Sound waves travel at $350\,\, m/s$ through a warm air and at $3500\,\, m/s$ through brass. The wavelength of a $700\,\, Hz$ acoustic wave as it enters brass from warm air 
AIPMT 2011, Medium
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$\text { Here, } v_{\text {air }}=350 \mathrm{m} / \mathrm{s}, v_{\text {brass }}=3500 \mathrm{m} / \mathrm{s}$

When a sound wave travels from one medium to another medium its frequency remains the same

$\because \quad$ Frequency, $v=\frac{v}{\lambda}$

since $v$ remains the same in both the medium

$\Rightarrow \quad \frac{v_{\text {air }}}{\lambda_{\text {air }}}=\frac{\nu_{\text {brass }}}{\lambda_{\text {brass }}}$

$\lambda_{\text {brass }}=\lambda_{\text {air }} \times \frac{V_{\text {brass }}}{V_{\text {air }}}=\lambda_{\text {air }} \times \frac{3500}{350}=10 \lambda_{\text {air }}$

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