Ch – 26 Electric Field. Electric Field Model One or more charges (source charges) alter the space...
Transcript of Ch – 26 Electric Field. Electric Field Model One or more charges (source charges) alter the space...
Ch – 26 Electric Field
Electric Field Model
• One or more charges (source charges) alter the space around them by creating an electric field, E.
• A separate charge (test charge or probe) experiences a force F, exerted by the field.
• F = qE
Electric Field of a Point Charge
The unit vector points outward from the source charge
If q is negative the vector is reversed and points inward, toward the source charge
Electric Field Simulation
Electric field of a dipole
• Two equal and opposite charges small distance apart
• Zero net charge but it causes an E field
• Dipole moment:
p = qs, pointing from negative to positive
Electric Field of a Dipole
E Field for an Infinite line of Charge
Picturing the Electric Field
Electric Field of a Dipole
E Field for an Infinite line of Charge
Electric Field of a Ring of Charge
(Ering)z = [1/(4πε0)] [zQ/(z2+R2)3/2]
Electric Field of Charged Disk
Limit as R ∞
Note that this value of E does not depend on the distance from the charged plane (z), only on the surface charge density
Electric field strength of an infinitely charged plane is independent of
distance from the charge
Parallel Plate Capacitor
A parallel plate capacitor provides a uniform electric field.
Motion of a charged particle in a uniform electric field
• a = F/m = qE/m = constant
• direction of a parallel to E
• charged particle will accelerate/decelerate in the direction of E
• projectile motion, if v0 is not parallel to E
Motion in a Nonuniform Field
• circular motion of a charged particle around a point charge, charged sphere or wire
|q|E = mv2/r
Simulation labSimulation lab
Superposition problem
Earth’s internal structure
Figure 1.13
Plate tectonics: the new paradigm
Plate boundaries • Types of plate boundaries
• Divergent plate boundaries (constructive margins)
• Two plates move apart• Mantle material upwells to create new
seafloor • Ocean ridges and seafloor spreading
• Oceanic ridges develop along well-developed boundaries
• Along ridges, seafloor spreading creates new seafloor
Figure 15.10a
Figure 15.12
Plate tectonics: the new paradigm
Plate boundaries • Types of plate boundaries
• Convergent plate boundaries (destructive margins)
• Oceanic-continental convergence • Denser oceanic slab sinks into the
asthenosphere • Pockets of magma develop and rise • Continental volcanic arcs form• Examples include the Andes,
Cascades, and the Sierra Nevadan system
Figure 15.14a
Plate tectonics: the new paradigm
Plate boundaries • Types of plate boundaries
• Convergent plate boundaries (destructive margins)
• Oceanic-oceanic convergence • Two oceanic slabs converge and one
descends beneath the other • Often forms volcanoes on the ocean
floor • Volcanic island arcs forms as
volcanoes emerge from the sea • Examples include the Aleutian,
Mariana, and Tonga islands
Figure 15.14b
Plate tectonics: the new paradigm
Plate boundaries • Types of plate boundaries
• Convergent plate boundaries (destructive margins)
• Continental-continental convergence • When subducting plates contain
continental material, two continents collide
• Can produce new mountain ranges such as the Himalayas
Figure 15.14c
Plate tectonics: the new paradigm
Plate boundaries • Types of plate boundaries
• Transform fault boundaries • Plates slide past one another
• No new crust is created or destroyed • Transform faults
• Most join two segments of a mid-ocean ridge
• Aid the movement of oceanic crustal material
Figure 15.16