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‑90‑
Structure Drive Model Reactor Model
Inductance (mH) Loss (W)
T12 MD520‑4T315(S)(‑L) MD‑ACL‑660‑0.021‑4T‑2% 0.021 ‑
MD520‑4T355(S)(‑L) MD‑ACL‑800‑0.017‑4T‑2% 0.017 ‑
MD520‑4T400(S)(‑L) MD‑ACL‑800‑0.017‑4T‑2% 0.017 ‑
T13 MD520‑4T500(S)(‑A) GH‑MVT504ZG‑L2 0.022 ‑
MD520‑4T560(S)(‑A) GH‑MVT634ZG‑L3 0.018 ‑
MD520‑4T630(S)(‑A) GH‑MVT634ZG‑L3 0.018 ‑
Note: For T13 models with the model name containing "‑A", the reactor is standard.
Table 5–15 Selection of AC input reactors (three‑phase 200 V to 240 V)
Structure Drive Model Reactor Model
Inductance (mH) Loss (W)
T1 MD520‑2T0.4B(S) MD‑ACL‑10‑5‑4T 5 50
MD520‑2T0.7B(S) MD‑ACL‑10‑5‑4T 5 50
MD520‑2T1.1B(S) MD‑ACL‑10‑5‑4T 5 50
MD520‑2T1.5B(S) MD‑ACL‑10‑5‑4T 5 50
T2 MD520‑2T2.2B(S) MD‑ACL‑15‑3‑4T 3 50
MD520‑2T3.7B(S) MD‑ACL‑15‑3‑4T 3 50
T3 MD520‑2T5.5B(S) MD‑ACL‑40‑1.45‑4T 1.45 100
T4 MD520‑2T7.5B(S) MD‑ACL‑50‑1.2‑4T 1.2 150
T5 MD520‑2T11(B)(S) MD‑ACL‑80‑0.17‑4T‑2% 0.17 ‑
T6 MD520‑2T15(B)(S) MD‑ACL‑80‑0.17‑4T‑2% 0.17 ‑
MD520‑2T18.5(B)(S) MD‑ACL‑90‑0.16‑4T‑2% 0.16 ‑
T7 MD520‑2T22(B)(S) MD‑ACL‑120‑0.12‑4T‑2% 0.12 ‑
MD520‑2T30(B)(S) MD‑ACL‑150‑0.095‑4T‑2% 0.095 ‑
T8 MD520‑2T37(B) (S) MD‑ACL‑200‑0.07‑4T‑2% 0.07 ‑
MD520‑2T45(S) MD‑ACL‑250‑0.056‑4T‑2% 0.056 ‑
MD520‑2T55(S) MD‑ACL‑250‑0.056‑4T‑2% 0.056 ‑
T9 MD520‑2T75(S) MD‑ACL‑330‑0.042‑4T‑2% 0.042 ‑
T10 MD520‑2T90(S) MD‑ACL‑490‑0.028‑4T‑2% 0.028 ‑
MD520‑2T110(S) MD‑ACL‑490‑0.028‑4T‑2% 0.028 ‑
T11 MD520‑2T132(S) MD‑ACL‑660‑0.021‑4T‑2% 0.021 ‑
T12 MD520‑2T160(S) MD‑ACL‑660‑0.021‑4T‑2% 0.021 ‑
MD520‑2T200(S) MD‑ACL‑800‑0.017‑4T‑2% 0.017 ‑
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