142735
A $U$ tube with both ends open to the atmosphere is partially filled with water. Oil, which is immiscible with water, is poured into one side until it stands at a distance of $10 \mathrm{~mm}$ above the water level on the other side Meanwhile the water rises by $65 \mathrm{~mm}$ from its original level (see diagram). The density of the oil is
142736 Two non-mixing liquids of densities $\rho$ and $n \rho$ $(n>1)$ are put in a container. The height of each liquid is $h$. A solid cylinder of length $L$ and density $d$ is put in this container. The cylinder floats with its axis vertical and length pL $(p \lt 1)$ in the denser liquid. The density $d$ is equal to
142737 The approximate depth of an ocean is $2700 \mathrm{~m}$. The compressibility of water is $45.4 \times 10^{-11} \mathrm{~Pa}^{-\mathrm{i}}$ and density of water is $10^{3} \mathrm{~kg} / \mathrm{m}^{3}$. What fractional compression of water will be obtained at the bottom of the ocean?
142735
A $U$ tube with both ends open to the atmosphere is partially filled with water. Oil, which is immiscible with water, is poured into one side until it stands at a distance of $10 \mathrm{~mm}$ above the water level on the other side Meanwhile the water rises by $65 \mathrm{~mm}$ from its original level (see diagram). The density of the oil is
142736 Two non-mixing liquids of densities $\rho$ and $n \rho$ $(n>1)$ are put in a container. The height of each liquid is $h$. A solid cylinder of length $L$ and density $d$ is put in this container. The cylinder floats with its axis vertical and length pL $(p \lt 1)$ in the denser liquid. The density $d$ is equal to
142737 The approximate depth of an ocean is $2700 \mathrm{~m}$. The compressibility of water is $45.4 \times 10^{-11} \mathrm{~Pa}^{-\mathrm{i}}$ and density of water is $10^{3} \mathrm{~kg} / \mathrm{m}^{3}$. What fractional compression of water will be obtained at the bottom of the ocean?
142735
A $U$ tube with both ends open to the atmosphere is partially filled with water. Oil, which is immiscible with water, is poured into one side until it stands at a distance of $10 \mathrm{~mm}$ above the water level on the other side Meanwhile the water rises by $65 \mathrm{~mm}$ from its original level (see diagram). The density of the oil is
142736 Two non-mixing liquids of densities $\rho$ and $n \rho$ $(n>1)$ are put in a container. The height of each liquid is $h$. A solid cylinder of length $L$ and density $d$ is put in this container. The cylinder floats with its axis vertical and length pL $(p \lt 1)$ in the denser liquid. The density $d$ is equal to
142737 The approximate depth of an ocean is $2700 \mathrm{~m}$. The compressibility of water is $45.4 \times 10^{-11} \mathrm{~Pa}^{-\mathrm{i}}$ and density of water is $10^{3} \mathrm{~kg} / \mathrm{m}^{3}$. What fractional compression of water will be obtained at the bottom of the ocean?
142735
A $U$ tube with both ends open to the atmosphere is partially filled with water. Oil, which is immiscible with water, is poured into one side until it stands at a distance of $10 \mathrm{~mm}$ above the water level on the other side Meanwhile the water rises by $65 \mathrm{~mm}$ from its original level (see diagram). The density of the oil is
142736 Two non-mixing liquids of densities $\rho$ and $n \rho$ $(n>1)$ are put in a container. The height of each liquid is $h$. A solid cylinder of length $L$ and density $d$ is put in this container. The cylinder floats with its axis vertical and length pL $(p \lt 1)$ in the denser liquid. The density $d$ is equal to
142737 The approximate depth of an ocean is $2700 \mathrm{~m}$. The compressibility of water is $45.4 \times 10^{-11} \mathrm{~Pa}^{-\mathrm{i}}$ and density of water is $10^{3} \mathrm{~kg} / \mathrm{m}^{3}$. What fractional compression of water will be obtained at the bottom of the ocean?