For dielectrics in alternating field, polarizability ae is a complex quantity. The imaginary part of ae is zero for-A-ω = 0B-ω → ∞C-ω = 0 and ω → ∞D-ω = natural frequency ω0-C-ω = 0 and ω → ∞

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For dielectrics in alternating field, polarizability ae is a complex quantity. The imaginary part of ae is zero for-A-&omega; = 0B-&omega; &rarr; &infin;C-&omega; = 0 and &omega; &rarr; &infin;D-&omega; = natural frequency &omega;0-C-&omega; = 0 and &omega; &rarr; &infin;

APTITUDE CRACK · Accepted Answer

C &omega; = 0 and &omega; &rarr; &infin; Imaginary part of ae is zero for &omega; = 0 and &omega; = &infin;.

Materials and Components - Engineering

For dielectrics in alternating field, polarizability a_e is a complex quantity. The imaginary part of a_e is zero for

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Materials and Components - Engineering

For dielectrics in alternating field, polarizability ae is a complex quantity. The imaginary part of ae is zero for

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For help Students Orientation Mcqs Questions

For dielectrics in alternating field, polarizability a_e is a complex quantity. The imaginary part of a_e is zero for

For help Students Orientation
Mcqs Questions