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An in-depth exploration of gravitational and electric potential energy, including their definitions, formulas, and applications. It covers topics such as newton's law of gravitation, field strength, gravitational potential energy, electric potential energy, and the concept of equipotential surfaces. The document also delves into the differences between point masses and charges, and the behavior of field lines and equipotential surfaces.
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โ we can think of fields as โforce fieldsโ present in space โ particles which are sensitive to the particular field feel the associated force when placed in the field
another mass - anything with mass
charge all charged particles โ both fields have a source (as opposed to magnetic field) โ fields take on a different interpretation in the quantum world
๐บ๐ 1 ๐ 2 ๐^2
magnitude (field strength)
๐บ๐ ๐^2 โ the large mass M is the SOURCE of gravitational field โ the field lines emanate from the source radially and are directed
โ if a small mass m planed near (subtlety!*), this mass feels an
๐บ๐๐ ๐ 2
1 ๐^2 infinitely far from the source ***** note that the large mass also feels a force with the same magnitude directed towards the small mass (Newtonโs 3rd Law)
โ consider the above scenario of the 2 masses M & m - they both feel an attractive force towards each other โ GPE is stored in the field = an energy shared between the 2 masses โ when we talk about the GPE of Earth, we use formula:
๐
2 things to note: โ the Earth is approximately flat very close to its surface (we donโt feel curvature in our daily lives) โ the field is approximately uniform meaning g = 9.8msยฏยฒ is approximately constant!
โ we only talk about the CHANGE in height and the CHANGE in GPE โ what do we
position form when they were infinitely apart Apart from the notion of infinity in space, we also neglect the change in the KE involved (very small constant speed) Recall: ๐ = ๐น๐ โ for a constant force F โ for a spatially varying force ( eg: gravitational force), the definition of work is:
the large mass M is:
โ ๐
๐บ๐๐ ๐'^
'
๐บ๐๐ ๐'^
โ ๐
๐บ๐๐ ๐ โ the gravitational potential energy stored in such a situation is:
โ๐บ๐๐ ๐ the work done by the external agent to bring in the mass m from infinity ***** force of gravity is attractive โ to separate the masses infinitely, we need to do work against the gravitational field:
๐บ๐๐ ๐ EG: to move away from the Earth surface, we need to put in energy ( eg: jumping)
mass in bringing a small point mass m from infinity to the point P โ always -ve โ at infinity = 0 ***** to calculate the gravitational potential due to multiple masses: simply add up the gravitational potential due to the individual masses
quantity (c.f. forces & field strengths are vector quantities)
๐บ๐ ๐ โ neglecting KE, work done to move from point A to B in a gravitational field is the change in GPE
๐ต
๐ด
*** PATH INDEPENDENT** quantity
๐
๐๐ ๐
๐
๐บ๐ ๐ โ the points with the same distance r from the source (point charge / mass) have
โ they lie on EQUIPOTENTIAL SURFACES
the same potential
๐๐๐
๐๐๐ ๐๐ (electric) (gravitational)
โ๐ โ๐ โ where โV = change ingravitaitonal potential between 2 points & โr = distance between the 2 points โ slope of a graph which plots the graviational potential against the distance from the mass
โ๐
๐บ๐ ๐^2
โ density of field lines is proportional to the field strength โ field lines & equipotential surfaces are perpendicular to each other โ can be understood in terms of work done: if we move a mass / charge along the
โ field lines (which indicate the direction of force) are perpendicular to the equipotential โ force is perpendicular to direction of motion - no work done EG: field lines - red / equipotential line - black 2 equal charges
2 unequal charges
โ the equipotential surfaces are therefore also straight lines, just perpendicular to the field of lines โ if the potential difference between the plates is V , then the electric field strength is
๐ ๐
โ assume a satellite with mass m orbiting around a large planet with mass M , such that M โซ m โ due to the mass difference, we can assume that the planet is not moving โ the forces are still equal and opposite! โ the accelerations are different due to the mass difference โ the total energy of this system (satellite + planet) is total energy = KE of satellite + PE shared by planet and satellite
๐
1
2
๐บ๐๐ ๐
mean disrance from the Sun
2
3 โ assuming that a planetโs orbit is circular (which is not exactly correct but is a good approximation in most cases), then the mean distance from the SUn is a constant ?> the radius โ F is the force of gravity on the planet + F is the centripetal force
2ฯ๐ ๐ ๐บ๐๐ ๐ ^2
๐๐ฃ 2
๐ 2ฯ๐ /๐[ ] 2 ๐
The possible paths of the satellite are related to the sign of ๐ธ๐! ๐ธ : bound - orbits the planets (circular / elliptical orbit) ๐
๐ธ๐ = 0 : free - shoots off to infinity & stops there (parabolic path) ๐ธ๐ > 0 : free, shoots off and keeps moving (hyperbolic path)
never return / stay in orbit around โ an object launched at / above its escape speed will not return to the planet due to gravity
๐
1
2
๐บ๐๐
***** where R is the radius of the planet
๐๐ ๐
2๐บ๐ ๐