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2. Calculation of the number of quanta for heating:

Given:

Frequency (take the upper threshold of microwave radiation):

f = 300 GHz

Solving:

Change in body heat when exposed to quanta:

(7)

Hence, the number of quanta required to heat the body to a certain temperature:

= (8)

Quantum energy (1):

Calculate the number of quanta needed to heat the body in everyday life:

Let's calculate the number of quanta needed to heat the body in production:

We conclude that the number of quanta needed to heat the body in production is / = 7 times greater than the number of quanta needed for heating in everyday life.

Answer:

Body temperature change in everyday life: ;

Body temperature change in production: ;

The number of quanta for heating in everyday life: ;

The number of quanta for heating in production: ;

0.75 балл

Task №3

3. Compare numerically 2 typical devices: vacuum and semiconductor according to the following parameters:

3.1 The maximum velocity of charged particles.

3.2 The length of the interaction region for the angle of flight-radian.

3.3 Volumetric charge density

3.4 Calculate the microperviance, the «plasma» frequency for the vacuum device.

3.5 For semiconductor: Debye length, plasma frequency.

Compare the values in clauses 4.4. and 4.5. Explain the difference in physical processes in both variants.

Parameters of the vacuum device: current 120 mA, accelerating voltage 5,2 kV, flow diameter 14 mm.

Semiconductor: doping level 6 1016 cm-3, voltage 20 V, current channel thickness 1 microns.

The operating frequency of the devices is 13 GHz.

The operating temperature is 306 K.

Given:

Parameters of the vacuum device:

IV = 120 mA

UV = 5,2 kV

d = 14 mm = 0,014 m

Parameters of a semiconductor device:

n = 6 1016 cm-3 = 6 1022 m-3

US = 20 V

h = 1 = 10-6 m

Operating frequency of both devices:

f = 13 GHz

Operating temperature of both devices:

T = 306 K

Solving:

1. Numerical comparison of the maximum velocities of charged particles:

1.1 Vacuum device:

According to the formula [11]:

VVmax = (9)

where q - electron charge; m - electron mass; UV – accelerating voltage.

We get the following value:

VVmax = = = 4,276 107 m/s

1.2 Semiconductor device:

Field strength:

E = = = 200 kV/cm

So, the maximum speed corresponds to the saturation current [12]:

VSmax = Vsat= 105 m/s

Thus, the maximum velocity of charged particles in a vacuum device is 4,276 107/105 = 428 times greater than in a semiconductor device.

2. Numerical comparison of the length of the interaction region for the span angle of π - radians:

2.1 Vacuum device:

The formula of the span angle [13]:

= = (10)

where f – frequency; lV - the length of the interaction area; vV - flight speed.

Hence, the length of the interaction area:

lВ = = = = = = 0,00164 m

2.2 Semiconductor device:

lS = = = = = = 3,846 10-6 m

That is, the length of the interaction region of the vacuum device is 0,00164/3,846 10-6 = 426 times longer.

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