This item is no longer available.
Review Summary
Accidents happen. Protect your favorite Adorama products and purchase a protection plan to stay covered from accidental damage, mechanical or electrical failures, and more.
If we can’t fix it, we’ll replace it at no additional cost.
Protect your product from drops, spills, and more.
Enjoy your gear without fear. We have you covered!
When regular use of your product over time results in mechanical or electrical failure.
We will never charge you a deductible after the purchase of a plan.
Our claims process is simple & easy and our customer service team is happy to help.
Adorama Protect powered by Extend is available for purchase to customers in the United States. Not available for international or U.S. territories purchases. Plans on open box items do not cover pre-existing damage.
Adorama Protect plans are available for ABS clients. If you have any questions or require assistanse, please call 800-223-2500
Browse our FAQ
8 mA
4 mA
90 Ohms
600 Ohms
20 Hz
40 Hz - 20 kHz
14 mV/Pa
A-Weighted: 15 dB-A
CCIR: 24 dB
79 dB-A
132 dB-SPL
Without Connector: 1.81 to 2.28" (46 to 58mm)
0.78" / 20mm
1.52oz / 43g
The Schoeps CCM 41 L Supercardioid Compact Matte Gray Microphone with Lemo Disconnect is strongly directional. Sound arriving from off axis is attenuated even more than with a cardioid. The pickup is "drier" and less susceptible to acoustic feedback than any other SCHOEPS microphone type (a loudspeaker should not be located directly along the rear axis of the microphone, however).
Its directivity is highly independent of frequency, so that even sounds arriving off axis and reverberant sound are registered without coloration. Consequently, even distant placement of the capsule produces a very natural sound pickup. This is a real advantage over interference-tube "shotgun" microphones, whose directivity is very frequency-dependent - exceeding that of a supercardioid only at higher frequencies. Interference-tube microphones are notoriously sensitive to their position in a room, where the shifting patterns of reflections cause corresponding shifts in sound color.