Title: Mathematical Models of Love
1Mathematical Models of Love Happiness
- J. C. Sprott
- Department of Physics
- University of Wisconsin - Madison
- Presented to the
- UW-Madison Math Club
- in Madison, Wisconsin
- on October 21, 2002
2Disclaimers
Its Strogatz fault
This is not serious psychology
3The Mathematics
R is Romeos love for Juliet (or hate if negative)
J is Juliets love for Romeo
The simplest linear model is
dR/dt aR bJ
a and b describe Romeos Romantic Style
4Some Romantic Styles
- dR/dt aR bJ
- a0 (out of touch with own feelings)
- b0 (oblivious to others feelings)
- agt0, bgt0 (eager beaver)
- agt0, blt0 (narcissistic nerd)
- alt0, bgt0 (cautious lover)
- alt0, blt0 (hermit)
5What about Juliet?
She has her own style
dJ/dt cR dJ
4 parameters with 3 choices for each gives 81
different romantic pairings
6Both out of touch with their own feelings
0
- dR/dt aR bJ
- dJ/dt cR dJ
- Four subclasses
- b gt 0, c gt 0 (mutual love fest or war)
- b gt 0, c lt 0 (never-ending cycle)
- b lt 0, c gt 0 (never-ending cycle)
- b lt 0, c lt 0 (unrequited love)
0
7Out of touch with their own feelings (continued)
b gt 0, c gt 0
b lt 0, c lt 0
b gt 0, c lt 0
War
Two lovers Love fest (or war)
Two nerds Unrequited love
Nerd lover Never-ending cycle
8With Self-Awarenessand bc lt 0 (nerd lover)
a d lt -2bc1/2
a d lt 0
a d gt 0
Extremely cautious Rapid apathy
Somewhat cautious Eventual apathy
Overly eager Growing volatility
(The only equilibrium is apathy)
9Fire and Water(Do opposites attract?)
- Take c -b and d -a
- Result depends on a, c, and the initial
conditions - Can end up in any quadrant
- Or with a steady oscillation
- But never apathy
10Peas in a Pod(Are clones bored or blissful?)
- Take c b and d a
- Result depends on a, b, and the initial
conditions - Can end up in any quadrant
- Or at the origin (boredom)
- But no oscillations
11Romeo the Robot(How does Juliet react?)
- Take a b 0 (dR/dt 0)
- dJ/dt cR dJ
- There is an equilibrium at J -cR/d
- Can be either love or hate depending on signs of
R, c, and d - Stable if d lt 0, unstable if d gt 0
- Her feelings never die
- No oscillations are possible
12A Love Triangle
- Romeo has a mistress, Guinevere
- Guinevere and Juliet dont know about one another
- Romeo responds to each with the same romantic
style (same a and b) - Guineveres hate has the same effect on his
feelings for Juliet as does Juliets love, and
vice versa
13Love Triangle Equations
- dRJ/dt aRJ b(J - G)
- dJ/dt cRJ dJ
- dRG/dt aRG b(G - J)
- dG/dt eRG fG
- System is 4D (4 variables)
- There are 6 parameters
- System is linear (no chaos)
14Love Triangle Examples
15Romeos Fate
- Averaged over all romantic styles (64
combinations of parameters) and 64 initial
conditions - 37 loves Juliet hates Guinevere
- 37 loves Guinevere hates Juliet
- 6 loves both (2 everyone in love)
- 6 hates both (2 everyone in hate)
- 14 apathy (10 everyone apathetic)
- Anything can happen!
16Effect of Nonlinearities
Replace ax with ax(1-x) (logistic function)
ax(1 - x)
ax
x
17New kinds of Dynamics
New equilibrium points
Limit cycles
(but no chaos in 2D)
18One Chaotic Solution of Nonlinear Love Triangle
Strange attractor of love
19Simple 2D Linear Model
- d2R/dt2 bdR/dt w2R 0
- b -a - d (damping)
- w2 ad - bc (frequency)
20Solutions of 2-D Linear System
Time
21Happiness Model
- d2x/dt2 bdx/dt w2x F(t)
- Happiness H dx/dt
- Habituation
- Acclimation
- Adaptation
- Only changes are perceived
Damping
Oscillation
External forces
22What is x?
- x integral of H
- x is what others perceive
- In the love model x is what the other feels
- H (your happiness) must average to zero (with
positive damping) - x does not average to zero
23Winning the Lottery
24Drug or Other Addiction
25Intermittent Reinforcement
26Random Events
27Real Life
28Parameter Space
b
w
2
29Nonlinearities
- There are many possibilities.
- Try bdx/dt --gt b(1 - x2)dx/dt
- This gives growth for small x and damping for
large x. - The resulting equation was studied by van der Pol
(1926). - Oscillations occur even without an external
force. - It has been used to model a variety of nonlinear
oscillators.
30Bipolar Behavior
31Periodically Driven Chaos
32Happiness Attractor
33Autonomous Chaos
34Happiness Attractor 2
35Some Implications
- Constant happiness is an unrealistic goal.
- Others see less volatility in you and often
wrongly conclude how you feel. - Individuals can be categorized by their values of
b and w. - Bipolar disorders may correspond to negative or
small b. - Long prison terms may be ineffective.
36Some other happiness studies
- Brickman, Coates Janoff-Bulman (1978) report
only small differences in life satisfaction
between paraplegics, control subjects, and
lottery winners. - Lykken (1981) reports that religious people are
not noticeably happier than freethinkers. - Diener Diener (1996) review studies indicating
that all American socioeconomic groups score
above neutral in life satisfaction, as do people
with severe disabilities.
37Studies involving disabilities
- Hellmich (1995) reports that 84 of individuals
with extreme quadriplegia say that their life is
average or above average. - Delespaul DeVries (1987) report that people
with chronic mental problems claim positive
well-being.
38Studies of the dynamics
- Silver (1982) reports that individuals with
spinal cord injuries are very unhappy immediately
following their injury, but that 58 state that
happiness is their strongest emotion by the third
week after their injuries. - Suh, Diener, Fujita (1996) report that good and
bad events have almost no effect on happiness
after 6 months.
39In Summary ...(Lykken 1999)
- There seem to be no permanent ups and downs
natural selection has made us this way, because,
by accommodating to both adversity and to good
fortune in this fashion, we remain more
productive, more adaptable to changing
circumstances, and more likely to have viable
offspring.
40Other Similar Qualities
- Sense of wealth
- Health
- Beauty
- Intelligence
- Spirituality
- Skills
- Senses
- hot/cold
- smell
- vision
- hearing ...
41Summary
- Love and happiness are wonderful
- So is mathematics
42References
- http//sprott.physics.wisc.edu/
lectures/lovehap/ (This talk) - Steven H. Strogatz, Nonlinear Dynamics and Chaos
(Addison-Wesley, 1994) - sprott_at_physics.wisc.edu
- Collaborations are welcome!