundaries.

Typology: Study notes

2010/2011

Uploaded on 09/10/2011

aisha-92
aisha-92 🇬🇧

4.5

(2)

20 documents

1 / 2

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
PX266 Geophysics (2010/11)
Lecture 14 Handout Rotation Poles and Tectonic Plate Motion
Dr. Gavin Bell
Plate motions on a ‘flat Earth’ are easily described by vector addition of relative
velocities.
On a spherical Earth, the plates are not planar, but segments of the spherical surface.
Since they are constrained to stay on the surface, their (instantaneous) motion can be
uniquely and completely described by rotation about an axis passing through the
centre of the Earth. Formally, this is a consequence of Euler’s ‘fixed point theorem’
for motion of rigid bodies, but it should be fairly obvious from intuition that any
possible motion of a spherical cap segment can be thus expressed.
The intersections of the rotation axis with the Earth’s surface are the Euler poles or
instantaneous rotation poles, one positive and one negative. The sign convention is
that clockwise rotation looking out from the centre of the Earth corresponds to the
positive rotation pole (but don’t worry too much about getting this wrong in an exam).
The relative motion of any two plates can be described by a positive rotation pole
(a latitude and longitude) together with an angular velocity.
This description gives the relative motion at any point on the boundary between the
two plates. The (vector) velocity will, in general, be different at different points on the
boundary. The local relative velocity vector together with the local plate boundary
direction tell you the local nature of the plate boundary (normal constructive, oblique
constructive, conservative, etc.), which changes along the boundary.
Speed vabout a rotation pole at a point
an angular distance away from the
pole. The vector version for velocity
xv
will not be used in exams but
you should be aware of it (see Q. 20)
sin
E
Rv
You should know this equation and understand its application.
Note that ‘instantaneous’ is relative to the geological timescale a pole may describe
the motion of a plate over many thousands of years, though in general the relative
plate motions have changed over geological history and the rotation poles apply to
present-day motion only.
pf2

Partial preview of the text

Download Geophysics Lecture 14: Rotation Poles and Tectonic Plate Motion and more Study notes Physics in PDF only on Docsity!

PX266 Geophysics (2010/11)

Lecture 14 Handout – Rotation Poles and Tectonic Plate Motion

Dr. Gavin Bell Plate motions on a ‘flat Earth’ are easily described by vector addition of relative velocities. On a spherical Earth, the plates are not planar, but segments of the spherical surface. Since they are constrained to stay on the surface, their (instantaneous) motion can be uniquely and completely described by rotation about an axis passing through the centre of the Earth. Formally, this is a consequence of Euler’s ‘fixed point theorem’ for motion of rigid bodies, but it should be fairly obvious from intuition that any possible motion of a spherical cap segment can be thus expressed. The intersections of the rotation axis with the Earth’s surface are the Euler poles or instantaneous rotation poles , one positive and one negative. The sign convention is that clockwise rotation looking out from the centre of the Earth corresponds to the positive rotation pole (but don’t worry too much about getting this wrong in an exam). The relative motion of any two plates can be described by a positive rotation pole (a latitude and longitude) together with an angular velocity. This description gives the relative motion at any point on the boundary between the two plates. The (vector) velocity will, in general, be different at different points on the boundary. The local relative velocity vector together with the local plate boundary direction tell you the local nature of the plate boundary (normal constructive, oblique constructive, conservative, etc.), which changes along the boundary. Speed v about a rotation pole at a point an angular distance  away from the pole. The vector version for velocity v x

   will not be used in exams but you should be aware of it (see Q. 20)

v   RE sin 

You should know this equation and understand its application. Note that ‘instantaneous’ is relative to the geological timescale – a pole may describe the motion of a plate over many thousands of years, though in general the relative plate motions have changed over geological history and the rotation poles apply to present-day motion only.

Figure (above) – schematic of a pole and plate boundary. Further study Problems 18, 19 and 20. Q18/19 are important – you need to get the hang of the spherical geometry involved in plate motions. Q20 is optional and deals with the full vector approach (which we would not use in a 30 min. exam question). See the web site (Extra Material) for suggested exercises to get your head around rotation poles for a few well known plate boundaries. Note – simplified plate boundaries will normally be used in exam questions.