discussion | summary | practice | problems |

## Kinetic and Potential Energy Practice

### practice problem 1

#### solution

Answer it.

### practice problem 2

#### solution

Answer it.

### practice problem 3

^{9}J of chemical potential energy.)

#### solution

State the givens and the unknown.

h = | 415 m |

m = | 2(550,000,000 kg) ^{9} kg |

U = _{g} | ? |

Since the mass of the towers is distributed throughout their volume and is not concentrated at a point, this problem is best solved using calculus. Assume a uniform linear mass density (λ = *m*/*h*) and integrate the potential energy formula over the height of the towers.

h | | |

U = _{g} | ⌠⌡ | λgy dy |

| 0 | |

| | | h | |

U = _{g} | m | g | ⌠⌡ | y dy |

h | ||||

| | | 0 | |

U = _{g} | mg | | h^{2} |

h | 2 |

Not surprisingly, the results show that the center of mass of a tower lies at its geometric center, halfway up.

U = _{g} | mgh |

2 |

Numbers in.

U = _{g} | (1.1. × 10^{9} kg)(9.8 m/s^{2})(415 m) | |

2 |

Answer out (in joules).

U = _{g} | 2.2 × 10^{12} J |

Convert to the TNT equivalent.

U = _{g} | 2.2 × 10^{12} J | |

4.184 × 10^{9} J/ton TNT | | |

U = 530 ton tnt_{g} | ||

The gravitational energy released when the towers collapsed was thus about a thousand times greater than the chemical energy released when the truck bomb exploded.

### practice problem 4

A region of space has the following two-dimensional potential energy function…

*U*(*x*, *y*) = *x*^{4} + *y*^{4} + 2*x*^{2}*y*^{2} − 8*x*^{2} + 8*y*^{2} + 16

Find the…

- points of stable and unstable equilibrium
- range of bound states (not the right term for what I’m thinking of)

#### solution

- Stable equilibrium occurs at local minima. Unstable equilibrium occurs at local maxima. Minima and maxima are local extrema and occur where the value of the first derivative is zero. Let’s find those points.
*U*(*x*,*y*) =*x*^{4}+*y*^{4}+ 2*x*^{2}*y*^{2}− 8*x*^{2}+ 8*y*^{2}+ 16**∂***U***= 4***x*^{3}+ 0 + 4*xy*^{2}− 16*x*+ 0 + 0 = 0**∂***x***∂***U***= 0 + 4***y*^{3}+ 4*x*^{2}*y*− 0 + 16*y*+ 0 = 0∂ *y*Clean up and simplify the results.

*x*^{3}+*xy*^{2}− 4*x*= 0*y*^{3}+*x*^{2}*y*+ 4*y*= 0Factor each equation.

*x*(*x*^{2}+*y*^{2}− 4) = 0*y*(*y*^{2}+*x*^{2}+ 4) = 0Therefore…

*x*= 0**or***x*^{2}+*y*^{2}− 4 = 0*y*= 0**or***y*^{2}+*x*^{2}+ 4 = 0The last of these conditions is impossible to satisfy using real numbers.

*y*^{2}+*x*^{2}+ 4 = 0This expression has no real solutions. Therefore

*y*= 0 and nothing else. Which means that the statement…*x*= 0**or***x*^{2}+*y*^{2}− 4 = 0should really be stated as…

*x*= 0**or***x*^{2}− 4 = 0and therefore

*x*= 0, +2, −2A point with zero derivative could be a minimum, but it could also be a maximum or a saddle point. Use the second derivative to determine the type of stationary point.

*U*(*x*,*y*) =*x*^{4}+*y*^{4}+ 2*x*^{2}*y*^{2}− 8*x*^{2}+ 8*y*^{2}+ 16**∂**^{2}*U***= 12***x*^{2}+ 0 + 4*y*^{2}− 16 + 0 + 0**∂***x*^{2}**∂**^{2}*U***= 0 + 12***y*^{2}+ 4*x*^{2}− 0 + 16 + 0**∂***y*^{2}Clean up and simplify the results.

**∂**^{2}*U***= 12***x*^{2}+ 4*y*^{2}− 16**∂***x*^{2}**∂**^{2}*U***= 12***y*^{2}+ 4*x*^{2}+ 16**∂***y*^{2}Let’s test each of the three stationary points. Start with (−2, 0)…

**∂**^{2}*U***= 12(−2)**^{2}+ 4(0)^{2}− 16 = +32**∂***x*^{2}**∂**^{2}*U***= 12(0)**^{2}+ 4(−2)^{2}+ 16 = +32**∂***y*^{2}Then (+2, 0)…

**∂**^{2}*U***= 12(+2)**^{2}+ 4(0)^{2}− 16 = +32**∂***x*^{2}**∂**^{2}*U***= 12(0)**^{2}+ 4(+2)^{2}+ 16 = +32**∂***y*^{2}The second derivative in both coordinate directions at both locations is positive, which means the curvature is concave up in every direction and that these two points are local minima or points of stable equilibrium.

At the origin (0, 0), however,…

**∂**^{2}*U***= 12(0)**^{2}+ 4(0)^{2}− 16 = −16**∂***x*^{2}**∂**^{2}*U***= 12(0)**^{2}+ 4(0)^{2}+ 16 = +16**∂***y*^{2}The second derivative is negative along the

*x*-axis, which means the surface curves down, but it is positive along the*y*-axis, which means the surface curves up. What we have here is a saddle point. The location is unstable in the ±*x*directions and stable in the ±*y*directions.To summarize…

coordinates stationary point equilibrium (−2, 0) local minimum stable in all directions (0, 0) saddle point unstable along the *x*-axis

stable along the*y*-axis(+2, 0) local minimum stable in all directions - We could continue trying to visualize this potential energy surface in our heads or we could use some appropriate technology and view a computer rendered image. I think we’ve laid out enough basics to give us a head start. Our potential energy surface has two wells lying on the
*x*-axis on opposite sides of the origin and a saddle point in the middle.I think it looks something like a pair of trousers, so I’ve dubbed it the “trouser potential”. This is my personal name and is not something you should memorize for a test.

The whole thing is one giant well. The saddle point at the origin divides the potential surface into two domains for values below 16 of our arbitrary units.

*U*(*x*,*y*) =*x*^{4}+*y*^{4}+ 2*x*^{2}*y*^{2}− 8*x*^{2}+ 8*y*^{2}+ 16*U*(0, 0) =0 + 0 + 0 − 0 + 0 + 16 *U*(0, 0) =+16 Come back and finish this later.