LIFE TIME:
BILL ADONGO(1983-present),
a Ghanaian mathematician, actuary, chemist and physicist. He defined modern
science by his Least Whole Normal Theory which is used for fitting two or more
quantitative products in sciences. He is a brilliant
scientist and he formulated new laws in sciences and mathematics that have
great impact in the life of present scientists. BILL ADONGO keeps diary recording all applications of his Least Whole Normal theory. Below is copy
of his diary.
CAPACITOR, VOLTAGE AND CHARGE
A capacitor is a passive element designed to store energy in
its electric field. Besides resistors, capacitors are the most common
electrical components. Capacitors are used extensively in electronics
communications, computers, and power systems. For example, they are used in the
tuning circuits at radio receivers and as dynamic memory element,
In many practical applications, the plates may be aluminum
foil which the dielectric may be air, ceramic, paper, or mica. When a voltage
source deposits a positive charge q on
one plate and a negative charge -q on the other, Capacitor is said to
store the electric charge. The amount of charge stored, represented by q, is
directly proportional to the applied voltage V so that
q=CV
Where C, the
constant of proportionality, is known as the capacitance of the capacitor. Finding
way of measuring unknown amount of charge stored q sand unknown capacitance of the capacitor C, with only known voltage V
is impossible without employing my Least
Whole Normal Measurement. From previous publications, I talk of theory of
quantitative products where two or more quantitative products in science can be
fitted by my Least Whole Normal Function and when applying this theory, the
equation above will yield
T= µc*τv-
ф-1(γ%)√(S2τv)
E(C)=1/Vp[T+ф-1(γ%)√(S2Vp)]
E(q)=E(C)Vp
where Vp is
the independent voltage for
predicting the expected of amount of
charge stored E(q) and the expected capacitance of the capacitor E(C).
EXAMPLE
Calculate the capacitance of the capacitor C and amount of
Charge stored q if the voltage is 8V based on the previous experiment made on
six Capacitance of the capacitors and their known voltage.(take γ=95).
Capacitance of the capacitor(C)
|
Voltage(V)
|
60mF=60x10-3
|
5
|
50mf=50x10-3
|
6
|
40mF=40x10-3
|
7.5
|
30mF=30x10-3
|
10
|
20mF=20x10-3
|
15
|
10mF=10x10-3
|
30
|
SOLUTION
MEAN AND STANDARD DEVIATION
C
|
V
|
CV
|
Deviation of c from mean(d)
|
d2
|
Vd2
|
60mF=60x10-3
|
5
|
0.3
|
0.03551
|
0.001261
|
0.006305
|
50mf=50x10-3
|
6
|
0.3
|
0.02551
|
0.000651
|
0.003905
|
40mF=40x10-3
|
7.5
|
0.3
|
0.01551
|
0.000241
|
0.001804
|
30mF=30x10-3
|
10
|
0.3
|
0.00551
|
0.000030
|
0.003036
|
20mF=20x10-3
|
15
|
0.3
|
0.00449
|
0.000020
|
0.000302
|
10mF=10x10-3
|
30
|
0.3
|
-0.01449
|
0.000210
|
0.006299
|
Mean(µc)=∑CV/∑V=1.8/73.5=0.02449
Standard Deviation(S)=√(∑Vd2/∑V=√(0.021651/73.5=0.017147
From the data above we have;
T= µc*τv-
ф-1(γ%)√(S2τv)
But τv=∑V/N=73.5/6=12.25
T=0.02449x12.25- ф-1(95%)√(0.0171472x12.25)
T=0.2012761475
E(C)=µc*Vp=1/Vp[T+ф-1(γ%)√(S2Vp)]
E(C)= 1/8[0.2012761475+ф-1(95%)√(0.0171472x8)]
E(C)=0.035=35x10-3=35mF
q=E(C)Vp=35x10-3x8=0.3
Hence, the capacitance of the capacitor and charge stored
are 35mF and 0.3 respectively if the voltage is 8V.
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