हिंदी

What is the Pressure Inside the Drop of Mercury of Radius 3.00 Mm at Room Temperature? Surface Tension of Mercury at that Temperature (20°C) is 4.65 × 10–1 N M–1. the Atmospheric Pressure is 1.01 × 105 Pa. Also Give the Excess Pressure Inside the Drop - Physics

Advertisements
Advertisements

प्रश्न

What is the pressure inside the drop of mercury of radius 3.00 mm at room temperature? The surface tension of mercury at that temperature (20°C) is 4.65 × 10–1 N m–1. The atmospheric pressure is 1.01 × 105 Pa. Also give the excess pressure inside the drop

उत्तर १

1.01 x 105 Pa; 310 Pa

Radius of the mercury drop, r = 3.00 mm = 3 × 10–3 m

Surface tension of mercury, S = 4.65 × 10–1 N m–1

Atmospheric pressure, P0 = 1.01 × 105 Pa

Total pressure inside the mercury drop

= Excess pressure inside mercury + Atmospheric pressure

`= (2S)/r + P_0`

`= (2xx4.65xx10^(-1))/(3xx10^(-3)) + 1.01 xx 10^5`

= 1.0131 × 105

= 1.01 ×105 Pa

Excess Pressure =  2S/r

`= (2xx4.65xx10^(-1))/(3xx10^(-3)) = 310 Pa`

shaalaa.com

उत्तर २

Excess pressure =  `(2sigma)/R` = (2xx4.65xx10^(-1))/(3xx10^(-3)) = 310 Pa`

Total Pressure = `1.01 xx 10^5  + (2sigma)/R`

=` 1.01 xx 10^5 + 310 = 1.0131 xx 10^5 Pa`

Since data is correct up to three significant figures, we should write total pressure inside the drop as 1.01 x 105  Pa.

shaalaa.com
  क्या इस प्रश्न या उत्तर में कोई त्रुटि है?
अध्याय 10: Mechanical Properties of Fluids - Exercises [पृष्ठ २७०]

APPEARS IN

एनसीईआरटी Physics [English] Class 11
अध्याय 10 Mechanical Properties of Fluids
Exercises | Q 19 | पृष्ठ २७०

संबंधित प्रश्न

A vertical off-shore structure is built to withstand a maximum stress of 109 Pa. Is the structure suitable for putting up on top of an oil well in the ocean? Take the depth of the ocean to be roughly 3 km, and ignore ocean currents.


A tank with a square base of area 1.0 m2 is divided by a vertical partition in the middle. The bottom of the partition has a small-hinged door of area 20 cm2. The tank is filled with water in one compartment, and an acid (of relative density 1.7) in the other, both to a height of 4.0 m. compute the force necessary to keep the door close.


It is known that density ρ of air decreases with height as `0^(e^(y/y_0))` Where`rho_0` 1.25 kg m–3 is the density at sea level, and y0 is a constant. This density variation is called the law of atmospheres. Obtain this law assuming that the temperature of atmosphere remains a constant (isothermal conditions). Also, assume that the value of gremains constant


In the derivation of P1 − P2 = ρgz, it was assumed that the liquid is incompressible. Why will this equation not be strictly valid for a compressible liquid?


Suppose the density of air at Madras is ρo and atmospheric pressure is P0. If we go up, the density and the pressure both decrease. Suppose we wish to calculate the pressure at a height 10 km above Madras. If we use the equation Po − P = ρogz, will we get a pressure more than the actual or less than the actual? Neglect the variation in g. Does your answer change if you also consider the variation in g?


Share
Notifications

Englishहिंदीमराठी


      Forgot password?
Use app×