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An electric dipole consists of two equal but opposite charges, separated by a specific distance. The electric dipole moment \( \mathbf{p} \) quantifies the strength and direction of this dipole. It points from the negative charge to the positive charge which means from \( q_1 \) to \( q_2 \). The formula for calculating the electric dipole moment is:

• \( p = q \times d \)

where \( q \) is the magnitude of one charge, and \( d \) is the distance between the charges. In the current scenario, this would be: \( p = (4.5 \times 10^{-9} \text{ C}) \times (3.1 \times 10^{-3} \text{ m}) \).
The units for dipole moment are Coulomb-meters (C·m), and this physical quantity is critical in understanding the interaction of dipoles in electric fields. It shows how the separation of charge can create an electric field. A larger dipole moment means the charges have a potentially stronger influence in an electric field.

A uniform electric field has the same strength and direction at every point in space. This simplifies analysis as the force experienced by charges in such a field is consistent across different positions.
The uniform electric field can interact with an electric dipole, leading to torque on the dipole. A real-life analogy might be turning a compass in a magnetic field, where the field 'wants' to align the compass needle in its direction.
In our problem, this uniform electric field applies a torque to the dipole when it's not aligned with the field. The magnitude of the field itself was to be determined from the known torque, allowing us to gauge how strong this field was at exerting influence on the dipole.

Torque is a measure of the rotational force on an object, in this case, the dipole. When placed in a uniform electric field, a dipole experiences torque because of the forces acting on the two opposite charges.
Torque \( \tau \) is calculated with the formula:

• \( \tau = pE \sin \theta \)

Here, \( \tau \) is the torque, \( p \) is the electric dipole moment, \( E \) is the electric field strength, and \( \theta \) is the angle between the dipole moment and the electric field. The sine function collaborates the angle's proportion in leading to the rotational effect thus, \( \sin(36.9^{\circ}) \approx 0.6 \).
In our example, the angle wasn’t zero, meaning the dipole wasn’t aligned with the field, resulting in a measurable torque of \( 7.2 \times 10^{-9} \text{ N·m} \).

Electrostatics studies charges at rest, typically involving electric forces, fields, and potentials caused by stationary charges. It focuses on understanding the forces and reactions between electrically charged objects under various conditions.
This domain helps us understand the behavior of electric dipoles within electric fields. An electric dipole, such as our example, perfectly ties with electrostatic basics since it comprises two static point charges, one positive and one negative.
Analyzing how such dipoles interact with electric fields under the framework of electrostatics can unravel fundamental electromagnetic phenomena that are intrinsically critical in technology, from capacitors to the molecular polarity in chemistry.

Physics problem solving can be navigated effectively using a systematic approach:

• Understand the problem: Clarify what’s known and what’s being asked.
• Use relevant equations: Identify formulas that connect known quantities to unknowns.
• Substitute values: Plug known values into formulas to find unknowns.
• Check the units: Ensure your computational steps maintain unit consistency.
• Verify solutions: Consider if the computational results logically fit the physical scenario.

In our scenario, determining the electric dipole moment and the field required correlating provided values of force and charge to find the electric field strength. By incorporating principles from electrostatics and understanding the interaction of forces, solutions are more intuitive and physics problems become less of a mystery.