Gravitational Potential Energy
How much GPE?
How much GPE?
GPE = mgh?
How much GPE?
GPE = mgh?
How much GPE?
GPE = mgh?
How much GPE?
GPE = mgh?
We do know that the GPE must be
decreasing. But where is the GPE zero?
How much GPE?
GPE = mgh?
We do a little physicists trick. We take the GPE at infinity to be zero! That
means that it has negative GPE at distance closer than
infinity!
Gravitational potential energy
Gravitational potential energy at a point is defined as the work done to move a mass from infinity to that point.
Gravitational potential energy
Gravitational potential energy at a point is defined as the work done to move a mass from infinity to that point.
M
m
I’ve come from infinity!
R
Gravitational potential energy
Gravitational potential energy at a point is defined as the work done to move a mass from infinity to that point.
M
m
I’ve come from infinity!
R
Work done = force x distance
The force however is changing as the mass gets closer
Gravitational potential energy
M
m
I’ve come from infinity!
R
W =
R
Fdr
R
GMmdr
r2
= = [ ]GMm
r
R
=GMm
R
- -
Gravitational potential energy
Gravitational potential energy at a point is defined as the work done to move a mass from infinity to that point.
Ep = -GMm
r
Ep is always negative
Gravitational Potential
It follows that the Gravitational potential at a point is the work done per unit mass on a small point mass moving from infinity to that point. It is given by
V = -GM
rNote the difference between gravitational potential energy (J) and Gravitational potential (J.kg-1)
Ep = mV
Moving masses in potentials
If a mass is moved from a position with potential V1 to a position with potential V2, work = m(V2 – V1) = mΔV
V1
V2
(independent of path)
Equipotential surfaces/lines
Equipotential surfaces/lines
Field and equipotentials
• Equipotentials are always perpendicular to field lines. Diagrams of equipotential lines give us information about the gravitational field in much the same way as contour
maps give us information about geographical heights.
Field strength = potential gradient
In fact it can be shown from calculus that the gravitational field is given by the potential gradient (the closer the equipotential lines are together, the stronger the field)
g = -dVdr
Let’s stop and read!
Pages 127 to 130Pages142 to 151
Escape speed
Imagine throwing a ball into the air
Escape speed
It falls to the ground
Escape speed
What happens if you throw harder?
Escape speed
It goes higher and takes longer to return.
Escape speed
It goes higher and takes longer to return.
Escape speed
The kinetic energy of the ball changes to gravitational potential energy as the ball rises. This in turn turns back into kinetic energy as the ball falls again.
Escape speed
How fast would you have to throw the ball so that it doesn’t come back? (i.e. goes to “infinity” or escapes the gravitational field of the earth)
Escape speed
At “infinity”, its gravitational energy is given by Ep = -GMm/r
= zero when r is infinite
Escape speed
Energy conservation tells us that it must therefore have zero energy to start with if it is to escape the earth’s gravity.
i.e. KE + GPE = 0
Escape speed
i.e. KE + GPE = 0
½mv2 + -GMem/Re = 0
(where Re is the radius of the earth)
½mv2 = GMem/Re
v = √2GMe/Re
Escape speed
v = √2GM/Re
v = √(2 x 6.67 x 10-11 x 5.98 x 1024)/6.38 x 106
v = 12000 m.s-1
I can’t throw that fast!
In reality the escape
velocity of the earth is bigger
than this. WHY?
Let’s try some questions!
Hold on!
Isn’t electricity similiar?
Gravitational Potential
The Gravitational potential at a point is the work done per unit mass on a small point mass moving from infinity to that point. It is given by
V = -GM
rNote the difference between gravitational potential energy (J) and Gravitational potential (J.kg-1)
Ep = mV
Electrical Potential
The Electrical potential at a point is the work done per unit charge on a small positive test charge moving from infinity to that point. It is given by
V = W
qNote the difference between electrical potential energy (J) and Electrical potential (J.C-1)
Uel = qV
Scalar quantity
Moving charges in potentials
If a charge is moved from a position with potential V1 to a position with potential V2, work = q(V2 – V1) = qΔV
V1
V2
(independent of path)
Gravitational potential energy
Gravitational potential energy at a point is defined as the work done to move a mass from infinity to that point.
Ep = -GMm
r
Ep is always negative
Electrical potential energy
Electrical potential energy at a point is defined as the work done to move a positive charge from infinity to that point.
Uel = kQq
r
Equipotential surfaces/lines
Ep = -GMmr
Equipotential surfaces/lines
Field and equipotentials
• Equipotentials are always perpendicular to field lines. Diagrams of equipotential lines give us information about the gravitational field in much the same way as contour
maps give us information about geographical heights.
Field strength = potential gradient
In fact it can be shown from calculus that the gravitational field is given by the potential gradient (the closer the equipotential lines are together, the stronger the field)
E = dVdr
From “Physics for the IB Diploma”K.A.Tsokos (Cambridge University Press)
Gravitation ElectricityActs on Mass (always +?) Charge (+ or -)
Force F = GM1M2/r2
Attractive only, infinite range
F = kQ1Q2/r2
Attractive or repulsive, infinite range
Relative strength 1 1042
Field g = GM/r2 E = kQ/r2
Potential V = -GM/r V = kQ/r
Potential energy Ep = -GMm/r Ep = kQq/r
Let’s try some questions
Pages 307 Questions 2, 4, 5, 6, 11, 12.