Product introduction:
Faraday quasi-capacitance refers to the capacitance related to the charge potential of the electrode, which is generated by the highly reversible chemical adsorption, desorption or oxidation and reduction reaction of the electroactive substance on the two-dimensional or quasitwo-dimensional space of the electrode surface or the bulk phase. Faraday quasi-capacitance can be generated not only on the surface of the electrode, but also in the whole electrode, so it can obtain higher capacitance and energy density than double-layer capacitance. Under the condition of the same electrode area, the Faraday quasi-capacitance can be 10~100 times of the capacitance of the electric double layer.
Series specification table:
series name | series | |||||||
type name | YKY-6R0 | |||||||
Rated voltage VR | 6.0V | |||||||
surge voltage | 6.3V | |||||||
Capacity range | 0.47F-12F | |||||||
Operating temperature range | -40℃~+65℃ | |||||||
Product life | Normal temperature cycle life: 25°C, 500,000 cycles between VR and 1/2VR, capacity decay ≤30%, internal resistance change ≤4 times | |||||||
High temperature endurance life: 65℃, keep VR, 1000 hours, capacity decay ≤30%, internal resistance change ≤4 times. |
Product performance table
model | Voltage V | Capacity F | AC internal resistance mΩ1KHz | 24h leakage current uA | Product size mm | ||||
width F±1 | Length A±1 | Height B±1 | Pitch P | ||||||
YKY-6R0-Z474VYE06 | 6.0 | 0.47 | 700 | 10 | 8.5 | 16.5 | 15 | 12 | |
YKY-6R0-Z105VYE07 | 6.0 | 1.0 | 350 | 20 | 8.5 | 16.5 | 22 | 12 | |
YKY-6R0-Z155TYE0 | 6.0 | 1.5 | 200 | 30 | 8.5 | 16.5 | 22 | 12 | |
YKY-6R0-Z155VYE1 | 6.0 | 1.5 | 200 | 30 | 10.5 | 20.5 | 22 | 15.3 | |
YKY-6R0-Z205VYE0 | 6.0 | 2.0 | 180 | 40 | 13 | 25.5 | 23 | 17.8 | |
YKY-6R0-Z255VYE1 | 6.0 | 2.5 | 180 | 50 | 10.5 | 20.5 | 22 | 15.3 | |
YKY-6R0-Z305VYE1 | 6.0 | 3.0 | 150 | 60 | 10.5 | 20.5 | 22 | 15.3 | |
YKY-6R0-Z355VYE1 | 6.0 | 3.5 | 140 | 70 | 10.5 | 20.5 | 22 | 15.3 | |
YKY-6R0-Z405VYE0 | 6.0 | 4.0 | 120 | 80 | 13 | 25.5 | 23 | 17.8 | |
YKY-6R0-Z505VYE1 | 6.0 | 5.0 | 110 | 100 | 13 | 25.5 | 27 | 17.8 | |
YKY-6R0-Z505VYE1 | 6.0 | 5.0 | 120 | 100 | 10.5 | 20.5 | 27 | 15.3 | |
YKY-6R0-Z605VYE1 | 6.0 | 6.0 | 80 | 120 | 13 | 25.5 | 36 | 17.8 | |
YKY-6R0-Z106VYL21 | 6.0 | 10 | 60 | 100 | 16.5 | 32.5 | 28 | 24 | |
YKY-6R0-Z126VYL2 | 6.0 | 12 | 60 | 240 | 16.5 | 32.5 | 28 | 24 |
Product Description:
Advantages of double layer super Faraday capacitor
High reliability, cycle life: > 500000 times
Good frequency characteristics, high temperature resistance, low temperature rise and high adhesion
High energy conversion efficiency
Small loss during use
Green power supply :
The charging circuit is simple, without the charging circuit like charging battery, and maintenance free for long-term use
product photo and desing:
It is widely used in gas meters, water meters, heat meters, meter reading systems, etc. for starting devices, detonators, tax controllers, toys, power equipment, etc
testing method:
1. Electrostatic capacity test method:
(1) Test principle
The test of the electrostatic capacity of the supercapacitor is to use the method of constant current discharge of the capacitor , and calculate it according to the formula.
C=It(U1-U2)
In the formula: C - electrostatic capacity, F;
I-constant discharge current, A;
U1, U2 - use voltage, V;
t-Discharge time required for U1 to U2, S
(2), test procedure
Charge the capacitor with a current of 100A, charge the capacitor to the working voltage and keep the voltage constant for 10 seconds, then discharge the capacitor with a current of 100A, take U1 as 1.2V and U2 as 1.0V, record the discharge time within this voltage range, and the total cycle Capacitance, take the average value.
2. Stored energy test
(1) Test principle:
The test of supercapacitor energy is carried out by the method of discharging the capacitor with constant power to 1/2 of the working voltage with the given voltage range of the capacitor. The output energy W of the capacitor is obtained from the relationship between the constant discharge power P and the discharge time T, namely:
W=PT
(2) Test procedure
Charge the capacitor to the working voltage with a constant current of 100A, and then keep it constant until the charging current drops to the specified current (10A for traction type, 1A for start-up type), after 5 seconds of rest, discharge the capacitor with constant power to 1/2 of the working voltage, record Discharge time and calculate magnitude. Repeat the measurement 3 times and take the average value.
3. Equivalent series resistance test (DC)
(1) Test principle
The internal resistance of the capacitor is measured according to the sudden change of the voltage within 10 milliseconds of the capacitor disconnecting the constant current charging circuit. That is: in the formula:
R - the internal resistance of the capacitor;
U0 - capacitor cut off the voltage before charging;
Ui - cut off the voltage within 10ms after charging;
I - cut off the current before charging.
(2) Measurement process
Charge the capacitor with a constant current of 100A, disconnect the charging circuit when the charging working voltage is 80%, use a sampling machine, record the voltage change value within 10 milliseconds after the capacitor is powered off, and calculate the internal resistance, repeat 3 times, and take the average value.
4. Leakage current test
After charging the capacitor to the rated voltage with a constant current of 100A, charge the capacitor with a constant voltage for 30min at this voltage value, and then leave it open for 72h. During the first three hours, the voltage value was recorded every minute, and during the remaining time, the voltage value was recorded every ten minutes.
Calculate the self-discharge energy loss, SDLF=1-(V/VW)2, and the calculation time points are: 0.5, 1, 8, 24, 36, 72h.
Note: The voltage tester must have high input impedance to minimize the impact of discharge.