The sound in steel covers the distance L (length of the bridge) in a time [tex]t_S[/tex], with a velocity [tex]v_S=5100 m/s[/tex]:
[tex]v_S = \frac{L}{t_S} [/tex]
which we can rewrite as
[tex]L=v_S t_S[/tex] (1)
Similarly, the sound in air covers the length of the bridge L in a time [tex]t_A[/tex], with a velocity [tex]v_A=340 m/s[/tex]:
[tex]v_A = \frac{L}{t_A} [/tex]
which we can rewrite as
[tex]L=v_A t_A[/tex] (2)
We also know that the sound in air arrives with a delay of 1.4 s. This means we can rewrite tA as
[tex]t_A = t_S+1.4 s[/tex] (3)
The length of the bridge is always the same, so we can write (1)=(2) and using the information found in (3):
[tex]v_A (t_S+1.4)=v_S t_S[/tex]
Re-arranging, we find
[tex]t_S = \frac{1.4 v_A }{v_S -v_A}=0.1 s [/tex]
And at this point we can find the length of the bridge:
[tex]L=v_s t_S = (5100 m/s)(0.1 s)=510 m[/tex]