Nikola Tesla Books
make the ratio $! {{E \over e} = {x^{2} \over 60^{2}}} $!, where x will be in feet. At the lowest estimate E was 10,000 volts and assuming an ordinary instrument be used as a receiver, requiring $! {i \over 10,000} $! of a volt = e between c and d, we would have $! {x^{2} = 60^{2} \times {10,000 \over {1 \over 10,000}} = {36 \times 10^{10}}} $! or 600,000 feet or x = 114 miles nearly. But by making the distance between c and d much greater the transmission radius may be greatly extended.
Capacity of secondary 35 turns used in preceding experiments.
The average length of one turn may be put at approximately 135.1 feet = 4120 cm. The wire is No. 10 B. & S. diam = 0.102" = 0.26 cm. Surface of wire in sq. cm. = â¼ x 0.26 x 4120 x 35 = â¼ x 37,500 cm. approx. The capacity was compared with that of 1/2 mfd. standard condenser and was found to be C = 3600 cm. This measurement was I expect correct within 1/2%.
Note: The measurement was made by connecting the cable with one end, or with both ends to the source, the other terminal of which was connected to the earth. Result was the same.
Now it is of interest to compare the value found by measurement with that which the cable would have when stretched out. Its capacity would then be $! {C_{1} = {l \over {2 \log_{e} {l \over p}}}} $! considered as a cylinder remote from the ground. Taking the values as above
$! {C_{1} = {{4120 \times 25} \over {2 \log_{e} {4120 \over 0.13}}} = {{4120 \times 35} \over {2 \log_{e} 31,700}} = {{2060 \times 35} \over {\log_{e} 31,700}} = {{2060 \times 35} \over {4.50106 \times 2.3}} =} $!
$! {{2060 \times 35} \over 10.35244} $! = 6965 cm.
If we consider the cable in its capacity with reference to the earth or conducting plane its capacity would then be $! {C_{2} = {1 \over {2 \log_{e} {2 d \over r}}}} $!. Since we have found the measured value we may find from it the distance d; we have $! {3600 = {{4120 \times 35} \over {2 \log_{e} {2 d \over r}}}} $! from which $! {{\log_{e}{2 d \over r}} = {{4120 \times 35} \over {2 \times 3600}} = 20.3} $! and this gives
$! {{\log_{e} {2 d \over r}} = {20.3 \over 2.3} = 8.82607} $!, hence $! {2 d \over r} $! = 67,000,000 cm
$! {d = {{67,000,000 \over 2} \times {13 \over 100}} = {670,000 \times 13 \over 2} = 670,000 \times 6.5 = 67,000 \times 65 =} $! 44,550 meters!
The result only shows that the cable measures much more when straight and at some distance from the ground since d comes out so large.
104
July 24
During that day the notes are divided in three parts (previous day in two parts), which is shown by designation of original handwritten pages. The first part pertains to experiments with oscillator secondary with 35 turns, and it is described on three pages; second part on five pages, pertains to this experiments continuation, and third part on three pages is devoted to the question of oscillator secondary capacitance. The oscillator secondary consists of 35 turns.
When adjusting the oscillator; Tesla most frequently changes the regulating coil in the primary, and so obtains the maximum voltage in secondary (which he determines according to the longest spark). In the secondary he connects "additional coil" to the open secondary terminal. He checks the operation with harmonics so that he doubles the primary capacitance*, and by small regulations of primary inductance he changes the primary operating frequency, in order to achieve maximum effect on the secondary which is supposed to oscillate at double frequency - primary harmonic. He doesn't obtain the expected results and continues the experiment with capacitive loading changes in secondary circuit, and looks for most suitable elements in the primary circuit. He considers that he obtained the best result when sparks in the secondary are most powerful.
In continuation of experiments with the transmitter, he looks for an explanation for the appearance of largest current streamers in the secondary when the inductance of regulating coil in the primary circuit is reduced to a minimum (and then it is practically disconnected from the circuit). Tesla was confused with the fact that maximum voltage at the open end of the additional coil (this coil is connected to the secondary similar as on Fig. 2 on July 11) doesn't occur when the excitation current frequency is equal to the coil's self resonant frequency. After an extensive analysis, Tesla came to the correct conclusion (opposite to the one of June 30 which was correct only in a special case) that in cases where the secondary free vibration is emphasized, parameters, of the primary circuit have to be weighed such as to achieve the maximum voltage in the secondary, and the additional coil self-resonant frequency has to be equal to the frequency of the combined system primary-secondary. It appears Tesla did not assume that when the link is good, the combined system produces a distinguished spectrum during and after spark interruption. It seems to us that much more important is the abovementioned conclusion which he established when combining the experimental results, simple theory and intuition.
When experimenting with his oscillator, Tesla observed that during a discharge in the secondary the sparking appears on lighting arresters as well. As these arresters are connected to the supply feeder, he assumed that the high frequency voltage originates from a wave which propagated through the ground, and at a certain location entered the feeder. The data is missing which would help to establish whether this high frequency voltage is actually a consequence of the oscillator link via supply transformer with the supply feeder.
In third part of notes on July 24 he gives measurement results of secondary coil capacitance as a whole with respect to the ground. He didn't mentioned how he performed the measurement by comparison with standard capacitor and then, by using several methods he calculates the wire capacitance of the same length as coil wire (C1) according to the equation for capacitance of a single ellipsoide of which the longer axis is considerably longer than short one, and C2 according to the equation for conductor capacitance above an ideally conductive plane under the condition when the distance from the plane is considerably larger than wire radius). Expanding on considerations for capacitances, he describes the methods for achieving the largest capacitances, and moves further and further away from his initial topic. He ends the notes with a discussion on the spheres filled with hydrogen which were supposed to have maximum capacitance for given dimensions, and which would therefore be used for telegraphy without wires.
* In order to get the primary to oscillate on two times lower frequency, the capacitance has to be four-fold. It is possible instead of series connection 8-9 jars which is equivalent to 4-4 1/2 jars he connected two previous series connections in parallel, and obtained the equivalent capacitance of 16-18 jars, that is four times larger than the equivalent capacitance of jars connected in series.