GRADE 11 PRACTICE
Physics Problems: Optics, Grade 11
Reflection, refraction, lenses and diffraction.
Here the conditions and analysis of the solution can be read without an account. In the simulator, you need to collect the same analyzes yourself: “Given,” formulas, order of steps and answer.
Problem statements
The answer options are there to check against, and the walkthrough opens under each problem.
Problem #37
Geometric opticsBeam angle 40^{\circ}, refractive index of the medium 1{,}5. What is the angle of refraction? Light falls from the air; take its refractive index equal to 1.
Show the walkthroughHide the walkthrough
- \alpha
- 40^{\circ}
- n
- 1{,}5
\beta - ?
- n = \dfrac{\sin\alpha}{\sin\beta}\ \Rightarrow\ \sin\beta = \dfrac{\sin\alpha}{n}\dfrac{\sin 40^{\circ}}{1{,}5} = \dfrac{0{,}643}{1{,}5}\sin\beta = 0{,}4285
- \beta = \arcsin 0{,}4285\beta = 25{,}4^{\circ}
Answer\beta = 25{,}4^{\circ}
Problem #38
Lenses, interference and diffractionDistance from an object to an image of equal size 80\,\text{см}. Determine the focal length and optical power of the lens.
Show the walkthroughHide the walkthrough
- S
- 80\,\text{см}
- \Gamma
- 1
F - ?D - ?
- \Gamma = \dfrac{f}{d} = 1\ \Rightarrow\ f = d
The image is equal to the object only at d = 2F.
- \dfrac{1}{F} = \dfrac{1}{d} + \dfrac{1}{f} = \dfrac{2}{d}\ \Rightarrow\ d = 2F,\ f = 2F
- S = d + f = 4F\ \Rightarrow\ F = \dfrac{S}{4}F = \dfrac{80}{4}F = 20\,\text{см} = 0{,}2\,\text{м}
- D = \dfrac{1}{F}D = \dfrac{1}{0{,}2}D = 5\,\text{дптр}
AnswerF = 0{,}2\,\text{м}D = 5\,\text{дптр}
Problem #41
Geometric opticsHeight of the Sun above the horizon 20^{\circ}. At what angle to the horizon should a mirror be placed to illuminate the bottom of a vertical well?
Show the walkthroughHide the walkthrough
- h_{\odot}
- 20^{\circ}
- \alpha
- 70^{\circ}
\beta - ?
- \alpha_1 = \gamma_1 = \dfrac{90^{\circ} + 20^{\circ}}{2}\beta = 55^{\circ}
The beam must go vertically downwards, so the angle between the incident and reflected rays is 110°.
- \beta = \gamma\beta = 55^{\circ}
Angles with mutually perpendicular sides are equal: the mirror is placed at 55° to the horizon.
Answer\beta = 55^{\circ}
Problem #42
Geometric opticsAt angle of incidence 40^{\circ} the angle of refraction is 24^{\circ}. Determine the refractive index, the speed of light in the substance, and the limiting angle of total internal reflection. What will happen at the angle of incidence 40^{\circ} from matter into air?
Show the walkthroughHide the walkthrough
- \alpha
- 40^{\circ}
- \beta
- 24^{\circ}
- \beta_2
- 40^{\circ}
- c
- 3\cdot 10^{8}\,\text{м/с}
n - ?c_{\text{в}} - ?\alpha_0 - ?\alpha_2 - ?
- n = \dfrac{\sin\alpha}{\sin\beta}\dfrac{\sin 40^{\circ}}{\sin 24^{\circ}} = \dfrac{0{,}6428}{0{,}4067}n = 1{,}58
- c_{\text{в}} = \dfrac{c}{n}c_{\text{в}} = \dfrac{3\cdot 10^{8}}{1{,}58}c_{\text{в}} = 1{,}9\cdot 10^{8}\,\tfrac{\text{м}}{\text{с}}
- \sin\alpha_0 = \dfrac{1}{n}\sin\alpha_0 = \dfrac{1}{1{,}58}\alpha_0 = 0{,}6328\ \Rightarrow\ \alpha_0 = 39{,}3^{\circ}
Limiting angle of total reflection.
- \sin\alpha_2 = n\sin\beta_2\sin\alpha_2 = 1{,}58\cdot 0{,}64281{,}0156 > 1
There is no angle of incidence with 40° refraction: the maximum angle of refraction is 39.3°, and this is achieved at 90° incidence.
Answern = 1{,}58c_{\text{в}} = 1{,}9\cdot 10^{8}\,\tfrac{\text{м}}{\text{с}}\alpha_0 = 39{,}3^{\circ}\text{When fall from substances B air at an angle 40° is happening Total internal reflection}
Problem #43
Geometric opticsWhat must be the refractive index of a substance so that the reflected and refracted rays make an angle? 90^{\circ}? Express your answer in terms of the angle of incidence \alpha. Light falls from the air; take the refractive index of air equal to 1.
Show the walkthroughHide the walkthrough
- \beta + \gamma
- 90^{\circ}
n - ?
- n = \dfrac{\sin\alpha}{\sin\beta} = \dfrac{\sin\alpha}{\sin\left(90^{\circ} - \alpha\right)}
The angle of reflection is equal to the angle of incidence, therefore, when the rays are perpendicular, β = 90° − α.
- n = \dfrac{\sin\alpha}{\cos\alpha} = \operatorname{tg}\alphan = \operatorname{tg}\alpha
For example, at α = 60° you get n = tan 60° ≈ 1.73.
Answern = \operatorname{tg}\alpha
Problem #44
Lenses, interference and diffractionThe object is at a distance 20\,\text{см} from the lens, the image in 3 times the size of the item. Determine the possible focal lengths and optical powers for real and virtual images.
Show the walkthroughHide the walkthrough
- d
- 20\,\text{см}
- \Gamma
- 3
F_1 - ?D_1 - ?F_2 - ?D_2 - ?
- \Gamma = \dfrac{\left|f\right|}{d}\ \Rightarrow\ \left|f\right| = \Gamma d\left|f\right| = 3\cdot 20\left|f\right| = 60\,\text{см}
- \dfrac{1}{F} = \dfrac{1}{d} + \dfrac{1}{f}\ \Rightarrow\ F = \dfrac{df}{d + f}
- F_1 = \dfrac{20\cdot 60}{20 + 60}F_1 = 15\,\text{см} = 0{,}15\,\text{м}
The image is valid.
- D_1 = \dfrac{1}{F_1}D_1 = \dfrac{1}{0{,}15}D_1 = 6{,}67\,\text{дптр}
- F_2 = \dfrac{20\cdot\left(-60\right)}{20 + \left(-60\right)}F_2 = 30\,\text{см} = 0{,}3\,\text{м}
The image is imaginary - for it f is taken with a minus sign.
- D_2 = \dfrac{1}{F_2}D_2 = \dfrac{1}{0{,}3}D_2 = 3{,}33\,\text{дптр}
AnswerF_1 = 15\,\text{см}D_1 = 6{,}67\,\text{дптр}F_2 = 30\,\text{см}D_2 = 3{,}33\,\text{дптр}
Problem #45
Lenses, interference and diffractionConverging lens with focal length 20\,\text{см} gives an image enlarged by 5 times. Find the distance between the object and the image: a) for a real image; b) for imaginary. Then find this distance if the actual image is reduced in 5 times.
Show the walkthroughHide the walkthrough
- F
- 20\,\text{см}
- \Gamma
- 5
- \Gamma_2
- \dfrac{1}{5}
S_1 - ?S_2 - ?S_3 - ?
- \dfrac{1}{F} = \dfrac{1}{d} + \dfrac{1}{\Gamma d} = \dfrac{\Gamma + 1}{\Gamma d}\ \Rightarrow\ d_1 = \dfrac{F\left(\Gamma + 1\right)}{\Gamma}d_1 = \dfrac{20\left(5 + 1\right)}{5}d_1 = 24\,\text{см}
- f_1 = \Gamma d_1,\quad S_1 = d_1 + f_1f_1 = 120\,\text{см};\quad S_1 = 24 + 120S_1 = 144\,\text{см}
Real image: object and image on opposite sides of the lens.
- \dfrac{1}{F} = \dfrac{1}{d} - \dfrac{1}{\Gamma d} = \dfrac{\Gamma - 1}{\Gamma d}\ \Rightarrow\ d_2 = \dfrac{F\left(\Gamma - 1\right)}{\Gamma}d_2 = \dfrac{20\left(5 - 1\right)}{5}d_2 = 16\,\text{см}
- S_2 = \left|f_2\right| - d_2S_2 = 80 - 16S_2 = 64\,\text{см}
Virtual image: it is on the same side as the object.
- \Gamma_2 = \dfrac{1}{5}:\quad d_3 = \dfrac{F\left(\Gamma_2 + 1\right)}{\Gamma_2}\dfrac{20\cdot 1{,}2}{0{,}2} = 120\,\text{см};\quad f_3 = 24\,\text{см}S_3 = 144\,\text{см}
Zooming out by 5 times is the same scheme as zooming in, only the object and image are swapped.
AnswerS_1 = 144\,\text{см}S_2 = 64\,\text{см}S_3 = 144\,\text{см}
Problem #46
Lenses, interference and diffractionCoherent waves with a frequency interfere in the air 5\cdot10^{14}\,\text{Гц}. The light will increase or decrease at a point with a path difference 2{,}4\,\text{мкм}? The sources are in phase, the wave polarizations are the same.
Show the walkthroughHide the walkthrough
- \nu
- 5\cdot 10^{14}\,\text{Гц}
- \Delta d
- 2{,}4\cdot 10^{-6}\,\text{м}
- c
- 3\cdot 10^{8}\,\text{м/с}
\dfrac{\Delta d}{\lambda/2} - ?
- \lambda = \dfrac{c}{\nu}\lambda = \dfrac{3\cdot 10^{8}}{5\cdot 10^{14}}6\cdot 10^{-7}\,\text{м}\ \Rightarrow\ \dfrac{\lambda}{2} = 3\cdot 10^{-7}\,\text{м}
- \dfrac{\Delta d}{\lambda/2}\dfrac{\Delta d}{\lambda/2} = \dfrac{2{,}4\cdot 10^{-6}}{3\cdot 10^{-7}}\dfrac{\Delta d}{\lambda/2} = 8
An even number of half-waves means the light will intensify: this is the maximum.
Answer\dfrac{\Delta d}{\lambda/2} = 8\ \text{- свет усилится}
Problem #47
Lenses, interference and diffractionOn a diffraction grating with a period 1/200\,\text{мм} Monochromatic light falls normally. The third order maximum is visible at an angle 17{,}5^{\circ}. Find the wavelength in air and the wavelength and speed of light in glass with n=1{,}5, as well as the original frequency. Then find the wavelengths in air and glass at twice the frequency, assuming the refractive index remains constant.
Show the walkthroughHide the walkthrough
- d
- \dfrac{1}{200}\,\text{мм}=0{,}005\cdot 10^{-3}\,\text{м}
- k
- 3
- \alpha
- 17{,}5^{\circ}
- n
- 1{,}5
- \nu_1
- 2\nu
\lambda - ?\lambda_{\text{ст}} - ?c_{\text{ст}} - ?\nu - ?\lambda_1 - ?\lambda_{1\text{ст}} - ?
- d\sin\alpha = k\lambda\ \Rightarrow\ \lambda = \dfrac{d\sin\alpha}{k}\lambda = \dfrac{0{,}005\cdot 10^{-3}\cdot\sin 17{,}5^{\circ}}{3}\lambda = 5\cdot 10^{-7}\,\text{м}
- \lambda_{\text{ст}} = \dfrac{\lambda}{n}\lambda_{\text{ст}} = \dfrac{5\cdot 10^{-7}}{1{,}5}\lambda_{\text{ст}} = 3{,}33\cdot 10^{-7}\,\text{м}
- c_{\text{ст}} = \dfrac{c}{n}c_{\text{ст}} = \dfrac{3\cdot 10^{8}}{1{,}5}c_{\text{ст}} = 2\cdot 10^{8}\,\tfrac{\text{м}}{\text{с}}
- \nu = \dfrac{c}{\lambda}\nu = \dfrac{3\cdot 10^{8}}{5\cdot 10^{-7}}\nu = 6\cdot 10^{14}\,\text{Гц}
The frequency does not change when passing into glass - the speed and wavelength change.
- \lambda_1 = \dfrac{c}{\nu_1} = \dfrac{c}{2\nu} = \dfrac{\lambda}{2}\lambda_1 = \dfrac{5\cdot 10^{-7}}{2}\lambda_1 = 2{,}5\cdot 10^{-7}\,\text{м}
Doubling the frequency shortens the wave by half - this is ultraviolet.
- \lambda_{1\text{ст}} = \dfrac{\lambda_1}{n}\lambda_{1\text{ст}} = \dfrac{2{,}5\cdot 10^{-7}}{1{,}5}\lambda_{1\text{ст}} = 1{,}67\cdot 10^{-7}\,\text{м}
Answer\lambda = 5\cdot 10^{-7}\,\text{м}\lambda_{\text{ст}} = 3{,}33\cdot 10^{-7}\,\text{м}c_{\text{ст}} = 2\cdot 10^{8}\,\tfrac{\text{м}}{\text{с}}\nu = 6\cdot 10^{14}\,\text{Гц}\lambda_1 = 2{,}5\cdot 10^{-7}\,\text{м}\lambda_{1\text{ст}} = 1{,}67\cdot 10^{-7}\,\text{м}
Problem #48
Lenses, interference and diffractionThe diffraction grating has 85 cracks on 1\,\text{мм}. What is the angle between the second order purple maxima at \lambda=4\cdot10^{-7}\,\text{м}?
Show the walkthroughHide the walkthrough
- d
- \dfrac{1}{85}\,\text{мм}=1{,}176\cdot 10^{-5}\,\text{м}
- k
- 2
- \lambda
- 4\cdot 10^{-7}\,\text{м}
\gamma - ?
- d\sin\alpha = k\lambda\ \Rightarrow\ \sin\alpha = \dfrac{k\lambda}{d}\sin\alpha = \dfrac{2\cdot 4\cdot 10^{-7}}{1{,}176\cdot 10^{-5}}\sin\alpha = 0{,}068
- \alpha = \arcsin 0{,}068\alpha = 3{,}9^{\circ}
- \gamma = 2\alpha\gamma = 2\cdot 3{,}9\gamma = 7{,}8^{\circ}
The maxima are symmetrical about the center, so the angle between them is twice as large.
Answer\gamma = 7{,}8^{\circ}
Problem #49
Lenses, interference and diffractionFocal length of the projection lamp lens 15\,\text{см}. The slide is at a distance 15{,}6\,\text{см} from the lens. What linear magnification does the flashlight provide?
Show the walkthroughHide the walkthrough
- F
- 15\,\text{см}
- d
- 15{,}6\,\text{см}
\Gamma - ?
- \dfrac{1}{F} = \dfrac{1}{d} + \dfrac{1}{f}\ \Rightarrow\ f = \dfrac{dF}{d - F}f = \dfrac{15{,}6\cdot 15}{15{,}6 - 15}f = 390\,\text{см}
- \Gamma = \dfrac{f}{d}\Gamma = \dfrac{390}{15{,}6}\Gamma = 25
The slide is placed a little further from the focus - then the image turns out large and real.
Answer\Gamma = 25
Problem #52
Lenses, interference and diffractionAt a distance 1{,}5\,\text{м} from the screen there is a diffraction grating with a period 20\,\text{мкм}. At what distance from the central maximum is the second-order violet maximum at \lambda=4\cdot10^{-7}\,\text{м}?
Show the walkthroughHide the walkthrough
- L
- 1{,}5\,\text{м}
- d
- 20\,\text{мкм}=20\cdot 10^{-6}\,\text{м}
- k
- 2
- \lambda
- 4\cdot 10^{-7}\,\text{м}
\ell - ?
- d\sin\alpha = k\lambda,\quad \sin\alpha \approx \operatorname{tg}\alpha = \dfrac{\ell}{L}
The angles are small, so the sine can be replaced by a tangent.
- \dfrac{d\ell}{L} = k\lambda\ \Rightarrow\ \ell = \dfrac{k\lambda L}{d}\ell = \dfrac{2\cdot 4\cdot 10^{-7}\cdot 1{,}5}{20\cdot 10^{-6}}\ell = 0{,}06\,\text{м} = 6\,\text{см}
Answer\ell = 0{,}06\,\text{м}
Problem #122
Reflection and refraction of lightRefractive index of the medium 1{,}5. Speed of light in vacuum 300000000 m/s. Find the speed of light in the medium.
Show the walkthroughHide the walkthrough
- n
- 1{,}5\,\text{безразм.}
- c
- 300000000\,\text{м/с}
v - ?
- v=\frac{c}{n}v=\frac{300000000}{1{,}5}v=200000000\,\text{м/с}
The refractive index shows the slowing down of light.
Answer200000000\,\text{м/с}
Problem #123
Reflection and refraction of lightRefractive index of the medium 2. Speed of light in vacuum 300000000 m/s. Find the speed of light in the medium.
Show the walkthroughHide the walkthrough
- n
- 2\,\text{безразм.}
- c
- 300000000\,\text{м/с}
v - ?
- v=\frac{c}{n}v=\frac{300000000}{2}v=150000000\,\text{м/с}
The refractive index shows the slowing down of light.
Answer150000000\,\text{м/с}
Problem #124
Reflection and refraction of lightWhen passing from air to medium, the sine of the angle of incidence 0{,}6, sine of the angle of refraction 0{,}4. Find the speed of light in the medium; c = 300000000 m/s, air index is 1.
Show the walkthroughHide the walkthrough
- a
- 0{,}6\,\text{безразм.}
- b
- 0{,}4\,\text{безразм.}
- c
- 300000000\,\text{м/с}
v - ?
- n=\frac{\sin\alpha}{\sin\beta}n=\frac{0{,}6}{0{,}4}n=1{,}5\,\text{безразм.}
The law of refraction relates the sines of angles.
- v=\frac{c}{n}v=\frac{300000000}{1{,}5}v=200000000\,\text{м/с}
We find the speed from the refractive index.
Answer200000000\,\text{м/с}
Problem #125
Reflection and refraction of lightWhen passing from air to medium, the sine of the angle of incidence 0{,}8, sine of the angle of refraction 0{,}4. Find the speed of light in the medium; c = 300000000 m/s, air index is 1.
Show the walkthroughHide the walkthrough
- a
- 0{,}8\,\text{безразм.}
- b
- 0{,}4\,\text{безразм.}
- c
- 300000000\,\text{м/с}
v - ?
- n=\frac{\sin\alpha}{\sin\beta}n=\frac{0{,}8}{0{,}4}n=2\,\text{безразм.}
The law of refraction relates the sines of angles.
- v=\frac{c}{n}v=\frac{300000000}{2}v=150000000\,\text{м/с}
We find the speed from the refractive index.
Answer150000000\,\text{м/с}
Problem #126
Reflection and refraction of lightLight travels normally through layers of thickness 0{,}2 and 0{,}3 m with indicators 1{,}5 and 2. Find the total transit time in nanoseconds. c = 300000000 m/s.
Show the walkthroughHide the walkthrough
- d_1
- 0{,}2\,\text{м}
- d_2
- 0{,}3\,\text{м}
- n_1
- 1{,}5\,\text{безразм.}
- n_2
- 2\,\text{безразм.}
- c
- 300000000\,\text{м/с}
t_{\text{нс}} - ?
- t_1=\frac{d_1n_1}{c}t_1=\frac{0{,}2 \cdot 1{,}5}{300000000}t_1=1\cdot 10^{-9}\,\text{с}
The time of the first layer is equal to the thickness divided by c/n₁.
- t_2=\frac{d_2n_2}{c}t_2=\frac{0{,}3 \cdot 2}{300000000}t_2=2\cdot 10^{-9}\,\text{с}
We calculate the second layer separately.
- t_{\text{нс}}=(t_1+t_2)10^9t_{\text{нс}}=(1\cdot 10^{-9} + 2\cdot 10^{-9}) \cdot 1000000000t_{\text{нс}}=3\,\text{нс}
Add up the times and convert to nanoseconds.
Answer3\,\text{нс}
Problem #127
Reflection and refraction of lightLight travels normally through layers of thickness 0{,}3 and 0{,}2 m with indicators 2 and 1{,}5. Find the total transit time in nanoseconds. c = 300000000 m/s.
Show the walkthroughHide the walkthrough
- d_1
- 0{,}3\,\text{м}
- d_2
- 0{,}2\,\text{м}
- n_1
- 2\,\text{безразм.}
- n_2
- 1{,}5\,\text{безразм.}
- c
- 300000000\,\text{м/с}
t_{\text{нс}} - ?
- t_1=\frac{d_1n_1}{c}t_1=\frac{0{,}3 \cdot 2}{300000000}t_1=2\cdot 10^{-9}\,\text{с}
The time of the first layer is equal to the thickness divided by c/n₁.
- t_2=\frac{d_2n_2}{c}t_2=\frac{0{,}2 \cdot 1{,}5}{300000000}t_2=1\cdot 10^{-9}\,\text{с}
We calculate the second layer separately.
- t_{\text{нс}}=(t_1+t_2)10^9t_{\text{нс}}=(2\cdot 10^{-9} + 1\cdot 10^{-9}) \cdot 1000000000t_{\text{нс}}=3\,\text{нс}
Add up the times and convert to nanoseconds.
Answer3\,\text{нс}
Problem #128
Lenses and diffractionFocal length of the collecting lens 0{,}2 m. Find the optical power.
Show the walkthroughHide the walkthrough
- F
- 0{,}2\,\text{м}
D - ?
- D=\frac{1}{F}D=\frac{1}{0{,}2}D=5\,\text{дптр}
For diopters, we take the focal length in meters.
Answer5\,\text{дптр}
Problem #129
Lenses and diffractionFocal length of the collecting lens 0{,}25 m. Find the optical power.
Show the walkthroughHide the walkthrough
- F
- 0{,}25\,\text{м}
D - ?
- D=\frac{1}{F}D=\frac{1}{0{,}25}D=4\,\text{дптр}
For diopters, we take the focal length in meters.
Answer4\,\text{дптр}
Problem #130
Lenses and diffractionOptical power of the collecting lens 4 diopter Find the focal length in centimeters.
Show the walkthroughHide the walkthrough
- D
- 4\,\text{дптр}
F_{\text{см}} - ?
- F=\frac{1}{D}F=\frac{1}{4}F=0{,}25\,\text{м}
The inverse optical power gives the focus in meters.
- F_{\text{см}}=100FF_{\text{см}}=0{,}25 \cdot 100F_{\text{см}}=25\,\text{см}
Convert meters to centimeters.
Answer25\,\text{см}
Problem #131
Lenses and diffractionOptical power of the collecting lens 5 diopter Find the focal length in centimeters.
Show the walkthroughHide the walkthrough
- D
- 5\,\text{дптр}
F_{\text{см}} - ?
- F=\frac{1}{D}F=\frac{1}{5}F=0{,}2\,\text{м}
The inverse optical power gives the focus in meters.
- F_{\text{см}}=100FF_{\text{см}}=0{,}2 \cdot 100F_{\text{см}}=20\,\text{см}
Convert meters to centimeters.
Answer20\,\text{см}
Problem #132
Lenses and diffractionObject height 3 cm located in 30 cm in front of a thin converging lens of focal length 20 cm. Find the magnitude of the real image height. Use 1/F = 1/d + 1/f and H/h = f/d, where d is the object distance and f the image distance.
Show the walkthroughHide the walkthrough
- h
- 3\,\text{см}
- d
- 30\,\text{см}
- F
- 20\,\text{см}
H - ?
- f=\frac{dF}{d-F}f=\frac{30 \cdot 20}{(30 - 20)}f=60\,\text{см}
The object is further than the focus, the image is real.
- |\Gamma|=\frac{f}{d}|\Gamma|=\frac{60}{30}|\Gamma|=2\,\text{раз}
We calculate the linear increase modulus.
- H=h|\Gamma|H=3 \cdot 2H=6\,\text{см}
The height module of the inverted image is required.
Answer6\,\text{см}
Problem #133
Lenses and diffractionObject height 4 cm located in 60 cm in front of a thin converging lens of focal length 20 cm. Find the magnitude of the real image height. Use 1/F = 1/d + 1/f and H/h = f/d, where d is the object distance and f the image distance.
Show the walkthroughHide the walkthrough
- h
- 4\,\text{см}
- d
- 60\,\text{см}
- F
- 20\,\text{см}
H - ?
- f=\frac{dF}{d-F}f=\frac{60 \cdot 20}{(60 - 20)}f=30\,\text{см}
The object is further than the focus, the image is real.
- |\Gamma|=\frac{f}{d}|\Gamma|=\frac{30}{60}|\Gamma|=0{,}5\,\text{раз}
We calculate the linear increase modulus.
- H=h|\Gamma|H=4 \cdot 0{,}5H=2\,\text{см}
The height module of the inverted image is required.
Answer2\,\text{см}
The theory behind these problems
Work through the topic if a problem will not give in.
Formulas by topic
Look up symbols and units of measurement in the reference.