Gravitational and Electric Fields: Point Mass/Charge Fields
Introduction to Fields
- A field is a region of space where an object experiences a force.
- Gravitational fields exert forces on objects with mass.
- Electric fields exert forces on objects with electric charge.
- We consider fields created by point masses (gravity) or point charges (electricity).
KEY TAKEAWAY: Fields are models to explain forces acting at a distance.
Gravitational Fields
Direction of the Gravitational Field
- The direction of the gravitational field is the direction of the force that would be exerted on a test mass placed in the field.
- Gravitational force is always attractive.
- The gravitational field lines point radially inwards towards the point mass.
Shape of the Gravitational Field
- The gravitational field around a point mass is radial.
- Field lines are closest together near the point mass, indicating a stronger field.
- As distance from the point mass increases, the field lines spread out, indicating a weaker field.
Magnitude of the Gravitational Field
- The magnitude of the gravitational field, \(g\), at a distance \(r\) from a point mass \(M\) is given by Newton’s Law of Universal Gravitation:
\[
g = \frac{GM}{r^2}
\]
Where:
* \$G\$ is the gravitational constant (\$6.674 \times 10^{-11} \, Nm^2kg^{-2}\$)
* \$M\$ is the mass of the object creating the field
* \$r\$ is the distance from the center of the mass
- Inverse Square Law: The gravitational field strength is inversely proportional to the square of the distance from the point mass. This means doubling the distance reduces the field strength by a factor of four.
Gravitational Potential Energy Changes
- Gravitational potential energy (\(E_g\)) is the energy an object possesses due to its position in a gravitational field.
- For a point mass \(m\) in the gravitational field of another point mass \(M\), the change in gravitational potential energy (\(\Delta E_g\)) when moving from distance \(r_1\) to \(r_2\) is:
\[
\Delta E_g = -GMm \left(\frac{1}{r_2} - \frac{1}{r_1}\right)
\]
- Qualitative Analysis:
- As a mass moves away from another mass (against the gravitational field), its gravitational potential energy increases. Work is done on the mass by an external force.
- As a mass moves towards another mass (along the gravitational field), its gravitational potential energy decreases. Work is done by the gravitational field.
EXAM TIP: Always consider the direction of movement relative to the field when determining potential energy changes.
Electric Fields
Direction of the Electric Field
- The direction of the electric field is the direction of the force that would be exerted on a positive test charge placed in the field.
- Electric force can be attractive or repulsive, depending on the charges involved.
- Field lines point:
- Away from positive charges
- Towards negative charges
Shape of the Electric Field
- The electric field around a point charge is radial.
- Field lines are closest together near the point charge, indicating a stronger field.
- As distance from the point charge increases, the field lines spread out, indicating a weaker field.
- For multiple charges, the field shape becomes more complex, representing the vector sum of the individual fields.
Magnitude of the Electric Field
- The magnitude of the electric field, \(E\), at a distance \(r\) from a point charge \(Q\) is given by Coulomb’s Law:
\[
E = \frac{kQ}{r^2}
\]
Where:
* \$k\$ is Coulomb's constant (\$8.988 \times 10^9 \, Nm^2C^{-2}\$)
* \$Q\$ is the magnitude of the charge creating the field
* \$r\$ is the distance from the center of the charge
- Inverse Square Law: The electric field strength is inversely proportional to the square of the distance from the point charge.
Electric Potential Energy Changes
- Electric potential energy (\(E_e\)) is the energy a charge possesses due to its position in an electric field.
- For a charge \(q\) in the electric field of another charge \(Q\), the change in electric potential energy (\(\Delta E_e\)) when moving from distance \(r_1\) to \(r_2\) is:
\[
\Delta E_e = kQq \left(\frac{1}{r_2} - \frac{1}{r_1}\right)
\]
- Qualitative Analysis:
- If \(q\) and \(Q\) have the same sign (both positive or both negative):
- As \(q\) moves away from \(Q\) (against the electric field), its electric potential energy increases.
- As \(q\) moves towards \(Q\) (along the electric field), its electric potential energy decreases.
- If \(q\) and \(Q\) have opposite signs:
- As \(q\) moves away from \(Q\) (against the electric field), its electric potential energy decreases.
- As \(q\) moves towards \(Q\) (along the electric field), its electric potential energy increases.
COMMON MISTAKE: Forgetting to consider the signs of the charges when determining electric potential energy changes. Like charges repel, opposite charges attract.
Comparison of Gravitational and Electric Fields
| Feature |
Gravitational Field |
Electric Field |
| Source |
Mass |
Electric Charge |
| Force Type |
Attractive |
Attractive or Repulsive |
| Field Direction |
Inward towards mass |
Away from positive, towards negative |
| Potential Energy |
Always negative (relative to infinity) |
Positive or negative |
| Inverse Square Law |
Obeys |
Obeys |
STUDY HINT: Create a table summarizing the similarities and differences between gravitational and electric fields.
- Uniform Field: The field strength and direction are constant throughout the region of space. Electric fields between charged parallel plates are a good approximation of a uniform field. Gravitational field near earth’s surface is often treated as uniform.
- Non-Uniform Field: The field strength and/or direction vary with position. Radial fields around point masses and point charges are non-uniform.
VCAA FOCUS: VCAA often requires calculations involving both uniform and non-uniform fields. Make sure you understand when and how to apply the relevant formulas.
Applications
- Gravitational Fields: Satellite motion, planetary orbits, projectile motion.
- Electric Fields: Particle accelerators, cathode ray tubes (CRTs), inkjet printers.
APPLICATION: Particle accelerators use electric fields to accelerate charged particles to very high speeds for research purposes.