Gravitational constant "G" is called as universal gravitational constant and is defined as the gravitational force of attraction between two unit masses( having mass 1 Kg each) separated by unit distance(1 m). Its value is found to be 6.67 x 10-11 NM2/Kg2. It is independent of shape, size and distance between the masses. So ,it is termed as universal gravitational constant.
NP's Solution
Monday, September 29, 2014
Sunday, September 28, 2014
How to derive P=hdg? by Bikash Shrestha
This formula is used to calculate the pressure exerted by any liquid at certain depth.
Let a vessel with cross
sectional area 'A' is filled
with any liquid of
density 'd', volume 'V' and mass
'm' up to the height 'h'
as shown in the figure
alongside. Now ‘h’
is termed as depth of liquid
from the free surface.
According to the
definition of Pressure,
P = F/A
or, P = mg/A
[ since F = mg ]
or, P = Vdg/A
[ since m = Vd ]
or P =
Ahdg/A [ since V = Ah ]
\ P = hdg where g is the acceleration due
to gravity of that place.
This clearly shows that
liquid pressure is dependent on h(depth of liquid from the free surface), d(
the density of the liquid) and g( the acceleration due to gravity of that
place) but independent of volume of liquid, shape and size of the liquid
container.
At certain place, the density 'd' of the liquid and acceleration due to gravity 'g' are constant. So, pressure of the liquid only depends on depth 'h' from free surface. Due to this reason a bucket can be filled faster from the tap in ground floor than in other floors as liquid pressure is directly proportional to the depth and the depth of the liquid in the tap of ground floor is maximum.
At certain place, the density 'd' of the liquid and acceleration due to gravity 'g' are constant. So, pressure of the liquid only depends on depth 'h' from free surface. Due to this reason a bucket can be filled faster from the tap in ground floor than in other floors as liquid pressure is directly proportional to the depth and the depth of the liquid in the tap of ground floor is maximum.
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