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ZHCSOW0J January 2000 – March 2022 LM158-N , LM258-N , LM2904-N , LM358-N

PRODUCTION DATA

封裝選項

機械數(shù)據(jù) (封裝 | 引腳)

D|8
- MSOI002K
YPB|8
- MXBG213A
P|8
- MPDI001B
LMC|8
- MMBC008B

散熱焊盤機械數(shù)據(jù) (封裝 | 引腳)

訂購信息

6.6 Electrical Characteristics: LM358, LM2904

V⁺ = +5.0 V, See⁽²⁾, unless otherwise stated

PARAMETER		TEST CONDITIONS		LM358			LM2904			UNIT
PARAMETER		TEST CONDITIONS		MIN	TYP	MAX	MIN	TYP	MAX	UNIT
Input Offset Voltage		See⁽³⁾ , T_A = 25°C			2	7		2	7	mV
Input Bias Current		I_IN(+) or I_IN(?), T_A = 25°C, V_CM = 0 V, See⁽⁴⁾			45	250		45	250	nA
Input Offset Current		I_IN(+) ? I_IN(?), V_CM = 0 V, T_A = 25°C			5	50		5	50	nA
Input Common-Mode Voltage Range		V⁺ = 30 V, See⁽⁵⁾ (LM2904, V⁺ = 26 V), T_A = 25°C		0		V⁺?1.5	0		V⁺?1.5	V
Supply Current		Over Full Temperature Range
		R_L = ∞ on All Op Amps
		V⁺ = 30 V (LM2904 V⁺ = 26 V)			1	2		1	2	mA
		V⁺ = 5 V			0.5	1.2		0.5	1.2	mA
Large Signal Voltage		V⁺ = 15V, T_A = 25°C,
Gain		R_L ≥ 2 kΩ, (For V_O = 1 V to 11 V)		25	100		25	100		V/mV
Common-Mode Rejection Ratio		T_A = 25°C,		65	85		50	70		dB
Common-Mode Rejection Ratio		V_CM = 0 V to V⁺?1.5 V		65	85		50	70		dB
Power Supply Rejection Ratio		V⁺ = 5 V to 30 V		65	100		50	100		dB
Power Supply Rejection Ratio		(LM2904, V⁺ = 5 V to 26 V), T_A = 25°C		65	100		50	100		dB
Amplifier-to-Amplifier Coupling		f = 1 kHz to 20 kHz, T_A = 25°C (Input Referred), See⁽⁶⁾			?120			?120		dB
Output Current	Source	V_IN⁺ = 1 V,		20	40		20	40		mA
		V_IN^? = 0 V,
		V⁺ = 15 V,
		V_O = 2 V, T_A = 25°C
	Sink	V_IN^? = 1 V, V_IN⁺ = 0 V		10	20		10	20		mA
		V⁺ = 15V, T_A = 25°C,
		V_O = 2 V
		V_IN^? = 1 V,		12	50		12	50		μA
		V_IN⁺ = 0 V
		T_A = 25°C, V_O = 200 mV,
		V⁺ = 15 V
Short Circuit to Ground		T_A = 25°C, See⁽¹⁾, V⁺ = 15 V			40	60		40	60	mA
Input Offset Voltage		See⁽³⁾				9			10	mV
Input Offset Voltage Drift		R_S = 0 Ω			7			7		μV/°C
Input Offset Current		I_IN(+) ? I_IN(?)				150		45	200	nA
Input Offset Current Drift		R_S = 0 Ω			10			10		pA/°C
Input Bias Current		I_IN(+) or I_IN(?)			40	500		40	500	nA
Input Common-Mode Voltage Range		V⁺ = 30 V, See⁽⁵⁾ (LM2904, V⁺ = 26 V)		0		V⁺?2	0		V⁺ ?2	V
Large Signal Voltage Gain		V⁺ = +15 V		15			15			V/mV
		(V_O = 1 V to 11 V)
		R_L ≥ 2 kΩ
Output	V_OH	V⁺ = 30 V	R_L = 2 kΩ	26			22			V
Voltage	V_OH	(LM2904, V⁺ = 26 V)	R_L = 10 kΩ	27	28		23	24		V
Swing	V_OL	V⁺ = 5 V, R_L = 10 kΩ			5	20		5	100	mV
Output Current	Source	V_IN⁺ = 1 V, V_IN^? = 0 V,		10	20		10	20		mA
	Source	V⁺ = 15 V, V_O = 2 V		10	20		10	20		mA
	Sink	V_IN^? = 1 V, V_IN⁺ = 0 V,		5	8		5	8		mA
	Sink	V⁺ = 15 V, V_O = 2 V		5	8		5	8		mA

(1) Short circuits from the output to V⁺ can cause excessive heating and eventual destruction. When considering short circuits to ground, the maximum output current is approximately 40 mA independent of the magnitude of V⁺. At values of supply voltage in excess of +15 V, continuous short-circuits can exceed the power dissipation ratings and cause eventual destruction. Destructive dissipation can result from simultaneous shorts on all amplifiers.

(2) These specifications are limited to –55°C ≤ T_A ≤ +125°C for the LM158/LM158A. With the LM258/LM258A, all temperature specifications are limited to ?25°C ≤ T_A ≤ 85°C, the LM358/LM358A temperature specifications are limited to 0°C ≤ T_A ≤ 70°C, and the LM2904 specifications are limited to –40°C ≤ T_A ≤ 85°C.

(3) V_O ? 1.4 V, R_S = 0 Ω with V⁺ from 5 V to 30 V; and over the full input common-mode range (0 V to V⁺ ?1.5 V) at 25°C. For LM2904, V⁺ from 5 V to 26 V.

(4) The direction of the input current is out of the IC due to the PNP input stage. This current is essentially constant, independent of the state of the output so no loading change exists on the input lines.

(5) The input common-mode voltage of either input signal voltage should not be allowed to go negative by more than 0.3 V (at 25°C). The upper end of the common-mode voltage range is V⁺ ?1.5 V (at 25°C), but either or both inputs can go to 32 V without damage (26 V for LM2904), independent of the magnitude of V⁺.

(6) Due to proximity of external components, insure that coupling is not originating via stray capacitance between these external parts. This typically can be detected as this type of capacitance increases at higher frequencies.