問題一覧
1
This is called the law of presensmission since the resure apple ate poet transmitted to all points in the fluid.
2
16. 10 beth With the weich W aloaded on the piaton 4 (cross setio of the container with water in.
3
If W' = 100W for weights then the relation S' = 100S is true for the cross section.
4
In piston B, the centuple force given in piston A will arise.
5
This principle is applied to hydraulic system, etc.
6
In 1662 R. Boyle, Irish physicist, discovered experimentally that the pressure P of a gas is inversely proportional to its volume
7
Around i87 the French scientia SA Charles Bund that the volime V ofa gas is proportional to its absolute temperature 1.
8
These facts are true only of ideal gas or perfect gas and sive t I give the following equation of state, or Boyle-Charl law:
9
where R is the gas constant and 1 is the specific volume of the gas.
10
If these three variables in Eq. (17.1) are plotted along three mutually perpendicular axes, the equation defines a P -v-T surface as shown in Fig. 17.
11
Every possible equilibrium state of an ideal gas is represented by a point and a quasi static process by a line on the surface, as well.
12
In 1824, French physicist N. L. S. Carnot (1796-1832) planned the most efficient cycle of operation for a heat engine.
13
In his cycle four reversible processes: (1) isothermal expansion at thermodynamic temperature T1 with heat 8, caken up: 2 adiabaticenpanaton withatemperatur flt 7,6 othermal onpreso at 1, with hea 2, rejece la adiabatie compresion with a tonperature riee back to T
14
Obeying the first law of thermodynamics and the definition of efficiency n, we can conclude that n = 1 02/01 = 1 - Tz/Ts then Tr/T, = Q1/Q2.
15
Consequently, Is said that t he efficiency of an ideal reversibleheat engine depend only upon the temperature range through (which (it) works and not on the properties of the working substances used
16
When the ray A reaches incidence point O on the boundary surface between medium I and II, part of fit (the ray B) is reflected to the medium I and the rest (the ray C) is refracted into the medium II (see Fig. 19).
17
The sạy to caled the nden a 1 the relected one and the refracted one.
18
The ray A is caled the incident ray, B the reflected one and C the refracted one. The angle between the normal ine l and the incident ray on the boundary surfače is called the incidence angle i, and the angle between the line l and the reflected one is similarly called the reflection angle , and the angle between the line l and the refracted ray C is called the refraction angle k. The rays A. B C and
19
The rays A, B, C and the line l are in the identical in plane, and the following equations follow:
20
And Lq. 19. 2） is called the law of retraction anrefractive index for medium I to II.
21
The phenomenon that） waves such as sound and light do not go straight ahead but turn into the shadow of the obstacle is called dittraction
22
in Fig. 20, a monochromatic light is applied to slit S and the light leaving S is perpendicularly emitted at two parallel slits of S1 and S2.
23
The light passing S1 and Sz makes a tringe pattern on the screen, at a distance l, by the interference of the light dark.
24
(This) is because the light difracted at S reaches S and S, and the ones diffracted at those slits interfere with each other.
25
that is to say, if an optical path difference of the light coming out of S, and S2 is an even number times a half wave length 1/2) of light, it intensifies each other and leads to the brightness in the fringe pattern as shown in Eq. (20.1).
26
When an optical path difference is an odd number times a half wave length of fit), the fringe pattern darkens as a result of turning down the light for each other, as shown in Eq. (20.2).
27
Example based on the there en o ght are the color i i spreading on a water surface and the striped pattern of concentric circles in Newton rings.
28
When the structure of pure metal is examined, its atoms range very regularly.
29
The arrangement of these atoms is called the crystal structure.
30
If the atomic center points are connected, it becomes a solid crystal lattice.
31
(a) face-centered cubic lattice; in (which) the atom is put on each top and center of every face in the cube, (b)body centered cubic lattice; in (which) the atom is put on each top and center in the cube, it) is the simnplest crystal structure of the three types, (c) hexagonal closepacked lattice; in (which) the atom is put on eåch top and center of the upper and lower surfaces in the regular hexagonal S1
32
When an ultraviolet ray is put on the metal plate of a leaf electroscope, it is observed that the foil gradually opens as shown Fig. 22. It is shown that the electric charge is produced in this foil.
33
The positive electric 正の電A 會I# charge is observed when this foil is examined.
34
This phenomenon occurs because the negative electron is projected from the surface of the metal plate.
35
This phenomenon occurs because the negative electron is projected from the surface of the metal plate.
36
The phenomenon (which) produces free electron (photoelectron) 01 by the material absorbing light is called the photoelectric effect.
37
t) is confirmed by the expertment in (which) the light is put with various wavelengths onto the metal surface.
38
The photoelectron is discharged regardless of the intensity of the light, if is over the limitative frequency va in which) the frequency of the light is determined by the metallic type. This approach was inherited by Einstein and developed as a concept of the light quantum in later years.
39
This approach was inherited by Einstein and developed as a concept of the light quantum in later years.
40
This principle is applied to the phototube and to the photoelectriaity microscope (which) measure slight V1 displacement.
41
The equipment (which) changes alternating voltage using mutual induction is called a transformer.The equipment (which) changes alternating voltage using mutual induction is called a transformer.
42
Two coils are wound around an iron core as shown in Fig. 23.
43
When alternating voltage is applied to the primary coil, it is induced in the secondary coil.
44
The relation between the effective voltage VIV] given to the primary coil (winding number n1 ) and the voltage VIV] rising in the secondary coil (winding number nz ) is shown in the following equation:
45
When the external load is connected to the secondary coil, the effective current i flows in (it) and the effective current 4 flows in the primary coil.
46
Then, the electric power which) enters the primary coil and goes to the secondary (one) is the same, and the following equation is given:
47
The circuit of a Wheatstone Bridge is used to measure a resistance value precisely.
48
The known variable resistors R1. R2. Ry and the unknown resistance R, are connected as shown in Fig. 24.
49
In addition, a galvanometer G, a batttery E, and a switch S are connected and § is closed.
50
The resistor Ra is adiusted so that the current may not flow into the galvanometer G at this time.
51
When the currents flowing into the resistors Ry and Rz are i and i respectively, the currents i and is also flow into the resistors Re and Re severally since (they) do not flow into the galvanometer G.
52
The voltage drops (AV = iR) from A to C and from A to D become equal since the points C and D are equipotential.
53
By substituting the value of the known resistors R1, Rz and R3 into Eq. (24.1), the unknown value Ro can be decided.
54
This principle is also applied to the alternating current bridge (which) measures the electric capacity and to the Kohlrausch bridge measuring the resistance of electrolytic solution.
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はやちゃん · 26問 · 1年前文学特論
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26問 • 1年前問題一覧
1
This is called the law of presensmission since the resure apple ate poet transmitted to all points in the fluid.
2
16. 10 beth With the weich W aloaded on the piaton 4 (cross setio of the container with water in.
3
If W' = 100W for weights then the relation S' = 100S is true for the cross section.
4
In piston B, the centuple force given in piston A will arise.
5
This principle is applied to hydraulic system, etc.
6
In 1662 R. Boyle, Irish physicist, discovered experimentally that the pressure P of a gas is inversely proportional to its volume
7
Around i87 the French scientia SA Charles Bund that the volime V ofa gas is proportional to its absolute temperature 1.
8
These facts are true only of ideal gas or perfect gas and sive t I give the following equation of state, or Boyle-Charl law:
9
where R is the gas constant and 1 is the specific volume of the gas.
10
If these three variables in Eq. (17.1) are plotted along three mutually perpendicular axes, the equation defines a P -v-T surface as shown in Fig. 17.
11
Every possible equilibrium state of an ideal gas is represented by a point and a quasi static process by a line on the surface, as well.
12
In 1824, French physicist N. L. S. Carnot (1796-1832) planned the most efficient cycle of operation for a heat engine.
13
In his cycle four reversible processes: (1) isothermal expansion at thermodynamic temperature T1 with heat 8, caken up: 2 adiabaticenpanaton withatemperatur flt 7,6 othermal onpreso at 1, with hea 2, rejece la adiabatie compresion with a tonperature riee back to T
14
Obeying the first law of thermodynamics and the definition of efficiency n, we can conclude that n = 1 02/01 = 1 - Tz/Ts then Tr/T, = Q1/Q2.
15
Consequently, Is said that t he efficiency of an ideal reversibleheat engine depend only upon the temperature range through (which (it) works and not on the properties of the working substances used
16
When the ray A reaches incidence point O on the boundary surface between medium I and II, part of fit (the ray B) is reflected to the medium I and the rest (the ray C) is refracted into the medium II (see Fig. 19).
17
The sạy to caled the nden a 1 the relected one and the refracted one.
18
The ray A is caled the incident ray, B the reflected one and C the refracted one. The angle between the normal ine l and the incident ray on the boundary surfače is called the incidence angle i, and the angle between the line l and the reflected one is similarly called the reflection angle , and the angle between the line l and the refracted ray C is called the refraction angle k. The rays A. B C and
19
The rays A, B, C and the line l are in the identical in plane, and the following equations follow:
20
And Lq. 19. 2） is called the law of retraction anrefractive index for medium I to II.
21
The phenomenon that） waves such as sound and light do not go straight ahead but turn into the shadow of the obstacle is called dittraction
22
in Fig. 20, a monochromatic light is applied to slit S and the light leaving S is perpendicularly emitted at two parallel slits of S1 and S2.
23
The light passing S1 and Sz makes a tringe pattern on the screen, at a distance l, by the interference of the light dark.
24
(This) is because the light difracted at S reaches S and S, and the ones diffracted at those slits interfere with each other.
25
that is to say, if an optical path difference of the light coming out of S, and S2 is an even number times a half wave length 1/2) of light, it intensifies each other and leads to the brightness in the fringe pattern as shown in Eq. (20.1).
26
When an optical path difference is an odd number times a half wave length of fit), the fringe pattern darkens as a result of turning down the light for each other, as shown in Eq. (20.2).
27
Example based on the there en o ght are the color i i spreading on a water surface and the striped pattern of concentric circles in Newton rings.
28
When the structure of pure metal is examined, its atoms range very regularly.
29
The arrangement of these atoms is called the crystal structure.
30
If the atomic center points are connected, it becomes a solid crystal lattice.
31
(a) face-centered cubic lattice; in (which) the atom is put on each top and center of every face in the cube, (b)body centered cubic lattice; in (which) the atom is put on each top and center in the cube, it) is the simnplest crystal structure of the three types, (c) hexagonal closepacked lattice; in (which) the atom is put on eåch top and center of the upper and lower surfaces in the regular hexagonal S1
32
When an ultraviolet ray is put on the metal plate of a leaf electroscope, it is observed that the foil gradually opens as shown Fig. 22. It is shown that the electric charge is produced in this foil.
33
The positive electric 正の電A 會I# charge is observed when this foil is examined.
34
This phenomenon occurs because the negative electron is projected from the surface of the metal plate.
35
This phenomenon occurs because the negative electron is projected from the surface of the metal plate.
36
The phenomenon (which) produces free electron (photoelectron) 01 by the material absorbing light is called the photoelectric effect.
37
t) is confirmed by the expertment in (which) the light is put with various wavelengths onto the metal surface.
38
The photoelectron is discharged regardless of the intensity of the light, if is over the limitative frequency va in which) the frequency of the light is determined by the metallic type. This approach was inherited by Einstein and developed as a concept of the light quantum in later years.
39
This approach was inherited by Einstein and developed as a concept of the light quantum in later years.
40
This principle is applied to the phototube and to the photoelectriaity microscope (which) measure slight V1 displacement.
41
The equipment (which) changes alternating voltage using mutual induction is called a transformer.The equipment (which) changes alternating voltage using mutual induction is called a transformer.
42
Two coils are wound around an iron core as shown in Fig. 23.
43
When alternating voltage is applied to the primary coil, it is induced in the secondary coil.
44
The relation between the effective voltage VIV] given to the primary coil (winding number n1 ) and the voltage VIV] rising in the secondary coil (winding number nz ) is shown in the following equation:
45
When the external load is connected to the secondary coil, the effective current i flows in (it) and the effective current 4 flows in the primary coil.
46
Then, the electric power which) enters the primary coil and goes to the secondary (one) is the same, and the following equation is given:
47
The circuit of a Wheatstone Bridge is used to measure a resistance value precisely.
48
The known variable resistors R1. R2. Ry and the unknown resistance R, are connected as shown in Fig. 24.
49
In addition, a galvanometer G, a batttery E, and a switch S are connected and § is closed.
50
The resistor Ra is adiusted so that the current may not flow into the galvanometer G at this time.
51
When the currents flowing into the resistors Ry and Rz are i and i respectively, the currents i and is also flow into the resistors Re and Re severally since (they) do not flow into the galvanometer G.
52
The voltage drops (AV = iR) from A to C and from A to D become equal since the points C and D are equipotential.
53
By substituting the value of the known resistors R1, Rz and R3 into Eq. (24.1), the unknown value Ro can be decided.
54
This principle is also applied to the alternating current bridge (which) measures the electric capacity and to the Kohlrausch bridge measuring the resistance of electrolytic solution.