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What is the Franck-Hertz experiment?
The Franck-Hertz experiment is a classic physics experiment that demonstrates the quantization of energy levels in atoms. It involves passing electrons through a tube filled with mercury vapor and measuring the energy loss of the electrons as they collide with mercury atoms. The experiment shows that electrons can only transfer discrete amounts of energy to the mercury atoms, confirming the existence of quantized energy levels in atoms. This experiment played a crucial role in the development of quantum mechanics. **
What is the Franck-Hertz experiment in physics?
The Franck-Hertz experiment is a fundamental experiment in physics that demonstrates the quantization of energy levels in atoms. It involves passing electrons through a tube filled with gas atoms and measuring the energy levels of the electrons before and after they collide with the atoms. By observing how the electrons lose energy in discrete amounts, scientists were able to confirm the existence of quantized energy levels in atoms, which is a key concept in quantum mechanics. The experiment played a crucial role in the development of quantum theory and our understanding of atomic structure. **
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Hertz HMC U1HMC U1 is a Connecting Cable from Hertz with IPX7 certification. Optional for HMR 50, HMR 20, HMR 10 D, and HMR 10. Mounting method U-bracket. Diameter of the mounting hole 45 mm. Dimensions A 68 mm, A1 70 mm, B 58 mm, C 29 mm, D 18 mm, E 46 mm. Features Connecting Cable IPX7 certification Optional for HMR 50, HMR 20, HMR 10 D, HMR 10 Mounting method U-bracket Diameter of the mounting hole 45 mm Technical Specifications A 68 mm A1 70 mm B 58 mm C 29 mm D 18 mm E 46 mm89,59 €*Shipping: 11,74 €Secure redirect to the provider
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Hertz HMA C1306The HMA C1306 is a Connecting Cable from Hertz. It is a 13-pin remote controller extension cable with a length of 6 m. The design is described as a marine connecting cable. It is optional for the HMR 50. Features Connecting Cable 13-pin Length 6 m Extension cable for remote control Optional for HMR 50 Marine connecting cable40,87 €*Shipping: 11,95 €Secure redirect to the provider
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Hertz S8 DSPThe S8 DSP is an 8-Channel DSP from Hertz in a corrosion-resistant housing made of metal and composite materials. The signal processing occurs at 96 kHz and 24 Bit, including Hi-Res certification from JAS. A 32-Bit DSP manages 6 analog high/low-level input channels, one coaxial SPDIF input, and 8 output channels. For the outputs, there are level controls, a 15-band equalizer per channel, time delays, crossover filters, and polarity; for the inputs, a 7-band equalizer per channel. The bandwidth ranges from 10 Hz to 40 kHz, the signal-to-noise ratio is 105 dBA (analog input) and 112 dBA (digital input), THD+N is below 0.005 %, and channel separation is over 95 dBA. Control and setup are done via the BT app for iOS/Android in Configurator and DRC mode, as well as via PC/Mac, including the exchange of setup files via BT and four presets with selection via cable. The power supply operates with 7–20 VDC and ART Automatic Remote Turn-On/Off; Remote IN/OUT are specified. The housing measures 130 x 33.8 x 88.3 mm at 0.66 kg. The DSP chipset is the Analog Devices ADAU1451. Features 8-Channel DSP Ultra-compact, corrosion-resistant housing made of metal and composite materials Hi-Res certification from JAS Signal processing 96 kHz / 24 Bit 32-Bit DSP, chipset Analog Devices ADAU1451 6 analog high/low-level inputs (differential input) Coaxial SPDIF digital input up to 24 Bit / 96 kHz 8 analog outputs (RCA) DSP control per output: level, 15-band EQ, time delay, crossover, polarity Input EQ: 7 bands parametric per channel BT app control iOS/Android: Configurator and DRC mode Load setup files via BT DSP management via PC/Mac/iOS/Android Dimensions 130 x 33.8 x 88.3 mm Weight 0.66 kg Power supply 7–20 VDC with ART Automatic Remote Turn-On/Off Technical Specifications Nominal voltage 7–20 VDC Fuse 1 A Pulse operating voltage 5–24 VDC Idle current 0.34 A OFF current (ART= OFF) <80 µA OFF current (ART= ON) <80 µA Remote IN 6–20 VDC (10 mA) Remote OUT 4–20 VDC (150 mA) ART from BTL speaker outputs, selectable 1.5–7 VDC Analog low-level inputs: 6 channels, differential input (Molex micro connector to RCA) Analog high-level inputs: 6 channels, differential input (Molex micro connection at triggered ends) + USS Digital input: Coaxial SPDIF up to 24 Bit / 96 kHz (Molex Microfit to RCA) Input sensitivity low-level 0.8–6 V RMS Input sensitivity high-level 2.5–21 V RMS Audio input routing as matrix Analog input EQ: 7 bands parametric per channel ART Automatic Remote Turn-On/Off with Speaker-In Analog outputs: 8 channels (RCA) Max. output level 4 V RMS @ 0.05 % THD Bandwidth 10 Hz – 40 kHz (+/-3 dB) Signal-to-noise ratio (A-weighted) 105 dBA, analog input Signal-to-noise ratio (A-weighted) 112 dBA, digital input THD+N (@ 1 V RMS out, @ 1 kHz) <0.005 % Channel separation @ 1 kHz >95 dBA DSP sampling rate 96 kHz DSP bit depth 24 Output equalizer: 15 bands per channel, Q and frequency adjustable EQ resolution 0.1 dB per step, +12 dB / -12 dB Time alignment distance 0–468.4 cm...455,20 €*Shipping: 0,00 €Secure redirect to the provider
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Hertz Venezia V1Venezia V1 is a 1-Channel Amplifier from Hertz with Advanced Class D Technology and 1260 W @ 1 Ohm. Designed for marine applications with resistance to salt mist, UV light, and vibrations. Fanless cooling and fully differential input circuit. Supply voltage 9–16 VDC, minimum load impedance 1 Ohm, bandwidth 10–500 Hz. Distortion <0.02 % (100 Hz @ 4 Ohm), signal-to-noise ratio 102 dB (A-weighted @ 1 V), damping factor 500 (100 Hz @ 4 Ohm). Adjustable crossovers, Low-Pass 50–500 Hz @ 24 dB/Oct, High-Pass 50–250 Hz @ 12 dB/Oct at Pre-Out, Subsonic 25 Hz @ 24 dB/Oct, Phase 0–180°, Bass Boost 50 Hz 0–12 dB. PRE IN, Bypass Full, Current Draw @ 1 Ohm and 14.4 VDC (maximum musical power) 52 A. Features 1-Channel Amplifier Marine Version with Resistance to Salt Mist, UV Light, and Vibrations Advanced Class D Technology Fanless Cooling Fully Differential Input Circuit Inputs PRE IN Pre-Out High-Pass 50–250 Hz @ 12 dB/Oct Filter Yes Bypass Yes Full Low-Pass 50–500 Hz @ 24 dB/Oct Phase 0–180° Subsonic 25 Hz @ 24 dB/Oct Bass Boost 50 Hz 0–12 dB Load Impedance minimum 1 Ohm Adjustable Crossovers RMS Output Power @ 14.4 VDC, THD 1% 1 Channel 700 W RMS Output Power @ 14.4 VDC, THD 1% 1 Channel 1260 W Total Power RMS 1260 W Optional Accessories HRC BM2 Subwoofer Remote Control with Level -20 to +6 dB and Molex Connector Technical Specifications Channels 1 Supply Voltage 9–16 VDC Power On/Off 1 A / 0.04 mA Current Draw @ 1 Ohm, 14.4 VDC maximum musical power 52 A Remote Input 7–15 VDC 1 mA Distortion <0.02 % (100 Hz @ 4 Ohm) Bandwidth 10–500 Hz Signal-to-Noise Ratio (A-weighted @ 1 V) 102 dB Damping Factor (100 Hz @ 4 Ohm) 500 Sensitivity 0.2–5 VRMS Pre-In Impedance 10 kOhm High-Pass Pre-Out 50–250 Hz @ 12 dB/Oct Low-Pass 50–500 Hz @ 24 dB/Oct Subsonic 25 Hz @ 24 dB/Oct Phase 0–180° Bass Boost 50 Hz 0–12 dB Dimension A 270 mm Dimension B 240 mm Dimension C 185 mm Dimension D 155 mm Dimension E 54 mm Weight 2.72 kg455,20 €*Shipping: 0,00 €Secure redirect to the provider
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What is the Franck-Hertz experiment with neon?
The Franck-Hertz experiment with neon is a classic physics experiment that demonstrates the quantization of energy levels in atoms. In the experiment, a low-pressure tube filled with neon gas is bombarded with electrons, causing the gas to emit light. By measuring the energy of the emitted light, scientists can observe distinct peaks corresponding to the energy levels of the neon atoms. This experiment provided important evidence for the quantization of energy levels in atoms, which is a fundamental concept in quantum mechanics. **
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Why are there energy collisions in Franck-Hertz experiments?
Energy collisions occur in Franck-Hertz experiments because electrons are accelerated towards a positively charged grid, gaining kinetic energy. When these high-energy electrons collide with mercury atoms in the tube, they transfer some of their energy to the atoms, exciting them to higher energy levels. This energy transfer results in a decrease in the kinetic energy of the electrons, which can be measured as a drop in voltage across the tube. These collisions are crucial for observing the quantized energy levels of the mercury atoms. **
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Why are there energy impulses in Franck-Hertz experiments?
In Franck-Hertz experiments, energy impulses occur due to the collisions between electrons and atoms in a gas-filled tube. When electrons are accelerated towards the positively charged anode, they gain kinetic energy. Upon colliding with the atoms in the gas, the electrons transfer some of this energy to the atoms, causing them to become excited. The energy impulses are a result of this energy transfer process, which can be observed as peaks in the current-voltage curve of the experiment. **
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What is the polarity in the Franck-Hertz experiment?
The polarity in the Franck-Hertz experiment refers to the direction of the voltage applied to the electron tube. When the polarity is positive, the electrons are accelerated towards the positively charged grid, and when the polarity is negative, the electrons are repelled from the grid. This polarity affects the energy levels of the electrons and determines whether they can overcome the energy barriers in the tube, leading to the observation of distinct peaks in the current-voltage characteristic of the experiment. **
What is the Franck-Hertz experiment with other gases?
The Franck-Hertz experiment is a fundamental experiment in physics that demonstrates the quantization of energy levels in atoms. In the original experiment, electrons are accelerated through a vapor of mercury atoms, and the energy of the electrons is measured as they collide with the mercury atoms. When the electrons have enough energy to excite the mercury atoms to a higher energy level, a drop in the current is observed, indicating that the electrons have lost energy in the collision. The experiment has also been performed with other gases, such as neon and argon, to demonstrate the quantization of energy levels in different atomic systems. In these variations of the experiment, the energy levels of the atoms in the gas are measured by observing the energy loss of the electrons as they collide with the gas atoms. The results of these experiments confirm the quantized nature of energy levels in atoms, as predicted by quantum mechanics. **
With which gases can the Franck-Hertz experiment be conducted?
The Franck-Hertz experiment can be conducted with gases such as mercury vapor, neon, and argon. These gases are commonly used because they have discrete energy levels that allow for the observation of quantized energy transitions. By applying a voltage to the gas, electrons can be accelerated and collide with the gas atoms, leading to the excitation and de-excitation of the gas atoms, which can be measured to study the quantization of energy levels. **
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Hertz HRCThe HRC product is a Bass Remote Control from Hertz. It is a specialized bass level remote control for Hertz HCP Amplifiers. The model is compatible with Hertz HCP 1D, HCP 5D, and HMP 1D. Features Bass Remote Control Bass level remote control for Hertz HCP Amplifiers Compatible with Hertz HCP 1D Compatible with Hertz HCP 5D Compatible with Hertz HMP 1D21,90 €*Shipping: 11,67 €Secure redirect to the provider
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Hertz HMC U1HMC U1 is a Connecting Cable from Hertz with IPX7 certification. Optional for HMR 50, HMR 20, HMR 10 D, and HMR 10. Mounting method U-bracket. Diameter of the mounting hole 45 mm. Dimensions A 68 mm, A1 70 mm, B 58 mm, C 29 mm, D 18 mm, E 46 mm. Features Connecting Cable IPX7 certification Optional for HMR 50, HMR 20, HMR 10 D, HMR 10 Mounting method U-bracket Diameter of the mounting hole 45 mm Technical Specifications A 68 mm A1 70 mm B 58 mm C 29 mm D 18 mm E 46 mm89,59 €*Shipping: 11,74 €Secure redirect to the provider
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Hertz HMA C1306The HMA C1306 is a Connecting Cable from Hertz. It is a 13-pin remote controller extension cable with a length of 6 m. The design is described as a marine connecting cable. It is optional for the HMR 50. Features Connecting Cable 13-pin Length 6 m Extension cable for remote control Optional for HMR 50 Marine connecting cable40,87 €*Shipping: 11,95 €Secure redirect to the provider
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What is the Franck-Hertz experiment?
The Franck-Hertz experiment is a classic physics experiment that demonstrates the quantization of energy levels in atoms. It involves passing electrons through a tube filled with mercury vapor and measuring the energy loss of the electrons as they collide with mercury atoms. The experiment shows that electrons can only transfer discrete amounts of energy to the mercury atoms, confirming the existence of quantized energy levels in atoms. This experiment played a crucial role in the development of quantum mechanics. **
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What is the Franck-Hertz experiment in physics?
The Franck-Hertz experiment is a fundamental experiment in physics that demonstrates the quantization of energy levels in atoms. It involves passing electrons through a tube filled with gas atoms and measuring the energy levels of the electrons before and after they collide with the atoms. By observing how the electrons lose energy in discrete amounts, scientists were able to confirm the existence of quantized energy levels in atoms, which is a key concept in quantum mechanics. The experiment played a crucial role in the development of quantum theory and our understanding of atomic structure. **
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What is the Franck-Hertz experiment with neon?
The Franck-Hertz experiment with neon is a classic physics experiment that demonstrates the quantization of energy levels in atoms. In the experiment, a low-pressure tube filled with neon gas is bombarded with electrons, causing the gas to emit light. By measuring the energy of the emitted light, scientists can observe distinct peaks corresponding to the energy levels of the neon atoms. This experiment provided important evidence for the quantization of energy levels in atoms, which is a fundamental concept in quantum mechanics. **
-
Why are there energy collisions in Franck-Hertz experiments?
Energy collisions occur in Franck-Hertz experiments because electrons are accelerated towards a positively charged grid, gaining kinetic energy. When these high-energy electrons collide with mercury atoms in the tube, they transfer some of their energy to the atoms, exciting them to higher energy levels. This energy transfer results in a decrease in the kinetic energy of the electrons, which can be measured as a drop in voltage across the tube. These collisions are crucial for observing the quantized energy levels of the mercury atoms. **
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Hertz S8 DSPThe S8 DSP is an 8-Channel DSP from Hertz in a corrosion-resistant housing made of metal and composite materials. The signal processing occurs at 96 kHz and 24 Bit, including Hi-Res certification from JAS. A 32-Bit DSP manages 6 analog high/low-level input channels, one coaxial SPDIF input, and 8 output channels. For the outputs, there are level controls, a 15-band equalizer per channel, time delays, crossover filters, and polarity; for the inputs, a 7-band equalizer per channel. The bandwidth ranges from 10 Hz to 40 kHz, the signal-to-noise ratio is 105 dBA (analog input) and 112 dBA (digital input), THD+N is below 0.005 %, and channel separation is over 95 dBA. Control and setup are done via the BT app for iOS/Android in Configurator and DRC mode, as well as via PC/Mac, including the exchange of setup files via BT and four presets with selection via cable. The power supply operates with 7–20 VDC and ART Automatic Remote Turn-On/Off; Remote IN/OUT are specified. The housing measures 130 x 33.8 x 88.3 mm at 0.66 kg. The DSP chipset is the Analog Devices ADAU1451. Features 8-Channel DSP Ultra-compact, corrosion-resistant housing made of metal and composite materials Hi-Res certification from JAS Signal processing 96 kHz / 24 Bit 32-Bit DSP, chipset Analog Devices ADAU1451 6 analog high/low-level inputs (differential input) Coaxial SPDIF digital input up to 24 Bit / 96 kHz 8 analog outputs (RCA) DSP control per output: level, 15-band EQ, time delay, crossover, polarity Input EQ: 7 bands parametric per channel BT app control iOS/Android: Configurator and DRC mode Load setup files via BT DSP management via PC/Mac/iOS/Android Dimensions 130 x 33.8 x 88.3 mm Weight 0.66 kg Power supply 7–20 VDC with ART Automatic Remote Turn-On/Off Technical Specifications Nominal voltage 7–20 VDC Fuse 1 A Pulse operating voltage 5–24 VDC Idle current 0.34 A OFF current (ART= OFF) <80 µA OFF current (ART= ON) <80 µA Remote IN 6–20 VDC (10 mA) Remote OUT 4–20 VDC (150 mA) ART from BTL speaker outputs, selectable 1.5–7 VDC Analog low-level inputs: 6 channels, differential input (Molex micro connector to RCA) Analog high-level inputs: 6 channels, differential input (Molex micro connection at triggered ends) + USS Digital input: Coaxial SPDIF up to 24 Bit / 96 kHz (Molex Microfit to RCA) Input sensitivity low-level 0.8–6 V RMS Input sensitivity high-level 2.5–21 V RMS Audio input routing as matrix Analog input EQ: 7 bands parametric per channel ART Automatic Remote Turn-On/Off with Speaker-In Analog outputs: 8 channels (RCA) Max. output level 4 V RMS @ 0.05 % THD Bandwidth 10 Hz – 40 kHz (+/-3 dB) Signal-to-noise ratio (A-weighted) 105 dBA, analog input Signal-to-noise ratio (A-weighted) 112 dBA, digital input THD+N (@ 1 V RMS out, @ 1 kHz) <0.005 % Channel separation @ 1 kHz >95 dBA DSP sampling rate 96 kHz DSP bit depth 24 Output equalizer: 15 bands per channel, Q and frequency adjustable EQ resolution 0.1 dB per step, +12 dB / -12 dB Time alignment distance 0–468.4 cm...455,20 €*Shipping: 0,00 €Secure redirect to the provider
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Hertz Venezia V1Venezia V1 is a 1-Channel Amplifier from Hertz with Advanced Class D Technology and 1260 W @ 1 Ohm. Designed for marine applications with resistance to salt mist, UV light, and vibrations. Fanless cooling and fully differential input circuit. Supply voltage 9–16 VDC, minimum load impedance 1 Ohm, bandwidth 10–500 Hz. Distortion <0.02 % (100 Hz @ 4 Ohm), signal-to-noise ratio 102 dB (A-weighted @ 1 V), damping factor 500 (100 Hz @ 4 Ohm). Adjustable crossovers, Low-Pass 50–500 Hz @ 24 dB/Oct, High-Pass 50–250 Hz @ 12 dB/Oct at Pre-Out, Subsonic 25 Hz @ 24 dB/Oct, Phase 0–180°, Bass Boost 50 Hz 0–12 dB. PRE IN, Bypass Full, Current Draw @ 1 Ohm and 14.4 VDC (maximum musical power) 52 A. Features 1-Channel Amplifier Marine Version with Resistance to Salt Mist, UV Light, and Vibrations Advanced Class D Technology Fanless Cooling Fully Differential Input Circuit Inputs PRE IN Pre-Out High-Pass 50–250 Hz @ 12 dB/Oct Filter Yes Bypass Yes Full Low-Pass 50–500 Hz @ 24 dB/Oct Phase 0–180° Subsonic 25 Hz @ 24 dB/Oct Bass Boost 50 Hz 0–12 dB Load Impedance minimum 1 Ohm Adjustable Crossovers RMS Output Power @ 14.4 VDC, THD 1% 1 Channel 700 W RMS Output Power @ 14.4 VDC, THD 1% 1 Channel 1260 W Total Power RMS 1260 W Optional Accessories HRC BM2 Subwoofer Remote Control with Level -20 to +6 dB and Molex Connector Technical Specifications Channels 1 Supply Voltage 9–16 VDC Power On/Off 1 A / 0.04 mA Current Draw @ 1 Ohm, 14.4 VDC maximum musical power 52 A Remote Input 7–15 VDC 1 mA Distortion <0.02 % (100 Hz @ 4 Ohm) Bandwidth 10–500 Hz Signal-to-Noise Ratio (A-weighted @ 1 V) 102 dB Damping Factor (100 Hz @ 4 Ohm) 500 Sensitivity 0.2–5 VRMS Pre-In Impedance 10 kOhm High-Pass Pre-Out 50–250 Hz @ 12 dB/Oct Low-Pass 50–500 Hz @ 24 dB/Oct Subsonic 25 Hz @ 24 dB/Oct Phase 0–180° Bass Boost 50 Hz 0–12 dB Dimension A 270 mm Dimension B 240 mm Dimension C 185 mm Dimension D 155 mm Dimension E 54 mm Weight 2.72 kg455,20 €*Shipping: 0,00 €Secure redirect to the provider
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Hertz Venezia V4The Hertz Venezia V4 is a 4-Channel Amplifier with Advanced Class D technology. Its design for marine applications includes an IPX2 certification. The Hi-Res certification, a bandwidth of 10 to 42 kHz, and an A-weighted signal-to-noise ratio of 102 dBA characterize the signal processing. The amplifier can operate as a 4-, 3-, or 2-channel unit and offers adjustable crossovers with Hi-Pass and Lo-Pass for each channel pair, as well as a bass boost at 50 Hz. Inputs include PRE IN and a full-range Pre-Out; A and B channels provide mono switching and bypass. The power supply operates with 9 to 16 VDC, and the remote input works with 7 to 15 VDC at 1 mA. The architecture is designed for high efficiency with low heat generation and reduced electromagnetic radiation. Dimensions A/B/C/D/E: 270/240/185/155/54 mm, weight 2.66 kg. Features 4-Channel Amplifier Advanced Class D technology IPX2 certified Hi-Res certified Channel configuration: 4 / 3 / 2 Adjustable crossovers Designed for marine applications Optional accessories: HRC BM2 Subwoofer remote control, Subwoofer level -20 to +6 dB, Molex connector Technical Specifications Supply voltage: 9 - 16 VDC Current (On/Off): 1.6 A / 0.04 mA Consumption at 1 Ω, 14.4 VDC (max. musical power): 48 A Remote input: 7 - 15 VDC, 1 mA Distortion (THD, 100 Hz @ 4 Ω): < 0.06 % Bandwidth: 10 - 42 kHz S/N Ratio (A-weighted @ 1 V): 102 dBA Damping factor (100 Hz @ 4 Ω): 130 Sensitivity Low-In: 0.2 - 5 VRMS Pre-In impedance: 10 kΩ Minimum load impedance: 2 Ω Inputs: PRE IN Pre-Out: Full range A channel pair: MONO (on/off) A channel pair: Bypass Yes (Full) A channel pair: Hi-Pass 50 - 4,000 Hz @ 12 dB/Oct A channel pair: Lo-Pass 50 - 4,000 Hz @ 12 dB/Oct B channel pair: MONO (on/off) B channel pair: Bypass Yes (Full) B channel pair: Hi-Pass 50 - 4,000 Hz @ 12 dB/Oct B channel pair: Lo-Pass 50 - 4,000 Hz @ 12 dB/Oct Bass boost: 50 Hz, 0 - 12 dB 4 channels: 160 W x 4 (4 Ω) RMS @ 14.4 VDC, THD 1 % 4 channels: 290 W x 4 (2 Ω) RMS @ 14.4 VDC, THD 1 % 3 channels: 160 W x 2 (4 Ω) + 580 W x 1 (4 Ω) RMS @ 14.4 VDC, THD 1 % 3 channels: 290 W x 2 (2 Ω) + 580 W x 1 (4 Ω) RMS @ 14.4 VDC, THD 1 % 2 channels: 580 W x 2 (4 Ω) RMS @ 14.4 VDC, THD 1 % Total RMS power: 1160 W Dimensions: A 270 mm, B 240 mm, C 185 mm, D 155 mm, E 54 mm Weight: 2.66 kg496,06 €*Shipping: 0,00 €Secure redirect to the provider
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Hertz Venezia V5Venezia V5 is a 5-Channel Amplifier from Hertz featuring Hertz Advanced Class D technology and Hi-Res certification. The output power (RMS) @ 14.4 VDC, THD 1% includes 5 channels with 130 W x 4 (4 Ω) plus 490 W x 1 (4 Ω) as well as 5 channels with 220 W x 4 (2 Ω) plus 820 W x 1 (2 Ω). Alternatively, 3 channels with 440 W x 2 (4 Ω) plus 490 W x 1 (4 Ω) or 3 channels with 440 W x 2 (4 Ω) plus 820 W x 1 (2 Ω); total RMS power is 1700 W. The bandwidth is 10 - 42 kHz, the total harmonic distortion is <0.05% (100 Hz @ 4 Ω), the signal-to-noise ratio is 102 dB (A weighted @ 1 V), and the damping factor is 130 (100 Hz @ 4 Ω). The power supply operates with 9 - 16 VDC, the current draw is 1.8 A when turned on and 0.04 mA in standby, the consumption at 1 Ω and 14.4 VDC (max musical power) is 70 A, the remote input is 7 - 15 VDC and 1 mA. Preamp inputs are available for A, B, and Sub channels, Pre-Out is not available. The filters include Hi-Pass, Band-Pass, and Low-Pass with adjustable ranges, plus phase 0 - 180°, subsonic 25 Hz @ 24 dB/Oct, and boost 50 Hz 0 - 12 dB. The dimensions are A 330 mm, B 300 mm, C 200 mm, D 170 mm, E 54 mm; the weight is 3.72 kg. Features 5-Channel Amplifier Manufacturer: Hertz Hertz Advanced Class D technology Hi-Res certified Channels: 5 - 3 Adjustable crossovers Inputs: A Ch. Pre-In, B Ch. Pre-In, Sub Ch. Pre-In Pre-Out: No Supply voltage: 9 - 16 VDC Bandwidth: 10 - 42 kHz Dimensions: A 330 mm, B 300 mm, C 200 mm, D 170 mm, E 54 mm Weight: 3.72 kg Technical Specifications Output power (RMS) @ 14.4 VDC, THD 1%: 5 channels 130 W x 4 (4 Ω) + 490 W x 1 (4 Ω) Output power (RMS) @ 14.4 VDC, THD 1%: 5 channels 220 W x 4 (2 Ω) + 820 W x 1 (2 Ω) Output power (RMS) @ 14.4 VDC, THD 1%: 3 channels 440 W x 2 (4 Ω) + 490 W x 1 (4 Ω) Output power (RMS) @ 14.4 VDC, THD 1%: 3 channels 440 W x 2 (4 Ω) + 820 W x 1 (2 Ω) Total RMS power: 1700 W Distortion (THD, 100 Hz @ 4 Ω): <0.05% SNR (A weighted @ 1 V): 102 dB Damping factor (100 Hz @ 4 Ω): 130 Sensitivity Low-In: 0.2 - 5 VRMS Pre-In impedance: 10 kΩ Load impedance (MIN) 5Ch: 2 Ω Load impedance (MIN) 3Ch: 4 Ω + 4 Ω + 2 Ω Power supply: 9 - 16 VDC Current (On/Off): 1.8 A / 0.04 mA Consumption @ 1 Ω, 14.4 VDC (max musical power): 70 A Remote input: 7 - 15 VDC, 1 mA A Ch. Filter: Bypass Yes; Hi-Pass 50 - 500 Hz / 500 Hz - 5 kHz @ 12 dB/Oct B Ch. Filter: Bypass Yes; Hi-Pass 50 - 500 Hz @ 12 dB/Oct; Band-Pass 50 - 500 Hz / 500 Hz - 5 kHz @ 12 dB/Oct Sub Ch. Filter: Bypass No; Low-Pass 50 - 250 Hz @ 24 dB/Oct; Phase 0 - 180°; Subsonic 25 Hz @ 24 dB/Oct; Boost 50 Hz 0 - 12 dB Dimensions: A 330 mm, B 300 mm, C 200 mm, D 170 mm, E 54 mm Weight: 3.72 kg645,41 €*Shipping: 0,00 €Secure redirect to the provider
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Why are there energy impulses in Franck-Hertz experiments?
In Franck-Hertz experiments, energy impulses occur due to the collisions between electrons and atoms in a gas-filled tube. When electrons are accelerated towards the positively charged anode, they gain kinetic energy. Upon colliding with the atoms in the gas, the electrons transfer some of this energy to the atoms, causing them to become excited. The energy impulses are a result of this energy transfer process, which can be observed as peaks in the current-voltage curve of the experiment. **
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What is the polarity in the Franck-Hertz experiment?
The polarity in the Franck-Hertz experiment refers to the direction of the voltage applied to the electron tube. When the polarity is positive, the electrons are accelerated towards the positively charged grid, and when the polarity is negative, the electrons are repelled from the grid. This polarity affects the energy levels of the electrons and determines whether they can overcome the energy barriers in the tube, leading to the observation of distinct peaks in the current-voltage characteristic of the experiment. **
-
What is the Franck-Hertz experiment with other gases?
The Franck-Hertz experiment is a fundamental experiment in physics that demonstrates the quantization of energy levels in atoms. In the original experiment, electrons are accelerated through a vapor of mercury atoms, and the energy of the electrons is measured as they collide with the mercury atoms. When the electrons have enough energy to excite the mercury atoms to a higher energy level, a drop in the current is observed, indicating that the electrons have lost energy in the collision. The experiment has also been performed with other gases, such as neon and argon, to demonstrate the quantization of energy levels in different atomic systems. In these variations of the experiment, the energy levels of the atoms in the gas are measured by observing the energy loss of the electrons as they collide with the gas atoms. The results of these experiments confirm the quantized nature of energy levels in atoms, as predicted by quantum mechanics. **
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With which gases can the Franck-Hertz experiment be conducted?
The Franck-Hertz experiment can be conducted with gases such as mercury vapor, neon, and argon. These gases are commonly used because they have discrete energy levels that allow for the observation of quantized energy transitions. By applying a voltage to the gas, electrons can be accelerated and collide with the gas atoms, leading to the excitation and de-excitation of the gas atoms, which can be measured to study the quantization of energy levels. **
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