Pickett's Charge

(noun)

Pickett's Charge was an infantry assault ordered by Confederate General Robert E. Lee against Major General George G. Meade's Union positions on Cemetery Ridge on July 3, 1863, during the last day of the Battle of Gettysburg.

Related Terms

  • Gettysburg Address

Examples of Pickett's Charge in the following topics:

  • The Battle of Gettysburg

    • The main event was a dramatic infantry assault by 12,500 Confederates against the center of the Union line on Cemetery Ridge, known as Pickett's Charge.
    • The charge was repulsed by Union rifle and artillery fire at great losses to the Confederate army.
  • Electric Field from a Point Charge

    • The electric field of a point charge is, like any electric field, a vector field that represents the effect that the point charge has on other charges around it.
    • If the charge is positive, as shown above, the electric field will be pointing in a positive radial direction from the charge q (away from the charge).
    • This means that because the charges are both positive and will repel one another, the force on the test charge points away from the original charge.
    • If the test charge were negative, the force felt on that charge would be:
    • The electric field of a positively charged particle points radially away from the charge.
  • Static Electricity, Charge, and the Conservation of Charge

    • In both instances, charged particles will experience a force when in the presence of other charged matter.
    • The SI unit for charge is the Coulomb (C), which is approximately equal to $6.24\times 10^{18}$ elementary charges.
    • (An elementary charge is the magnitude of charge of a proton or electron. )
    • In physics, charge conservation is the principle that electric charge can neither be created nor destroyed.
    • The net quantity of electric charge, the amount of positive charge minus the amount of negative charge in the universe, is always conserved.
  • Stress and Strain

    • The electric field of a point charge is, like any electric field, a vector field that represents the effect that the point charge has on other charges around it.
    • This means that because the charges are both positive and will repel one another, the force on the test charge points away from the original charge.
    • If the test charge were negative, the force felt on that charge would be
    • This makes sense because opposite charges attract and the force on the test charge will tend to push it toward the original positive charge creating the field.
    • The electric field of a positively charged particle points radially away from the charge.
  • Conductors and Fields in Static Equilibrium

    • In the presence of charge or an electric field, the charges in a conductor will redistribute until they reach static equilibrium.
    • Conductors are materials in which charges can move freely.
    • If conductors are exposed to charge or an electric field, their internal charges will rearrange rapidly.
    • Negative charges in the conductor will align themselves towards the positive end of the electric field, leaving positive charges at the negative end of the field.
    • Describe behavior of charges in a conductor in the presence of charge or an electric field and under static equilibrium
  • Induced Charge

    • Electrostatic induction is the redistribution of charges within an object that occurs as a reaction to the presence of a nearby charge.
    • Electrostatic induction is the redistribution of charge within an object, which occurs as a reaction to a nearby charge.
    • As such, it has no net charge.
    • In such an event, the electrons in the neutral object move (the protons are relatively inert) according to the charge of the nearby charged object (inductor).
    • Total charge is conserved, and that of the inductor decreases as it transfers charge to its subject.
  • Equipotential Lines

    • Since they are located radially around a charged body, they are perpendicular to electric field lines, which extend radially from the center of a charged body.
    • For a single, isolated point charge, the formula for potential (V) is functionally dependent upon charge (Q) and inversely dependent upon radial distance from the charge (r):
    • Therefore, equipotential lines for a single point charge are circular, with the point charge at the center .
    • When multiple, discrete charges interact, their fields overlap.
    • At a point between the charges, a test charge may "feel" the effects of both charges.
  • Charge Separation

    • Charge separation, often referred to as static electricity, is the building of space between particles of opposite charges.
    • All matter is composed of atoms made up of negatively-charged electrons and positively-charged protons.
    • Thus, the opposite charges attract.
    • Charge separation can be created not only by friction, but by pressure, heat, and other charges.
    • Charge separation occurs often in the natural world.
  • Electric Field Lines: Multiple Charges

    • But what if another charge is introduced?
    • When modeling the electric fields of multiple charges, it's important to take into consideration the sign and magnitude of each charge.
    • This means that if charges q1 (with a +1 value) q2 (+2 charge) and q3 (+3 charge) are in the same field, one can connect 4, 8, and 12 field lines, respectively, to the charges.
    • Field lines should always point away from positive charges and towards negative charge.
    • Calculate the resultant force of the multiple electric charges on a test charge
  • Electric Fields and Conductors

    • Electric fields are found around electric charges and help determine the direction and magnitude of force the charge exerts on a nearby charged particle.
    • Therefore, they can facilitate the flow of charge, or current.
    • There is no electric field inside a charged conductor.
    • A charged conductor at electrostatic equilibrium will contain charges only on its outer surface and will have no net electric field within itself.
    • This is because all the charges in such a conductor will symmetrically oppose other charges within the conductor, causing the net result to sum to 0.
Subjects
  • Accounting
  • Algebra
  • Art History
  • Biology
  • Business
  • Calculus
  • Chemistry
  • Communications
  • Economics
  • Finance
  • Management
  • Marketing
  • Microbiology
  • Physics
  • Physiology
  • Political Science
  • Psychology
  • Sociology
  • Statistics
  • U.S. History
  • World History
  • Writing

Except where noted, content and user contributions on this site are licensed under CC BY-SA 4.0 with attribution required.