A metallic rod of length 1 m us rigidly clamped at its midpoint . Longitudinal stationary waves are set up in the rod in such a way that there are two nodes on either side of the midpoint . the amplitude of an antinode in 2*10^-6 m . write the equation of motion at a point 2 cm from the midpoint and those of constituent waves in the rod.
{ y= 2*10^11 N/m^2 and rough = > 8*10^3 kg/m^3
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Hello pari : - )
As found in case of string , in case of rods also clamped point behaves as a
node while the free end antinode . the situation is shown in figure i have
made for you in paint : -)
Because the distance between two consecutive nodes is ( lambda/2)
while between a node and antinode is lambda/4 hence
4 × { lamda/2} + 2 {lambda/4} = > L or lambda = > 2×1/5 = > 0.4m
further , it is given that
lambda = > 2 ×10^11 N/m² and ρ = > 8 ×10 ³kg/m³
v= > √(λ/ρ) = > √[(2×10^11)/8×10^3] = > 5000 m /s
Hence from ν = > nλ
n = > v/λ = > 5000/0.4 = > 125 Hz
Now if incident and reflected waves along the rod are
y1 = > A sin(ωt -kx) and y2 = > sin(ωt+kx+Φ)
THE RESULTANT WAVE WILL BE
y = > y1 +y2 => Asin (ωt-kx) + sin(ωt+kx+Φ) = > 2A cos ( kx + (Φ/2) )sin (ωt+( Φ/2)
Because there is an antinode at the free end of the rod , hence amplitude is maximum at x = > 0 so
cos ( k ×0 + (Φ/2) ) = > maximum = > 1 i.e Φ = > 0
And ,
A max = > 2A = > 2×10^-6 m ------------------------( given )
y = > 2×10^-6 cos kx sinωt
as we know that y => 2×10^-6 cos 5πx sin 25000πt
Now because for a point 2cm from the midpoint x = > (0.50+,-0.02) ,
and hence we got
y => 2×10^-6 Cos 5π(0.5 +,- 0.02) sin25000(πt) is our required answer
HOPE THIS HELPS YOU !
@ engineer gopal khandelwal
As found in case of string , in case of rods also clamped point behaves as a
node while the free end antinode . the situation is shown in figure i have
made for you in paint : -)
Because the distance between two consecutive nodes is ( lambda/2)
while between a node and antinode is lambda/4 hence
4 × { lamda/2} + 2 {lambda/4} = > L or lambda = > 2×1/5 = > 0.4m
further , it is given that
lambda = > 2 ×10^11 N/m² and ρ = > 8 ×10 ³kg/m³
v= > √(λ/ρ) = > √[(2×10^11)/8×10^3] = > 5000 m /s
Hence from ν = > nλ
n = > v/λ = > 5000/0.4 = > 125 Hz
Now if incident and reflected waves along the rod are
y1 = > A sin(ωt -kx) and y2 = > sin(ωt+kx+Φ)
THE RESULTANT WAVE WILL BE
y = > y1 +y2 => Asin (ωt-kx) + sin(ωt+kx+Φ) = > 2A cos ( kx + (Φ/2) )sin (ωt+( Φ/2)
Because there is an antinode at the free end of the rod , hence amplitude is maximum at x = > 0 so
cos ( k ×0 + (Φ/2) ) = > maximum = > 1 i.e Φ = > 0
And ,
A max = > 2A = > 2×10^-6 m ------------------------( given )
y = > 2×10^-6 cos kx sinωt
as we know that y => 2×10^-6 cos 5πx sin 25000πt
Now because for a point 2cm from the midpoint x = > (0.50+,-0.02) ,
and hence we got
y => 2×10^-6 Cos 5π(0.5 +,- 0.02) sin25000(πt) is our required answer
HOPE THIS HELPS YOU !
@ engineer gopal khandelwal
paridhigupta1234:
thnx a lot : -)
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