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Question: Gravitational force is the weakest force in nature. Explain....

Gravitational force is the weakest force in nature. Explain.

Explanation

Solution

Contrasting the other three key powers, gravity is the most vulnerable as far as the extent of the power. Electrostatic power and gravitational power are both contrarily corresponding to the separation squared.

Complete answer:
Electromagnetic power is relative to the charge of two items; gravitational power is legitimately corresponding to the mass of two articles. In this way, the recipe of the two appears to be comparative:
Fe=keq1q2d2{{F}_{e}}={{k}_{e}}\dfrac{{{q}_{1}}{{q}_{2}}}{{{d}^{2}}}
Fg=Gm1m2d2{{F}_{g}}=G\dfrac{{{m}_{1}}{{m}_{2}}}{{{d}^{2}}}
As it is obvious, then two have a part increased by a constant. To look at them, we can essentially think about the force:
ke=14πε0=8.99×109N.m2.C2{{k}_{e}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}=8.99\times {{10}^{9}}N.\,{{m}^{2}}.{{C}^{-2}}
G=6.67×1011N.kg2.m2G=6.67\times {{10}^{-11}}N.\,k{{g}^{-2}}.\,{{m}^{2}}
We don't need to take the qualities in front, we can essentially be the example of 10. ke{{k}_{e}} , the Coulomb's force, has an example of 9; , the gravitational constant, has a type of - 11. Clearly the power of gravity is frail.
Gravity is the weakest of the four central forces which are

  1. the strong atomic force
  2. the electromagnetic force
  3. the frail atomic force
  4. gravity.
    If by chance that you take two protons and hold them near one another, they will apply a few forces on one another. Since the two of them have mass, the two protons apply gravitational attraction on one another. Since the two of them have a positive electric charge, the two of them apply electromagnetic repulsion on one another.

Note : Additionally, the two of them have internal charge and subsequently apply attraction through the solid atomic power. Since the solid atomic power is the most grounded at short separations, it rules over different forces, and the two protons become bound. Gravity is so feeble at the nuclear scale that researchers can ordinarily disregard it without causing critical mistakes in their counts.