English, asked by virenderdhanda2019, 15 days ago

What please you on the river

Answers

Answered by isabellacarter681
0

Answer:

is this a question ⁉️⁉️

please type it properly

and foll.w me

and mark me as brainiest

Answered by pmynameiswolf
0

I don't know water?

hah kidding what pleases me is The top-most layer of the Seven Layers of Open Systems Interconnection (OSI) Model is the Application Layer and the bottom-most layer of the Seven Layers of Open Systems Interconnection (OSI) Model is Physical LayerWhat is the 1st and last layer of OSI modelthe value of the limit lim(x-->o){x/sinx}1/x2e

1

6

Explanation:

sin

x

=

x

x

3

3

!

+

x

5

5

!

+

x

7

7

!

+

this is an alternate series and if

|

x

|

<

1

x

x

3

3

!

x

<

sin

x

x

<

x

x

3

3

!

+

x

5

5

!

x

lim

x

0

x

x

3

3

!

x

1

x

2

=

lim

x

0

(

1

x

2

6

)

1

x

2

but making

y

=

x

2

6

lim

x

0

(

1

x

2

6

)

1

x

2

=

lim

y

0

(

(

1

+

y

)

1

y

)

1

6

=

e

1

6

analogously

lim

x

0

x

x

3

3

!

+

x

5

5

!

x

1

x

2

=

lim

x

0

(

1

x

2

3

!

+

x

4

5

!

)

1

x

2

=

e

1

6

The Bohr theory of the atom has a number of severe limitations.

o It applies only to hydrogen and one-electron ions such as He+

and Li+2

.

o It cannot explain why certain spectral lines are more intense than others (that is, why

certain transitions between energy levels have greater probabilities of occurrence than

others).

o It cannot account for the observation that many spectral lines actually consist of several

separate lines whose wavelengths differ slightly.

o Perhaps most important, it does not permit us to obtain an understanding of how

individual atoms interact with one another to endow macroscopic aggregates of matter

with the physical and chemical properties we observe.

• A more general approach to atomic phenomena is required. Such an approach was

developed in 1925 and 1926 by Erwin Schrödinger, Werner Heisenberg, Max Born, Paul

Dirac, and others under the name of quantum mechanics.

5.1 QUANTUM MECHANICS

• Classical mechanics is an approximation of quantum mechanics

• The fundamental difference between classical (or Newtonian) mechanics and quantum

mechanics lies in what they describe.

o In classical mechanics, the future history of a particle is completely determined by its

initial position and momentum together with the forces that act upon it.

o Quantum mechanics also arrives at relationships between observable quantities, but the

uncertainty principle suggests that the nature of an observable quantity is different in the

atomic realm.

• In quantum mechanics, the kind of certainty about the future characteristic of classical

mechanics is impossible because the initial state of a particle cannot be established with

sufficient accuracy.

o The more we know about the position of a particle now, the less we know about its

momentum and hence about its position later.

• The quantities whose relationships quantum mechanics explores are probabilities.

o The Bohr theory states the radius of the electron’s orbit in a ground state hydrogen atom

is always exactly 5.3x10-11 m.

o Quantum mechanics states that this is the most probable radius. In a suitable experiment,

most trials will yield a different value, either larger or smaller, but the value most likely

to be found will be 5.3x10-11 m.

Wave Function

• The quantity with which quantum mechanics is concerned is the wave function Ψ of a body.

• The linear momentum, angular momentum, and energy of the body are other quantities that

can be established from Ψ.

• The problem of quantum mechanics is to determine Ψ for a body when its freedom of

motion is limited by the action of external forces.

• Wave functions are usually complex with both real and imaginary parts.

where A and B are real functions.

• A probability, however, must be a positive real quantity. The probability density |Ψ|2

for a

complex is therefore taken as the product of Ψ and its complex conjugate Ψ* which is Ψ*Ψ.

• The complex conjugate of any function is obtained by replacing i by -i wherever it appears

in the function.

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