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Note that 1 μGal equals 1 × 10−8 m s−2 in gravity change.
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Even though the negative-positive pattern in gravity changes and the positive-negative-positive feature in northern gradient changes are still obviously detected, the signals retrieved from the 1-month data set are more contaminated by stripes than those from the 2-year data (see Figure 4a,b,c,d) due to the absence of stacking to suppress stripe errors.
At OMZ and KKG close to the Suruga Trough, gravity increases by 3 μGals in the periods after year 2000 and 2008, which can explain 30 and 10% of the secular increase in the gravity change, respectively.
The distribution of the gravity changes in this period is look similar trend with the previous period in 1999 to 2008 gravity change.
The vertical axes denote relative gravity change in μGal and offsets are added for visualization.
Instead of invoking dark matter, the Modified Newtonian Dynamics theory says that the effects of gravity change in places where its pull is very low.
In our model, the gravity change was nearly zero at W3, and the location of the maximum increase almost agreed with their result (Fig. 6(b)).
Both postseismic processes produce similar gravity change in spatial and temporal pattern as well as the magnitude.
To identify temporal variations in the gravity changes associated with the LSSEs, we calculated rate changes for the gravity data at all the correction levels (Fig. 3a c).
Figure 6(a) shows the gravity change Ag in the year following the 2011 eruption.
Figure 2 shows global distribution of the annual gravity change used in this study.
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