In the Bohr model of the hydrogen atom, an electron (mass = 9.10 10-31 kg) orbits a proton at a distance of 4.76x10-10 m. The proton pulls on the electron with an electric force of 1.02x10-9 N. How many revolutions per second does the electron make?

Answer 1
We know that the force of attraction #F#of proton on electron in the hydrogen atom provides the required centripetal force required for the motion of electron in circular orbit.
If #n# be the number of revolutions per sec made by the electron around the nucleus then centripetal force is given by
#F=momega^2r=m4pi^2n^2r#
where radius of the orbit #" "r=4.76xx10^-10m#
mass of an electron #" "m=9.1xx10^-31kg#
#F=1.02xx10^-19N#

So

#m4pi^2n^2r=F#
#=>n^2=F/(4pi^2xxmxxr)#
#=>n=sqrt(F/(4pi^2xxmxxr))#
#=sqrt((1.02xx10^-19N)/(4pi^2xx9.1xx10^-31kgxx4.76xx10^-10m))#
#=3.74xx10^8Hz#
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Answer 2

The frequency of the electron's revolutions can be calculated using the formula:

[ f = \frac{v}{2\pi r} ]

Where ( f ) is the frequency, ( v ) is the velocity of the electron, and ( r ) is the radius of its orbit.

The velocity of the electron can be determined using the centripetal force equation:

[ F = \frac{mv^2}{r} ]

Solving for ( v ):

[ v = \sqrt{\frac{Fr}{m}} ]

Substituting the given values:

[ v = \sqrt{\frac{(1.02 \times 10^{-9} , N) \times (4.76 \times 10^{-10} , m)}{9.10 \times 10^{-31} , kg}} ]

[ v \approx 2.19 \times 10^6 , m/s ]

Now, substituting ( v ) into the frequency formula:

[ f = \frac{2.19 \times 10^6 , m/s}{2 \pi \times 4.76 \times 10^{-10} , m} ]

[ f \approx 3.67 \times 10^{15} , Hz ]

So, the electron makes approximately ( 3.67 \times 10^{15} ) revolutions per second.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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