This note is not exactly an independent paper. The original intention was to create a brief communication to show the correlation between the experimental data from two different experimental works. The author apologizes for lack of details on this communication about the Big G issue and recommends that interested readers check the reference for a complete overview on this point.

On August 29^th, 2018, a scientific team reported a measure of the Universal Gravitational Constant, also known as Big G, with the lowest error ever. In this journal, Li et al. [1] announced two new values for Big G using two independent settings. The values for G were determined to be 6.674184(12) × 10⁻¹¹ m³∙kg⁻¹∙s⁻² using a technique called TOS and 6.674484(12) × 10⁻¹¹ m³∙kg⁻¹∙s⁻² using another technique called AAF. The physical nature of Big G is so goosy that after more than two years of science-art work, Li et al. exceed the precision reported in the work by Gundlach et al. [2] in the year 2000 [6.674215(92) × 10⁻¹¹ m³∙kg⁻¹∙s⁻²] by only ninety parts in a million. Many technological advances have occurred within the last 18 years, but the increment in precision between both studies is not well correlated with those advances. Another intriguing situation appears after comparing the numbers in red in the values reported by Li et al. The errors in both values cannot cover the 300^th of a million separations between them. It is not hard to imagine that this situation indicates that something is missing or hidden.

Schlamminger [3] published a comment in Nature on August 29^th, 2018, calling attention to the fact that the TOS and AAF experiments were done by the same people, in the same place, and close in time. He thinks this could be a good combination to solve the G puzzle and proposes that Li et al. carry out a study explaining why they observe two non-overlapping values. He clarifies that the explanation can help to guide future research. Schlamminger moves as far as proposing to all the scholars to keep an open mind in regards to this problem. He wrote “A second possibility is that some unknown physics could explain the scatter in the published values. Although this possibility is, of course, the more exciting, it is also the less likely. Nevertheless, it should not be dismissed lightly”.

Moreover, I published papers in 2017 [4] and 2018 [5] covering the Big G issue both theoretically and experimentally. Therein, I mentioned that an unnoticed correlation exists between the best G values reported in the last 30 years and the distance to the Sun. Thirty years is a long period, which made it more difficult to draw a comparison between the studies carried out in so many labs throughout the world. Li et al.’s work enabled a facilitated analysis because their work and my work were produced during the same period.

I used a modified Cavendish’ balance with two strings instead of the original single string balance. The length and separation of the strings act as a mechanical filter allowing only microscopic oscillations. Nothing is moved by human decision in this setting. This dynamic permits a precise reading of any variation in the separation between the masses on the balance and the masses fixed to the ground. Thus, 650 variations were collected, one per day, due to the apparent attraction between the masses. Unfortunately, it was not possible to calculate the value for Big G with this setting because two new variables appeared, as shown in Equation (1) (For details, see Equation (3) in [5] ). The effect of the angular variable was cancelled out in regular gravitational experiments by alternating the position of the attractor masses. The other effect created by the distance to the Sun cannot be neutralized completely because of non-linear effects. Li et al. have obtained 29 precise values for Big G; however, they failed to study the systematic variations of those values throughout the years. Every team has plenty of information on one type but lack information on the other. An intelligent combination of both types of experimental information can produce a clear and precise pattern for this gravitational problem.

G exp = G N E + G ( a , α ) ( a r ) 3 C o s ( θ t o r u s ) (1)

The team of Li et al. failed to report any possible variations of their data by taking into account other variables that might affect the results such as time or the distance from the Sun. Figure 1 included only the AAF data for reasons

explained later. A pattern is clear in Figure 1, despite only having 29 G values. The figure included a dashed line representing the Earth’s path, an offset yellow spot representing the Sun and a fitting curve. The red side of the fitting curve corresponds to the January-December period.

Figure 2 was created using the main values from AAF to introduce a fitting function. Figure 2 included only the 29 G values obtained from the AAF experiments versus a unit-less parameter x correlate with the distance to the Sun. The x is the ratio between the instantaneous distance to the Sun and the average to that distance, also called the Astronomical Unit. Every value from AAF was determined after an average of three days. However, every value from TOS required an average of 132 days. That is an exclusionary condition in this analysis because such a large period hides progressive variations. This lengthy variation, which was not taken into account, can be used to explain why the final G value determined using TOS is closer to the average G recommended by standard government departments.

Figure 1 also includes the regression function that corresponds to the theoretical model proposed by the author.

G exp . = { ( 6.67218 ± 0.00037 ) + 0.00228 ± 0.00036 x 3 } × 10 − 11   m 3 kg − 1 s − 2 (2)

In Equation (2), the value of 6.67218 × 10⁻¹¹ m³∙kg⁻¹∙s⁻² corresponds to the constant Big G. According to the author, the 0.00228(36) × 10⁻¹¹ m³∙kg⁻¹∙s⁻² value is due to the dragging effect arising from the nucleus of the Sun.

Now, it is possible to integrate the Big G data obtained by Li et al. with the variations recorded by the author.

The pattern in Figure 3 matches very well with Equation (1). The observed peaks are due to nutation’ effects. Figure 3 includes a ribbon-like feature that is correlated to the fitting of Equation (2) but with new errors. The width of the ribbon is a visual representation of the new heightened precision. The ribbon was created using Equation (3) to contain the main sequence of the author’s experimental data.

G exp . = { ( 6.67218 ± 0.00020 ) + 0.00228 ± 0.00020 x 3 } × 10 − 11   m 3 kg − 1 s − 2 (3)

The average of the available experimental values of Big G can create confidence on its real value only to the third significant figure (6.67). Any researcher looking for more precise information about Big G requires considering the experimental variation of its value with the distance to the Sun. This is experimentally justified by all the research conducted since Cavendish. Any art of science work in the modern time ought not aim or attempt to overcome this constraint. Many scholars may disagree with the assertion made in the author’s initial hypothesis, but any argument can be brought in future work. In order to assert a different position on the hypothesis future work and research would have to be conducted; however, a six-significant figure on the value of Big G is due by now.

The author declares no conflicts of interest regarding the publication of this paper.

Parra, J.L. (2018) The Sun and Big G Measurements. Journal of Applied Mathematics and Physics, 6, 2397-2401. https://doi.org/10.4236/jamp.2018.611202