Mathematical Thinking

Table of Contents
Introduction
Fermi's Piano Tuner Problem
How Old is Old?
If the Terrestrial Poles were to Melt...
Sunlight Exerts Pressure
Falling Eastward
What if an Asteroid Hit the Earth
Using a Jeep to Estimate the Energy in Gasoline
How do Police Radars really work?
How "Fast" is the Speed of Light?
How Long is a Light Year?
How Big is a Trillion?
"Seeing" the Earth, Moon, and Sun to Scale
Of Stars and Drops of Water
If I Were to Build a Model of the Cosmos...
A Number Trick
Designing a High Altitude Balloon
Pressure in the Vicinity of a Lunar Astronaut Space Suit due to Outgassing of Coolant Water
Calendar Calculations
Telling Time by the Stars - Sidereal Time
Fields, an Heuristic Approach
The Irrationality of
The Irrationality of
The Number (i)i
Estimating the Temperature of a Flat Plate in Low Earth Orbit
Proving that (p)1/n is Irrational when p is a Prime and n>1
The Transcendentality of
Ideal Gases under Constant Volume, Constant Pressure, Constant Temperature and Adiabatic Conditions
Maxwell's Equations: The Vector and Scalar Potentials
A Possible Scalar Term Describing Energy Density in the Gravitational Field
A Proposed Relativistic, Thermodynamic Four-Vector
Motivational Argument for the Expression-eix=cosx+isinx
Another Motivational Argument for the Expression-eix=cosx+isinx
Calculating the Energy from Sunlight over a 12 hour period
Calculating the Energy from Sunlight over actual full day
Perfect Numbers-A Case Study
Gravitation Inside a Uniform Hollow Sphere
Further note on Gravitation Inside a Uniform Hollow Sphere
Pythagorean Triples
Black Holes and Point Set Topology
Field Equations and Equations of Motion (General Relativity)
The observer in modern physics


How Do Police Radars Really Work?

Problem:
A car, traveling at speed, V, approaches a police radar, scanning for speeders with a frequency, frequency. Calculate the approximate frequency shift of the reflected signal.

Solution:
Consider a single photon from the police radar. The photon must interact with the approaching car for a finite time while it is being reflected. Call this time, deltat. Let an interaction force, ± f, exist between the photon and the car for the time, deltat. The force exerted by the photon on the car, +f, acts to remove energy from the car. The force exerted by the car on the photon, -f, acts to add energy to the photon. Therefore, we expect the photon frequency to increase. During the time deltat, the car travels a distance deltas = V deltat. We may now write two equations, one for a change in momentum, deltap, and one for a change in energy, deltaE:

Momentum:
deltap = f deltat
1.
Energy:
deltaE = f deltas = fV deltat
2.

Since the photon energy, E, is equal to hn, where h = Planck's constant = 6.63 X 10-34 j sec, then

deltaE = h deltafrequency
3.

Also, since photon momentum equals h/c, where c is the speed of light, then

deltap = 2hfrequency/c + h deltafrequency/c
4.

where the first term on the RHS represents deltap for an elastic reflection (i.e., one for which deltaE = 0), and the second term takes into account the change in frequency due to the change in energy.

Dividing eq. 1 by eq. 2, and substituting for deltaE and deltap from eqs. 3 and 4, we find

(2hfrequency/c + h deltafrequency/c)/(h deltafrequency) = 1/V
5.

This equation may be simplified to read

deltafrequency/frequency = 2V/(c-V) approximately 2V/c
6.

where the final step results from V << c. Now, let V = 60 mph = 27 m/sec, and let frequency = 5 X 108 Hz. Then,

deltafrequency= 90 Hz
7.

The police radar detector easily detects this frequency shift.