参数资料
型号: TC1121CPA
厂商: Microchip Technology
文件页数: 5/14页
文件大小: 0K
描述: IC REG SWITCHED CAP INV ADJ 8DIP
产品变化通告: Obsolescence 22/Feb/2011
标准包装: 60
类型: 切换式电容器(充电泵),反相
输出类型: 可调式
输出数: 1
输出电压: -2.4 V ~ -5.5 V
输入电压: 2.4 V ~ 5.5 V
频率 - 开关: 10kHz ~ 200kHz
电流 - 输出: 100mA
同步整流器:
工作温度: 0°C ~ 70°C
安装类型: 通孔
封装/外壳: 8-DIP(0.300",7.62mm)
包装: 管件
供应商设备封装: 8-PDIP
产品目录页面: 663 (CN2011-ZH PDF)
其它名称: 158-1070
158-1070-ND
TC1121
3.0
APPLICATIONS
3.2
Changing Oscillator Frequency
3.1
Negative Voltage Converter
The TC1121’s clock frequency is controlled by four
modes:
The TC1121 is typically used as a charge-pump voltage
inverter. C1 and C2 are the only two external capacitors
used in the operating circuit (Figure 3-1).
TABLE 3-1:
OSCILLATOR FREQUENCY
MODES
FC
OSC
Oscillator Frequency
2.4V to 5.5V
Open
Open
10 kHz
1
FC
2 CAP +
8
V IN
OSC 7
FC = V +
Open or
FC = V +
Open 200 kHz
External Capacitor See Typical Operating
Characteristics
C1
+
3
TC1121
GND SHDN
6
SHDN*
Open     External Clock     External Clock Frequency
The oscillator runs at 10 kHz (typical) when FC and
OSC are not connected. The oscillator frequency is
4
CAP –
V OUT 5
+
C2
V OUT
lowered by connecting a capacitor between OSC and
GND, but FC can still multiply the frequency by 20
times in this mode.
An external clock source that swings within 100 mV of
V + and GND may overdrive OSC in the Inverter mode.
*SHDN should be tied to V IN if not used.
OSC can be driven by any CMOS logic output. When
OSC is overdriven, FC has no effect.
FIGURE 3-1:
Charge Pump Inverter
Note that the frequency of the signal appearing at
The TC1121 is not sensitive to load current changes,
although its output is not actively regulated. A typical
output source resistance of 11.8 Ω means that an input
of +5V results in -5V output voltage under light load,
and only decreases to -3.8V typ with a 100 mA load.
The supplied output current is from capacitor C2 during
one-half the charge-pump cycle. This results in a
peak-to-peak ripple of:
V RIPPLE = I OUT /2(f PUMP ) (C2) + I OUT (ESR C2 )
Where f PUMP is 5 kHz (one half the nominal 10 kHz
oscillator frequency), and C2 = 150 μ F with an ESR of
0.2 Ω , ripple is about 90 mV with a 100 mA load current.
If C2 is raised to 390 μ F, the ripple drops to 45 mV.
? 2006 Microchip Technology Inc.
CAP + and CAP – is half that of the oscillator. In addition,
by lowering the oscillator frequency, the effective
output resistance of the charge-pump increases. To
compensate for this, the value of the charge-pump
capacitors may be increased.
Because the 5 kHz output ripple frequency may be low
enough to interfere with other circuitry, the oscillator
frequency can be increased with the use of the FC pin
or an external oscillator. The output ripple frequency is
half the selected oscillator frequency. Although the
TC1121’s quiescent current will increase if the clock
frequency is increased, it allows smaller capacitance
values to be used for C1 and C2.
3.3 Capacitor Selection
In addition to load current, the following factors affect
the TC1121 output voltage drop from its ideal value 1)
output resistance, 2) pump (C1) and reservoir (C2)
capacitor ESRs and 3) C1 and C2 capacitance.
The voltage drop is the load current times the output
resistance. The loss in C2 is the load current times C2’s
ESR; C1’s loss is larger because it handles currents
greater than the load current during charge-pump
operation. Therefore, the voltage drop due to C1 is
about four times C1’s ESR multiplied by the load
current, and a low (or high) ESR capacitor has a
greater impact on performance for C1 than for C2.
In general, as the TC1121’s pump frequency increases,
capacitance values needed to maintain comparable
ripple and output resistance diminish proportionately.
DS21358C-page 5
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