Charged Particle in an Electric Field

 
 
This is part of the HSC Physics course under the topic Charged Particles, Conductors and Electric and Magnetic Fields.

HSC Physics Syllabus

  • investigate and quantitatively derive and analyse the interaction between charged particles and uniform electric fields, including: (ACSPH083)
– electric field between parallel charged plates `E=V/d`
– acceleration of charged particles by the electric field `F_(\text{net})=ma, F=qE`
  • model qualitatively and quantitatively the trajectories of charged particles in electric fields and compare them with the trajectories of projectiles in a gravitational field

Charges in Uniform Electric Fields

    This video analyses the interaction between charged particles and uniform electric fields, deriving the relevant syllabus equations. The video also qualitatively and quantitatively compares the trajectory of charged particles in electric fields to that of projectiles in gravitational fields.

     

    Electric Field Strength

    Students are advised to revise knowledge from Introduction to Electric Fields.

    When two parallel charged plates are connected to a potential difference, they produce a uniform electric field with strength:

     

    `E=V/d`

     

    where,

    • E is the electric field strength (V m-1 or N C-1)
    • V is the potential difference or voltage (V) between parallel charged plates
    • d is the perpendicular distance between parallel charged plates (m). 

       

      The direction of the electric field always goes from the positively charged plate to the negatively charged plate, as shown below.

       
      In the electric field above, the electric field strength is given by:

       

      $$E = \frac{10}{5} = 2 \, V m^{-1} \text{ downwards}$$

       

      Force due to electric field

       

      When a charged particle is placed in a uniform electric field, it experiences an electric force that is proportional to the magnitude of the charge and the strength of the electric field. This force acts in the direction of the electric field if the charge is positive, or opposite to the field if the charge is negative. 

        `F_E=qE`
         

        where,

        • F is the force (N)
        • q is the charge of the particle (C)
        • E is the electric field strength (V m-1 or N C-1) 

        The electric field strength can therefore be also expressed in the form:

         

        `E=F/q`

        Now, since:

        `E=V/d`

        then,

        `F/q=V/d` 

         

        In a uniform electric field, this force is constant, leading to a uniform acceleration of the charge in the direction of the force according to Newton's second law (`F = ma`).

            Parabolic motion of charges in electric fields

           

          If a charge moves in an electric field with velocity (`v_{_|_}`) that is perpendicular to the electric field lines, it undergoes parabolic motion. This is because the uniform acceleration due to the field only affects the charge's velocity component (`v_{||}`) that is parallel to the field; the velocity component that is perpendicular to the electric field remains constant (unaffected).

          This means `v_{||}` will increase due to the electric force while `v_{_|_}` remains constant during the charge's motion in an electric field. 

          Electric Fields vs Gravitational Fields

          This parabolic trajectory is similar to that of a mass in gravitational fields. The vertical component of velocity which is parallel to the direction of gravity is affected, whereas the horizontal component of velocity (perpendicular to gravity) remains constant (unaffected).

          Feature

          Motion in Electric Field

          Motion in Gravitational Field

          Shape of trajectory

          Parabolic (for uniform electric fields)

          Parabolic

          Is constant force experienced by projectile?

          Yes, in uniform electric fields.

          Yes, in uniform gravitational fields.

          Can be analysed by vector resolution into horizontal and vertical components?

          Yes

          Yes

          Horizontal component of motion

          Constant

          Constant

          What undergoes motion?

          Charged particles

          Any type of matter

          Magnitude of acceleration

          Typically much larger due to projectiles being of very small mass

          Typically much smaller, due to projectiles being of larger mass.

          Magnitude of forces

          Depends on different parameters than gravitational force.

           

          F = qE (force per unit charge)

           

          Depends on different parameters than electric force

           

           F = mg (force per unit mass)

           

          Direction of force

          Depends on nature of charge of projectile:

          • positive particle attracted to negative plate, repelled by positive plate.
          • negative particle attracted to positive plate, repelled by negative plate

          Always attractive towards centre of mass of source of gravitational attraction.

           

          Why is Gravity not Considered for Motion of Charged Particles?

          Charged particles experience negligible amounts of gravitational force. For example, an electron on the surface of Earth has gravitational force of magnitude:

            `F_g=(GMm)/d^2`
             
            `F_g=((6.67xx10^-11)(6.0xx10^24)(9.109xx10^-31))/(6.371xx10^6)^2`
             
            `F=9.0xx10^-30` N towards the centre of Earth
             
            Compared with typical electric fields, the contribution from electric force is much more significant than gravitational force.

            Calculation Example

            A proton enters an electric field produced by a pair of parallel metal plates with potential difference of 150 V and separated by a distance of 2.0 m apart.

            Calculate the force and acceleration due to the electric field for the proton.

             

            Next section: Work Done in Electric Fields

             

            BACK TO MODULE 6: ELECTROMAGNETISM