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The Compton effect is an interesting phenomenon in physics. Our fun Physics test which consists of some very informative practice questions on Compton Effect will test your numerical and theoretical knowledge of the topic. Compton effect, by definition, is the scattering of a high-frequency photon particle after interacting with a stationary particle in the system. Our quiz is here See moreto strengthen and test your fundamentals of the phenomenon. Make sure to attempt all the questions correctly and carefully. All the very best & study hard!
4
1
-2
-4
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Hν/c
Hν/c²
Zero
Hν²/c
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2c/3
C/3
√2c
2√2c/3
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0º to 90º
90º to 180º
0º to 180º
0º to 45º
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8
6
4
12
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0.08 Å
1 Å
12.26 Å
150 Å
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1.5
1.12
1.22
2.22
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H/√(3mkT)
H/√(2mkT)
√3h/(mkT)
3h/√(2mkT)
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1.67 Å
0.167 Å
0.227 Å
2.27 Å
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4V
V/4
V/8
8V
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705 nm
515 nm
630 nm
555 nm
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4000 K
4500 K
5000 K
5500 K
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E(ν) → 0 as ν → 0
E(T) → ∞ as T → 0
E(λ) → ∞ as λ → 0
E(λ) → ∞ as λ → ∞
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Hν/(exp[hν/kT] - 1)
Hν/(exp[hν/kT] + 1)
Hν
Hν*exp[-hν/kT]
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2 eV
2 keV
2 MeV
0.02 eV
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Negative
Zero
More positive than what is observed with X-rays
Positive but not detectable in the visible window
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ν³
ν²
ν
Hν/(exp[hν/kT] - 1)
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45°
90°
60°
180°
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I > I' for both carbon and silver
I = I' for both carbon and silver
I > I' for carbon, I < I' for silver
I < I' for carbon, I > I' for silver
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Photon's energy
Photon's energy >> kT
Photon's energy = kT
Photon's energy has any finite value
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Zero
∞
1
½
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1.3 nanometer
1.3 micrometer
3.3 nanometer
3.3 micrometer
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0.24 Å
0.024 Å
2.4 Å
0.0024 Å
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Infrared signature
Twin paradox
Ultraviolet catastrophe
Gibb's paradox
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Zero
∞
1
1/2
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9x10¹⁰ Joules
300 Joules
9x10¹³ Joules
900 Joules
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Higher temperature
All temperatures
Higher wavelength
Lower wavelength
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1.67 m₀
1.25 m₀
0.8 m₀
0.6 m₀
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7250 K
8750 K
3550 K
5200 K
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90°
180°
135°
60°
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(h/Mc)²
H/(Mc²)
H/(Mc)
Mc²/h
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T²
T⁴
T⁻⁴
T⁻¹
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1000:1
10000:1
1:1000
1:10000
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2
0.25
4
1
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2.1x10ˉ²⁸
2.1x10ˉ³⁴
0.5x10ˉ³⁴
5.0x10ˉ²⁴
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5:3
3:5
25:9
9:25
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1:2
1:4
2:1
4:1
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10ˉ³¹ m
10ˉ³³ m
10ˉ¹⁸ m
10ˉ²⁵ m
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The more precise a particle's energy can be measured, the less precise its position can be measured
The more precise a particle's momentum can be measured, the less precise its position can be measured
The more precise a particle's momentum can be measured, the less precise its time can be measured
A particle's momentum can be measured exactly
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1.72 kT
0.38 kT
0.58 kT
2.72 kT
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E²
E
1/E
1/E²
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