When a transverse wave travels down a real wire there are forces acting on eachportion of the wire in addition to the force resulting from the tension in the wire.An equation that gives an improved description of a wave on a real wire isJ²y T (8²yმყƏt²=дх2ayнwhere T> 0 is the tension, µ> 0 is the mass per unit length and a > 0 is aconstant.(a) Find the relationship between w, T, μ, k, a for y(x, t) = A cos(wt – kx) to be asolution where w> 0 and k> 0 are constants.

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When a transverse wave travels down a real wire there are forces acting on each portion of the wire in addition to the force resulting from the tension in the wire. An equation that gives an improved description of a wave on a real wire is T (8²y н მ2 where T> 0 is the tension, μ> 0 is the mass per unit length and a > 0 is a constant. მოყ Ət² ay (a) Find the relationship between w, T, μ, k, a for y(x, t) = A cos(wt - kx) to be a solution where w> 0 and k ≥0 are constants.

When a transverse wave travels down a real wire there are forces acting on each portion of the wire in addition to the force resulting from the tension in the wire. An equation that gives an improved description of a wave on a real wire is T (8²y н მ2 where T> 0 is the tension, μ> 0 is the mass per unit length and a > 0 is a constant. მოყ Ət² ay (a) Find the relationship between w, T, μ, k, a for y(x, t) = A cos(wt - kx) to be a solution where w> 0 and k ≥0 are constants.